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June, 2011 Page 1Course 601-2-3 (c)2011 Scott Baxter
Course 601
Intro to Wireless BDA, DAS,
and Repeater Technologies
Intro to Wireless BDA, DAS,
and Repeater Technologies
June, 2011 Page 2Course 601-2-3 (c)2011 Scott Baxter
601 Course Outline
Specialized Coverage Expansion Techniques – The Family Tree
Explained
• Repeaters, Boosters, Cell Enhancers: broadband, narrowband,
channelized, high power, frequency translating
• Distributed Antenna Systems
Bi-Directional Amplifiers: The engine inside most systems
• Linearity and Power Output Requirements
• The danger of oscillation/feedback
• output-input coupling and stability considerations
• modern DSP cancellation technologies
Examples of common BDA/DAS Applications and Systems
• Outdoor operator-licensed repeaters
• Indoor One-Operator Systems
• passive re-radiators
• Frequency-specific, stand-alone solutions (one cellular operator,
medical data, etc.)
• Neutral Host (Multi Frequency, Multi-Cellular Operator, Local
Wireless Systems)
June, 2011 Page 3Course 601-2-3 (c)2011 Scott Baxter
Specialized Coverage Expansion
Techniques – The Family Tree
Specialized Coverage Expansion
Techniques – The Family Tree
The Family Tree of Special RF Distribution
Re-radiators (boosters, cell enhancers, repeaters)
• Passive
– Coax-fed
• Active (bi-directional amplifiers, on-frequency)
– Coax-fed
– Fiber-fed
• Active, Frequency-Converting
Distributed Antenna Systems
• Passive
– Coax-fed
– Fiber-fed
• Active
– Cable fed
– Fiber fed with active remote nodes
• Single User
• Community/Co-operative
These are just the major branches of the tree – there are many variations
June, 2011 Page 4Course 601-2-3 (c)2011 Scott Baxter
Cell RR
Wireless Reradiators
Reradiators (also called “boosters”,
“repeaters”, “cell enhancers”) are amplifying
devices intended to add coverage to a cell site
Reradiators are transparent to the host
Wireless system
• A reradiator amplifies RF signals in both
directions, uplink and downlink
• The system does not control reradiators and
has no knowledge of anything they do to the
signals they amplify, on either uplink or
downlink
Careful attention is required when using
reradiators to solve coverage problems
• to achieve the desired coverage
improvement
• to avoid creating interference
• to ensure the active search window is large
enough to accommodate both donor signal
and reradiator signal as seen by mobiles
Reradiators are a
‘“crutch” with
definite application
restrictions. Many
operators prefer not
to use re-radiators at
all. However,
reradiators are a
cost-effective
solution for some
problems.
June, 2011 Page 5Course 601-2-3 (c)2011 Scott Baxter
Home or Small Office Reradiator Setup
Opposing Requirements:
• Reradiator must have
enough gain to deliver
coverage to its whole
intended coverage area
• But the reradiator
transmits on the same
frequency it is receiving
• To prevent oscillation, the
gain of the reradiator must
be at least 10 db less than
the isolation (loss)
between its serving and
donor antennas
Isolation
June, 2011 Page 6Course 601-2-3 (c)2011 Scott Baxter
Wilson Electronics Signal Booster
Wilson Electronics is probably
the best-known consumer-level
provider of bidirectional
amplifiers for deployment by
end-users.
Wilson’s early models often
oscillated and caused serious
interference to wireless systems.
• Customers often mounted
the antennas close together,
producing very low isolation
• Wilson’s current products are
better protected against
oscillation, but non-technical
end-users still make bad
installation choices
June, 2011 Page 7Course 601-2-3 (c)2011 Scott Baxter
What is a DAS?
A Distributed Antenna System, or DAS, is a network of spatially
separated antenna nodes connected to a common source via a
transport medium that provides wireless service within a
geographic area or structure.
1. Building-wide wireless services
(cellular/PCS, 2-way radio, paging) connect
to integrated access device (IAD) through
either base stations or off-air repeaters
2. IAD combines radio signals for
applications and services, filters them and
sends them into a single wired backbone
or trunk running up the building riser
3. The trunk (typ. 7/8”) distributes service to
every floor of building
4. WLAN, building automation, security, etc.
are added on floor-by-floor basis via
applications portals. Access points are in
locked closets on each floor
5. Antenna components, radiating cable,
standard cables, and omni and directional
antennas branch off the trunk on each
floor.
June, 2011 Page 8Course 601-2-3 (c)2011 Scott Baxter
Types of Distributed Antenna Systems
There are several kinds of Distributed Antenna Systems, each with
their own characteristics :
Passive DAS – where RF signals are combined using passive
components such as filters, splitters and couplers. Great for
multiple bands and small to medium size locations
• no power consumed, just off-air pickup and redistribution
Active DAS – RF signals are converted and distributed over fiber.
Easy to serve larger installations but more costly since each band
and operator must be filtered/amplified/processed individually.
Hybrid DAS – combination of active and passive techniques
DAS can be employed purely within a large building (In-building
DAS) or across a large urban area (Street Level DAS). Street
Level DAS can provide a very efficient solution for large urban
regeneration projects which require dense coverage. They can
also be provided in other busy areas such as Metros, Airports or
Railway Stations
June, 2011 Page 9Course 601-2-3 (c)2011 Scott Baxter
A Cable-Distributed DAS
June, 2011 Page 10Course 601-2-3 (c)2011 Scott Baxter
Fiber-distributed DAS: Lake Nona, FL
Block flow diagram of an actual Neutral-Host DAS serving three
wireless operators as well as public-safety systems
June, 2011 Page 11Course 601-2-3 (c)2011 Scott Baxter
Detailed Functions: Lake Nona, FL
Device functional diagram showing hardware detail for Lake Nona
DAS
June, 2011 Page 12Course 601-2-3 (c)2011 Scott Baxter
Equipment List for Lake Nona DAS
This list includes the major
active RF devices in the
Lake Nona DAS, broken out
by project
June, 2011 Page 13Course 601-2-3 (c)2011 Scott Baxter
Elements of an In-Building DAS Installation
June, 2011 Page 14Course 601-2-3 (c)2011 Scott Baxter
Elements of an Outdoor DAS Installation
June, 2011 Page 15Course 601-2-3 (c)2011 Scott Baxter
Typical Equipment of Neutral-Host DAS
With Operator’s BTSs On-Site
June, 2011 Page 16Course 601-2-3 (c)2011 Scott Baxter
Passive DAS System
June, 2011 Page 17Course 601-2-3 (c)2011 Scott Baxter
Off-Air vs. Direct Feed
A DAS which connects with outside radio systems through antennas over
the air is said to be in the “Off Air” mode
A DAS which has actual base stations of outside radio systems located in
its equipment rooms, and connects directly to them, is said to operate by
“Direct Feed”
Off-air operation is certainly less expensive, but the reliability and quality
of the connection is affected by possible changes in propagation and
interference.
• Since an off-air DAS merely uses existing capacity from the wireless
networks it carries, this places a practical limit on the amount of total
traffic the DAS is able to handle
Direct Feed brings more complicated and expensive Base Stations onto
the DAS headend premises, but the DAS operator is usually not
responsible for their cost. The connection is more reliable and the entire
capacity of the base stations is available for use on the DAS system.
• Most large DAS systems use Direct Feed mainly because of traffic
considerations.
June, 2011 Page 18Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 19Course 601-2-3 (c)2011 Scott Baxter
Bi-Directional Amplifiers: The
engine inside most systems
Bi-Directional Amplifiers: The
engine inside most systems
Bi-Directional Amplifiers
Depending upon the size of the desired coverage and the
expected traffic levels, most repeaters and DAS systems use
some form of Bi-Directional Amplifiers (BDAs) to boost the signal
level in both directions
• If the external signals are picked up using antennas aimed at
external cellsites, then the system is called “off-air”
• If base stations of the external operators are actually placed at
the DAS head end and connected directly to DAS equipment,
we say the system is “direct feed”.
June, 2011 Page 20Course 601-2-3 (c)2011 Scott Baxter
Linearity and Power Output Requirements
Power output of system amplifiers is determined by the needed
coverage and the gains and losses of other system components
• A formal link budget is used for design of the system
Amplifier linearity is expressed by the following specifications
• Third-order intercept
• Noise floor
• Levels of Intermodulation products
June, 2011 Page 21Course 601-2-3 (c)2011 Scott Baxter
Avoiding Oscillation and Feedback
What is BDA oscillation?
Oscillation is when the outside antenna hears the amplified signal from the
indoor antenna or the indoor antenna hears the amplified signal from the
outside antenna. This event is similar to microphone/speaker feedback in
audio.
Prior to about 2000, bidirectional amplifiers used automatic sensing to
gauge the level of isolation between their input and output signal lines
• The amplifiers would automatically reduce their gain to keep it below
the point of oscillation
Beginning around 2000, several manufacturers began using DSP
technology to do RF sensing and automatically inject oppositely-phased
RF energy into their input circuitry
• This technique can provide roughly an additional 30 db of cancellation
• For example, a reradiator with 100 db isolation between its antennas
would have been able to use only about 90 db of gain
• With the DSP cancellation, at the same 100 db isolation the advanced
amplifier is able to operate stably with about 120 db gain
June, 2011 Page 22Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 23Course 601-2-3 (c)2011 Scott Baxter
Course 602
Wireless BDA/DAS
Application and Design
Wireless BDA/DAS
Application and Design
June, 2011 Page 24Course 601-2-3 (c)2011 Scott Baxter
602 Course Outline
Classes of BDA/DAS Devices and Systems
Wireless Services and Frequencies
Wireless Technologies: Signal Types carried by BDA/DAS
Systems
Quality Criteria For BDA/DAS Systems
Basic BDA/DAS Coverage Requirements
In-Building Propagation
RF Propagation in BDA/DAS Systems
Antennas for BDA/DAS Systems
BDA/DAS System Link Budgets
System design to satisfy link budget requirements
BDA/DAS Equipment Manufacturers and Product Offerings
BDA/DAS Installation Techniques and Practices
BDA/DAS Example Case Studies
June, 2011 Page 25Course 601-2-3 (c)2011 Scott Baxter
Classes of BDA/DAS Devices and
Systems
Classes of BDA/DAS Devices and
Systems
Experimental 40 km Fiber DAS
June, 2011 Page 26Course 601-2-3 (c)2011 Scott Baxter
A Unique Kind of DAS Cable Distribution:
Using HVAC metal Ducting as Waveguide!
Wireless RF Distribution in Buildings
using Heating and Ventilation Ducts
• http://citeseerx.ist.psu.edu/viewdoc
/download?doi=10.1.1.81.368&rep
=rep1&type=pdf
June, 2011 Page 27Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 28Course 601-2-3 (c)2011 Scott Baxter
Wireless Services and
Frequencies
Wireless Services and
Frequencies
June, 2011 Page 29Course 601-2-3 (c)2011 Scott Baxter
Frequencies Used by Wireless Systems
Overview of the Radio Spectrum
3 4 5 6 7 8 9 10 12 14 16 18 20 22 24 26 28 30 GHz
30,000,000,000 i.e., 3x1010 Hz
Broadcasting Land-Mobile Aeronautical Mobile Telephony
Terrestrial Microwave Satellite
0.3 0.4 0.5 0/6 0.7 0.8 0.9 1.0 1.2 1.4 1.6 1.8 2.0 2.4 3.0 GHz
3,000,000,000 i.e., 3x109 Hz
UHF TV 14-59UHF GPS
DCS, PCS, AWS700 + Cellular
0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.2 1.4 1.6 1.8 2.0 2.4 3.0 MHz
3,000,000 i.e., 3x106 Hz
AM LORAN Marine
3 4 5 6 7 8 9 10 12 14 16 18 20 22 24 26 28 30 MHz
30,000,000 i.e., 3x107 Hz
Short Wave -- International Broadcast -- Amateur CB
30 40 50 60 70 80 90 100 120 140 160 180 200 240 300 MHz
300,000,000 i.e., 3x108 Hz
FM VHF TV 7-13VHF LOW Band VHFVHF TV 2-6
June, 2011 Page 30Course 601-2-3 (c)2011 Scott Baxter
Current Wireless Spectrum in the US
Modern wireless began in the 800 MHz. range, when the US FCC
reallocated UHF TV channels 70-83 for wireless use and AT&T’s Analog
technology “AMPS” was chosen.
Nextel bought many existing 800 MHz. Enhanced Specialized Mobile
Radio (ESMR) systems and converted to Motorola’s “IDEN” technology
The FCC allocated 1900 MHz. spectrum for Personal Communications
Services, “PCS”, auctioning the frequencies for over $20 billion dollars
With the end of Analog TV broadcasting in 2009, the FCC auctioned
former TV channels 52-69 for wireless use, “700 MHz.”
The FCC also auctioned spectrum near 1700 and 2100 MHz. for
Advanced Wireless Services, “AWS”.
Technically speaking, any technology can operate in any band. The
choice of technology is largely a business decision.
700 MHz 800 900 1700 1800 1900 2000 2100 2200
700 MHz. IDEN
IDEN
CELLDNLNK
CELLUPLINK
AWS
Uplink
AWS
Down-
Link
PCS
Uplink
PCS
Down-
Link
Proposed AWS-2
AWS?
SAT
SAT
Frequency, MegaHertz
June, 2011 Page 31Course 601-2-3 (c)2011 Scott Baxter
North American Cellular Spectrum
In each MSA and RSA, eligibility for ownership was restricted
• “A” licenses awarded to non-telephone-company applicants only
• “B” licenses awarded to existing telephone companies only
• subsequent sales are unrestricted after system in actual operation
Downlink Frequencies
(“Forward Path”)
Uplink Frequencies
(“Reverse Path”)
Frequency, MHz824 835 845 870 880 894
869
849
846.5825
890
891.5
Paging, ESMR, etc. A B
Ownership and
Licensing
Frequencies used by “A” Cellular Operator
Initial ownership by Non-Wireline companies
Frequencies used by “B” Cellular Operator
Initial ownership by Wireline companies
June, 2011 Page 32Course 601-2-3 (c)2011 Scott Baxter
By 1994, US cellular systems were seriously
overloaded and looking for capacity relief
• The FCC allocated 120 MHz. of spectrum
around 1900 MHz. for new wireless telephony
known as PCS (Personal Communications
Systems), and 20 MHz. for unlicensed services
• allocation was divided into 6 blocks; 10-year
licenses were auctioned to highest bidders
Development of North America PCS
51 MTAs
493 BTAs
PCS Licensing and Auction Details
• A & B spectrum blocks licensed in 51 MTAs (Major Trading Areas )
• Revenue from auction: $7.2 billion (1995)
• C, D, E, F blocks were licensed in 493 BTAs (Basic Trading Areas)
• C-block auction revenue: $10.2 B, D-E-F block auction: $2+ B (1996)
• Auction winners are free to choose any desired technology
A D B E F C
unlic.
data
unlic.
voice A D B E F C
1850
MHz.
1910
MHz.
1990
MHz.
1930
MHz.
15 15 155 5 5 15 15 155 5 5
PCS SPECTRUM ALLOCATIONS IN NORTH AMERICA
June, 2011 Page 33Course 601-2-3 (c)2011 Scott Baxter
The US 700 MHz. Spectrum and Its Blocks
To satisfy growing demand for wireless data services as well as
traditional voice, the FCC has also taken the spectrum formerly used as
TV channels 52-69 and allocated them for wireless
The TV broadcasters will completely vacate these frequencies when
analog television broadcasting ends in February, 2009
At that time, the winning wireless bidders may begin building and
operating their networks
In many cases, 700 MHz. spectrum will be used as an extension of
existing operators networks. In other cases, entirely new service will be
provided.
June, 2011 Page 34Course 601-2-3 (c)2011 Scott Baxter
Advanced Wireless Services: The AWS Spectrum
To further satisfy growing demand for wireless data services as well
as traditional voice, the FCC has also allocated more spectrum for
wireless in the 1700 and 2100 MHz. ranges
The US AWS spectrum lines up with International wireless
spectrum allocations, making “world” wireless handsets more
practical than in the past
Many AWS licensees will simply use their AWS spectrum to add
more capacity to their existing networks; some will use it to
introduce their service to new areas
June, 2011 Page 35Course 601-2-3 (c)2011 Scott Baxter
AWS Spectrum Blocks
The AWS spectrum is divided into “blocks”
Different wireless operator companies are licensed to use specific
blocks in specific areas
This is the same arrangement used in original 800 MHz. cellular,
1900 MHz. PCS, and the new 700 MHz. allocations
June, 2011 Page 36Course 601-2-3 (c)2011 Scott Baxter
Wireless Technologies: Signal
Types carried by BDA/DAS
Wireless Technologies: Signal
Types carried by BDA/DAS
Characteristics of a Radio Signal
The purpose of telecommunications is to
send information from one place to another
Our civilization exploits the transmissible
nature of radio signals, using them in a
sense as our “carrier pigeons”
To convey information, some characteristic
of the radio signal must be altered (I.e.,
‘modulated’) to represent the information
The sender and receiver must have a
consistent understanding of what the
variations mean to each other
RF signal characteristics which can be
varied for information transmission:
• Amplitude
• Frequency
• Phase
SIGNAL CHARACTERISTICS
S(t) = A cos [ ωc t + ϕ ]
The complete, time-
varying radio signal
Amplitude (strength)
of the signal
Natural Frequency
of the signal
Phase of the signal
Compare these Signals:
Different
Amplitudes
Different
Frequencies
Different
Phases
June, 2011 Page 37Course 601-2-3 (c)2011 Scott Baxter
Modulation and Occupied Bandwidth
The bandwidth occupied by a signal
depends on:
• input information bandwidth
• modulation method
Information to be transmitted, called
“input” or “baseband”
• bandwidth usually is small, much
lower than frequency of carrier
Unmodulated carrier
• the carrier itself has Zero bandwidth!!
AM-modulated carrier
• Notice the upper & lower sidebands
• total bandwidth = 2 x baseband
FM-modulated carrier
• Many sidebands! bandwidth is a
complex mathematical function
PM-modulated carrier
• Many sidebands! bandwidth is a
complex mathematical function
Voltage
Time
Time-Domain
(as viewed on an
Oscilloscope)
Frequency-Domain
(as viewed on a
Spectrum Analyzer)
Voltage
Frequency0
fc
fc
Upper
Sideband
Lower
Sideband
fc
fc
June, 2011 Page 38Course 601-2-3 (c)2011 Scott Baxter
The Emergence of AM: A bit of History
The early radio pioneers first used binary transmission, turning their
crude transmitters on and off to form the dots and dashes of Morse
code. The first successful demonstrations of radio occurred during
the mid-1890’s by experimenters in Italy, England, Kentucky, and
elsewhere.
Amplitude modulation was the first method used to transmit voice
over radio. The early experimenters couldn’t foresee other methods
(FM, etc.), or today’s advanced digital devices and techniques.
Commercial AM broadcasting to the public began in the early
1920’s.
Despite its disadvantages and antiquity, AM is still alive:
• AM broadcasting continues today in 540-1600 KHz.
• AM modulation remains the international civil aviation standard,
used by all commercial aircraft (108-132 MHz. band).
• AM modulation is used for the visual portion of commercial
television signals (sound portion carried by FM modulation)
• Citizens Band (“CB”) radios use AM modulation
• Special variations of AM featuring single or independent
sidebands, with carrier suppressed or attenuated, are used for
marine, commercial, military, and amateur communicationsSSBLSB USB
June, 2011 Page 39Course 601-2-3 (c)2011 Scott Baxter
Frequency Modulation (“FM”)
Frequency Modulation (FM) is a type of
angle modulation
• in FM, the instantaneous frequency
of the signal is varied by the
modulating waveform
Advantages of FM
• the amplitude is constant
– simple saturated amplifiers can
be used
– the signal is relatively immune
to external noise
– the signal is relatively robust;
required C/I values are typically
17-18 dB. in wireless
applications
Disadvantages of FM
• relatively complex detectors are
required
• a large number of sidebands are
produced, requiring even larger
bandwidth than AM
TIME-DOMAIN VIEW
sFM(t) =A cos [ωc t + mω m(x)dx+ϕ0 ]
t
t0
where:
A = signal amplitude (constant)
ωc = radian carrier frequency
mω = frequency deviation index
m(x) = modulating signal
ϕ0 = initial phase
FREQUENCY-DOMAIN VIEW
Voltage
Frequency0 fc
SFM(t)
UPPER
SIDEBANDS
LOWER
SIDEBANDS
June, 2011 Page 40Course 601-2-3 (c)2011 Scott Baxter
The Digital Advantage
The modulating signals shown in previous
slides were all analog. It is also possible to
quantize modulating signals, restricting them
to discrete values, and use such signals to
perform digital modulation. Digital
modulation has several advantages over
analog modulation:
Digital signals can be more easily
regenerated than analog
• in analog systems, the effects of noise
and distortion are cumulative: each
demodulation and remodulation
introduces new noise and distortion,
added to the noise and distortion from
previous demodulations/remodulations.
• in digital systems, each demodulation
and remodulation produces a clean
output signal free of past noise and
distortion
Digital bit streams are ideally suited to many
flexible multiplexing schemes
transmission
demodulation-remodulation
transmission
demodulation-remodulation
transmission
demodulation-remodulation
June, 2011 Page 41Course 601-2-3 (c)2011 Scott Baxter
Theory of Digital Modulation: Sampling
Voice and other analog signals first must
be sampled (converted to digital form) for
digital modulation and transmission
The sampling theorem gives the criteria
necessary for successful sampling,
digital modulation, and demodulation
• The analog signal must be band-
limited (low-pass filtered) to contain
no frequencies higher than fM
• Sampling must occur at least twice
as fast as fM in the analog signal.
This is called the Nyquist Rate
Required Bandwidth for p(t)
• If each sample p(t) is expressed as
an n-bit binary number, the
bandwidth required to convey p(t) as
a digital signal is at least N*2* fM
• this follows Shannon’s Theorem: at
least one Hertz of bandwidth is
required to convey one bit per
second of data
The Sampling Theorem: Two Parts
•If the signal contains no frequency higher
than fM Hz., it is comletely described by
specifying its samples taken at instants of
time spaced 1/2 fM s.
•The signal can be completely recovered
from its samples taken at the rate of 2 fM
samples per second or higher.
m(t)
Sampling
Recovery
m(t)
p(t)
June, 2011 Page 42Course 601-2-3 (c)2011 Scott Baxter
Sampling Example: the 64 kb/s DS-0
Telephony has adopted a world-wide PCM
standard digital signal employing a 64 kb/s
stream derived from sampled voice data
Voice waveforms are band-limited
• upper cutoff between 3500-4000 Hz. to
avoid aliasing
• rolloff below 300 Hz. to minimize
vulnerability to “hum” from AC power mains
Voice waveforms sampled at 8000/second rate
• 8000 samples x 1 byte = 64,000 bits/second
• A>D conversion is non-linear, one byte per
sample, thus 256 quantized levels are
possible
• Levels are defined logarithmically rather
than linearly to accommodate a wider range
of audio levels with minimum distortion
– µ-law companding (popular in North
America & Japan)
– A-law companding (used in most other
countries)
A>D and D>A functions are performed in a
CODEC (coder-decoder) (see following figure)
-10dB
-20dB
-30dB
-40dB
0 dB
100 300 1000 3000 10000
Frequency, Hz
C-Message Weighting
t
0
1
2
3
4
5
6
87
910
11
12
13
14
15
16
4
16
1
3
15
8
3
4
8
A-LAW
y= sgn(x)
A|x|
ln(1+ A)
for 0≤ x≤
1
A
(where A = 87.6)
y= sgn(x)
ln(1+ A|x)|
ln(1+ A)
for
1
A
< x ≤1
µ-Law
y = sgn(x)
ln(1+ µ|x|)
ln(1 + µ)
(whereµ = 255)
Companding
Band-Limiting
x = analog audio voltage
y = quantized level (digital)
June, 2011 Page 43Course 601-2-3 (c)2011 Scott Baxter
Digital ModulationDigital Modulation
June, 2011 Page 44Course 601-2-3 (c)2011 Scott Baxter
Modulation by Digital Inputs
For example, modulate a signal with this
digital waveform. No more continuous
analog variations, now we’re “shifting”
between discrete levels. We call this “shift
keying”.
• The user gets to decide what levels
mean “0” and “1” -- there are no
inherent values
Steady Carrier without modulation
Amplitude Shift Keying
ASK applications: digital microwave
Frequency Shift Keying
FSK applications: control messages in
AMPS cellular; TDMA cellular
Phase Shift Keying
PSK applications: TDMA cellular,
GSM & PCS-1900
Our previous modulation examples used continuously-variable
analog inputs. If we quantize the inputs, restricting them to
digital values, we will produce digital modulation.
Voltage
Time
1 0 1 0
1 0 1 0
1 0 1 0
1 0 1 0
June, 2011 Page 45Course 601-2-3 (c)2011 Scott Baxter
Claude Shannon:
The “Einstein” of Information Theory and Signal Science
The core idea that makes CDMA
possible was first explained by
Claude Shannon, a Bell Labs
research mathematician
Shannon's work relates amount
of information carried, channel
bandwidth, signal-to-noise-ratio,
and detection error probability
• It shows the theoretical
upper limit attainable
In 1948 Claude Shannon published his landmark paper on information theory,
A Mathematical Theory of Communication. He observed that "the
fundamental problem of communication is that of reproducing at one point
either exactly or approximately a message selected at another point." His
paper so clearly established the foundations of information theory that his
framework and terminology are standard today.
Shannon died Feb. 24, 2001, at age 84.
June, 2011 Page 46Course 601-2-3 (c)2011 Scott Baxter
Modulation Techniques of 1xEV Technologies
1xEV, “1x Evolution”, is a family of alternative
fast-data schemes that can be implemented on a
1x CDMA carrier.
1xEV DO means “1x Evolution, Data Only”,
originally proposed by Qualcomm as “High Data
Rates” (HDR).
• Up to 2.4576 Mbps forward, 153.6 kbps
reverse
• A 1xEV DO carrier holds only packet data,
and does not support circuit-switched voice
• Commercially available in 2003
1xEV DV means “1x Evolution, Data and Voice”.
• Max throughput of 5 Mbps forward, 307.2k
reverse
• Backward compatible with IS-95/1xRTT
voice calls on the same carrier as the data
• Not yet commercially available; work
continues
All versions of 1xEV use advanced modulation
techniques to achieve high throughputs.
QPSK
CDMA IS-95,
IS-2000 1xRTT,
and lower rates
of 1xEV-DO, DV
16QAM
1xEV-DO
at highest
rates
64QAM
1xEV-DV
at highest
rates
June, 2011 Page 47Course 601-2-3 (c)2011 Scott Baxter
Digital Modulation Systems
Each symbol of a digitally
modulated RF signal conveys
a number of bits of information
• determined by the number
of degrees of modulation
freedom
More complex modulation
schemes can carry more bits
per symbol in a given
bandwidth, but require better
signal-to-noise ratios
The actual number of bits per
second which can be
conveyed in a given bandwidth
under given signal-to-noise
conditions is described by
Shannon’s equations
Modulation
Scheme
Shannon Limit,
BitsHz
BPSK 1 b/s/hz
QPSK 2 b/s/hz
8PSK 3 b/s/hz
16 QAM 4 b/s/hz
32 QAM 5 b/s/hz
64 QAM 6 b/s/hz
256 QAM 8 b/s/hz
SHANNON’S
CAPACITY EQUATION
C = Bω log2 [ 1 + ]S
N
Bω = bandwidth in Hertz
C = channel capacity in bits/second
S = signal power
N = noise power
June, 2011 Page 48Course 601-2-3 (c)2011 Scott Baxter
Digital Modulation Schemes
There are many different schemes for digital modulation, each a
compromise between complexity, immunity to errors in transmission,
required channel bandwidth, and possible requirement for linear amplifiers
Linear Modulation Techniques
• BPSK Binary Phase Shift Keying
• DPSK Differential Phase Shift Keying
• QPSK Quadrature Phase Shift Keying IS-95 CDMA forward link
– Offset QPSK IS-95 CDMA reverse link
– Pi/4 DQPSK IS-54, IS-136 control and traffic channels
Constant Envelope Modulation Schemes
• BFSK Binary Frequency Shift Keying AMPS control channels
• MSK Minimum Shift Keying
• GMSK Gaussian Minimum Shift Keying GSM systems, CDPD
Hybrid Combinations of Linear and Constant Envelope Modulation
• MPSK M-ary Phase Shift Keying
• QAM M-ary Quadrature Amplitude Modulation
• MFSK M-ary Frequency Shift Keying FLEX paging protocol
Spread Spectrum Multiple Access Techniques
• DSSS Direct-Sequence Spread Spectrum IS-95 CDMA
• FHSS Frequency-Hopping Spread Spectrum
June, 2011 Page 49Course 601-2-3 (c)2011 Scott Baxter
Error Vulnerabilities of
Higher-Order Modulation Schemes
Higher-Order Modulation
Schemes (16PSK, 32QAM,
64QAM...) are more
vulnerable to transmission
errors than the simpler, more
rugged schemes (BPSK,
QPSK)
• Closely-packed
constellations leave little
room for vector error
Non-linearities (gain
compression, clipping,
reflections within antenna
system) “warp” the
constellation
Noise and long-delayed
echoes cause “scatter”
around constellation points
Interference blurs
constellation points into
“rings” of error
Q
I
Normal 64QAM
Q
I
Distortion
(Gain Compression)
Q
I
Noise Q
I
Interference
June, 2011 Page 50Course 601-2-3 (c)2011 Scott Baxter
Error Vector Magnitude and ρ (“Rho”)
A common measurement of
overall error is Error Vector
Magnitude “EVM”
• usually a small fraction of
total vector amplitude, ~0.1
EVM is usually averaged over
a large number of symbols
• Root-mean-square (RMS)
Commercial test equipment
for BTS maintenance
measures EVM
Signal quality is often
expressed as 1-EVM
• normally called ρ (“Rho”)
• typically 0.89-0.96
June, 2011 Page 51Course 601-2-3 (c)2011 Scott Baxter
Modulation used in IS-95 CDMA Systems
CDMA mobiles use offset
QPSK modulation
• the Q-sequence is
delayed half a chip, so
that I and Q never
change simultaneously
and the mobile TX never
passes through (0,0)
CDMA base stations use
QPSK modulation
• every signal (voice, pilot,
sync, paging) has its own
amplitude, so the
transmitter is unavoidably
going through (0,0)
sometimes; no reason to
include 1/2 chip delay
Base Stations: QPSK
Q Axis
I Axis
Short
PN Q
Σ
cos ωt
sin ωt
User’s
chips
Short
PN I
Mobiles: OQPSK
Q Axis
I Axis
Short
PN Q
Σ
cos ωt
sin ωt
User’s
chips
1/2
chip
Short
PN I
June, 2011 Page 52Course 601-2-3 (c)2011 Scott Baxter
CDMA Base Station Modulation Views
The view at top right shows the
actual measured QPSK phase
constellation of a CDMA base
station in normal service
The view at bottom right shows
the measured power in the code
domain for each walsh code on a
CDMA BTS in actual service
• Notice that not all walsh codes
are active
• Pilot, Sync, Paging, and
certain traffic channels are in
use
June, 2011 Page 53Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 54Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 55Course 601-2-3 (c)2011 Scott Baxter
Multiple Access Methods
Frequency
Time
Power
TDMA
Frequency
Time
Power
FDMA
Frequency
Time
Power
CDMA
CODE
FDMA: AMPS & NAMPS
•Each user occupies a private Frequency,
protected from interference through physical
separation from other users on the same
frequency
TDMA: IS-136, GSM
•Each user occupies a specific frequency but
only during an assigned time slot. The
frequency is used by other users during
other time slots.
CDMA
•Each user uses a signal on a particular
frequency at the same time as many other
users, but it can be separated out when
receiving because it contains a special code
of its own
June, 2011 Page 56Course 601-2-3 (c)2011 Scott Baxter
Multiple Access Methods
MIMO
OFDM OFDM, OFDMA
•Orthogonal Frequency Division Multiplexing;
Orthogonal Frequency Division Muliple Access
•The signal consists of many (from dozens to
thousands) of thin carriers carrying symbols
•In OFDMA, the symbols are for multiple users
•OFDM provides dense spectral efficiency and
robust resistance to fading, with great flexibility
of use
MIMO
•Multiple Input Multiple Output
•An ideal companion to OFDM, MIMO allows
exploitation of multiple antennas at the base
station and the mobile to effectively multiply
the throughput for the base station and users
Frequency
Tim
e
Power
June, 2011 Page 57Course 601-2-3 (c)2011 Scott Baxter
Quality Criteria For BDA/DAS
Systems
Quality Criteria For BDA/DAS
Systems
Signal Quality Criteria
C/I Carrier-to-Interference
• Ratio of power of desired signal to power of undesired signals in the
background
S/N Signal-to-Noise Ratio
• Ratio of power of desired signal to the noise in the background
Linearity
• Purity of the signal. Typically expressed as Rho or Error Vector
Magnitude.
• Typical specification: Rho >= 0.9, or EVM <0.1
Amplitude “tilt” over frequency
• Variable frequency response causing some parts of the signal to be
amplified more than others, distorting the waveform
Intersymbol Interference (ISI)
• The process of a 1 or 0 in the signal getting overlapped with adjoining
1’s or 0’s, potentially causing incorrect decoding
• ISI can be caused by distortion in equipment and by external
interference
June, 2011 Page 58Course 601-2-3 (c)2011 Scott Baxter
Phase Constellation ‘Argand’ Diagram
If a transmitter were
perfect, it would transmit
exactly the proper
strength and phase and
the diagram at right
would have only clean
little dots.
Real transmitters have
variable phase and
amplitude errors and
instead of precise dots,
the diagram at right looks
like a paintball target.
If the error is large
enough, the dots will
splatter enough to cause
mistakes in the decoding
process.
June, 2011 Page 59Course 601-2-3 (c)2011 Scott Baxter
Spectrum Display showing Noise Floor
On this spectrum
analyzer, the noise
floor is below the
specified maximum.
If the amplifier were
nonlinear, or there
were corroded
connections involved,
locally-generated
noise would drive the
noise floor up above
spec and potentially
interfere with other
communications.
June, 2011 Page 60Course 601-2-3 (c)2011 Scott Baxter
Working in DecibelsWorking in Decibels
June, 2011 Page 61Course 601-2-3 (c)2011 Scott Baxter
Decibels (DB)
Calculations of transmitted and received power on radio links and
many other electronic circuits always encounters very large and very
small numbers
• Multiplying and dividing these numbers is tedious
Fortunately, there is a simpler way to perform the needed
calculations: a logarithmic system which expresses the powers,
gains and losses of the circuits in units called decibels (db)
Decibels offer two big advantages over straight arithmetic:
• in decibels, the numbers are never very large or small
• working in arithmetic, power calculations always involve
multiplying. Working in decibels, only addition or subtraction are
needed.
Working in decibels
• can be performed using a calculator, or
• by remembering two or three key values in a table and knowing
how to apply them
June, 2011 Page 62Course 601-2-3 (c)2011 Scott Baxter
Using Decibels
In manual calculation of RF power
levels, unwieldy large and small
numbers occur as a product of
painful multiplication and division.
It is popular and much easier to work
in Decibels (dB).
• rather than multiply and divide
RF power ratios, in dB we can
just add & subtract
Decibel Examples
Number N dB
1,000,000,000 +90
100,000,000 +80
10,000,000 +70
1,000,000 +60
100,000 +50
10,000 +40
1,000 +30
100 +20
10 +10
4 +6
2 +3
1 0
0.5 -3
0.25 -6
0.1 -10
0.01 -20
0.001 -30
0.0001 -40
0.00001 -50
0.000001 -60
0.0000001 -70
0.00000001 -80
0.000000001 -90
db = 10 * Log ( X )
Ratio to Decibels
X = 10 (db/10)
Decibels to Ratio
June, 2011 Page 63Course 601-2-3 (c)2011 Scott Baxter
Example Link Budget, NOT Using DB
Let’s track the power flow
from transmitter to receiver in
a radio link. We’re going to
use typical values that
commonly occur in real links.
Receiver
Antenna
Antenna
Trans.
Line
Transmitter
Trans.
Line
20 Watts TX output
x 0.50 line efficiency
= 10 watts to antenna
x 20 antenna gain
= 200 watts ERP
x 0.000,000,000,000,000,1585 path attenuation
= 0.000,000,000,000,031,7 watts if intercepted by dipole antenna
x 20 antenna gain
= 0.000,000,000,000,634 watts into line
x 0.50 line efficiency
= 0.000,000,000,000,317 watts to receiver
Did you enjoy that arithmetic? (No!) Let’s go
back and do it a better and less painful way.
Why Use Decibels? For convenience and speed.
Here’s an example of why, then we’ll see how.
June, 2011 Page 64Course 601-2-3 (c)2011 Scott Baxter
Example Link Budget Using DB
Let’s track the power flow
again, using decibels.
Receiver
Antenna
Antenna
Trans.
Line
Transmitter
Trans.
Line
+43 dBm TX output
-3 dB line efficiency
= +40 dBm to antenna
+13 dB antenna gain
= +53 dBm ERP
-158 dB path attenuation
= -105 dBm if intercepted by dipole antenna
+13 dB antenna gain
= -92 dBm into line
-3 dB line efficiency
= -95 dBm to receiver
Wasn’t that better?! How to do it -- next.
June, 2011 Page 65Course 601-2-3 (c)2011 Scott Baxter
Decibels - Relative and Absolute
Decibels normally refer to power ratios -- in
other words, the numbers we represent in dB
usually are a ratio of two powers. Examples:
• A certain amplifier amplifies its input by a
factor of 1,000. (Pout/Pin = 1,000). That
amplifier has 30 dB gain.
• A certain transmission line has an efficiency
of only 10 percent. (Pout/Pin = 0.1) The
transmission line has a loss of -10 dB.
Often decibels are used to express an absolute
number of watts, milliwatts, kilowatts, etc....
When used this way, we always append a letter
(W, m, or K) after “db” to show the unit we’re
using. For example,
• 20 dBK = 50 dBW = 80 dBm = 100,000
watts
• 0 dBm = 1 milliwatt
1 watt.001 w
x 1000
0 dBm 30 dBm
+30 dB
100 w
+50 dBm
x 0.10
-10 dB
10 w
+40 dBm
June, 2011 Page 66Course 601-2-3 (c)2011 Scott Baxter
Decibels
Two Other Popular Absolute References
dBrnc: a common telephone noise measurement
• “db above reference noise, C-weighted”
• “Reference Noise” is 1000 Hz. tone at -90 dBm
• “C-weighting”, an arbitrary frequency response,
matches the response best suited for intelligible toll
quality speech
• this standard measures through a “C-message” filter
dBu: a common electric field strength expression
• dBu is “shorthand” for dBµV/m
• “decibels above one microvolt per meter field
strength”
• often we must convert between E-field strength in
dBu and the power recovered by a dipole antenna
bathed in such a field strength:
FSdBu = 20 * Log10(FMHZ) + 75 + PwrDBM
PwrDBM = FSdBu - 20 * Log10(FMHZ)-75
-10dB
-20dB
-30dB
-40dB
0 dB
100 300 1000 3000 10000
Frequency, Hz
C-Message Weighting
Electro-
magnetic
Field
dBµV/m
@ FMHZ
Dipole
Antenna
Pwr dBm
June, 2011 Page 67Course 601-2-3 (c)2011 Scott Baxter
Decibels referring to Voltage or Current
By convention, decibels are based on power ratios.
However, decibels are occasionally used to express to voltage or
current ratios. When doing this, be sure to use these alternate
formulas:
db = 20 x Log10 (V or I) (V or I) = 10 ^ (db/20)
• Example: a signal of 4 volts is 6 db. greater than a signal of 2
volts
db = 20 x Log10 (4/2) = 20 x Log10 (2) = 20 x 0.3 = 6.0 db
June, 2011 Page 68Course 601-2-3 (c)2011 Scott Baxter
Prefixes for Large and Small Units
Large and small quantities
pop up all over
telecommunications and
the world in general.
We like to work in units we
can easily handle, both
in math and in concept.
So, when large or small
numbers arise, we often
use prefixes to scale
them into something
more comfortable:
• Kilometers
• Megahertz
• Milliwatts
– etc....
Summary of Units
Number N x10y Prefix
1,000,000,000,000 x1012 Tera
1,000,000,000 x109 Giga-
1,000,000 x106 Mega-
1,000 x103 Kilo-
100 x102 hecto-
10 x101 deca-
1 x100
0.1 x10-1 deci-
0.01 x10-2 centi-
0.001 x10-3 milli-
0.000001 x10-6 micro-
0.000000001 x10-9 nano-
0.000000000001 x10-12 pico-
0.000000000000001 x10-15 femto-
June, 2011 Page 69Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 70Course 601-2-3 (c)2011 Scott Baxter
Basic BDA/DAS Coverage
Requirements
Basic BDA/DAS Coverage
Requirements
Coverage Tradeoffs
After the desired coverage area is known, the next step is to
determine how many antennas will be required to serve it
Alternatives will be available for antennas of different gains and
transmitters of different power outputs
In general, the solution with the maximum number of antennas will
have the fewest significant coverage holes
June, 2011 Page 71Course 601-2-3 (c)2011 Scott Baxter
A Resource for Indoor Radio Planning
A new version of the bestseller, updated
with an introduction to LTE and
treatments of modulation principle, DAS
systems for MIMO/LTE , designing
repeater systems and elevator coverage
Addresses the challenge of providing
coverage inside train, and high speed rail
Outlines the key parameters and metrics
for designing DAS for GSM, DCS, UMTS,
HSPA & LTE
Essential reading for engineering and
planning personnel at mobile operators,
also giving a sound grounding in indoor
radio planning for equipment
manufacturers
Written by a leading practitioner in the
field with more than 20 years of practical
experience
June, 2011 Page 72Course 601-2-3 (c)2011 Scott Baxter
Radio PropagationRadio Propagation
June, 2011 Page 73Course 601-2-3 (c)2011 Scott Baxter
Some Physics: Wavelength of the Signal
and Its Influence on Propagation
Radio signals in the atmosphere
travel at the speed of light
λ = wavelength
C = distance traveled in 1 second
F = frequency, Hertz
The wavelength of a radio signal
determines many of its propagation
characteristics
• Internal antenna elements’ size are
typically in the order of 1/4 to 1/2
wavelength
• Objects bigger than a wavelength
can reflect or obstruct RF energy
• RF energy can penetrate into a
building or vehicle if it has
openings the size of a wavelength,
or larger
λ = C / F
Frequency,
GHz.
Wavelength
cm. in.
0.92 32.6 12.8
2.4 12.5 4.9
5.8 5.2 2.0
λ/2
June, 2011 Page 74Course 601-2-3 (c)2011 Scott Baxter
Propagation:
Getting the Signal to the Customer
“Propagation” is the name for the general process of getting a
radio signal from one place to another
During propagation, the signal gets weaker because of several
natural processes. This weakening is called “attenuation”.
Point-to-point radio links work best when there is “line-of-sight”
between the two antennas. This is the condition of least
attenuation
• nothing along the way to block the signal
AP SM
June, 2011 Page 75Course 601-2-3 (c)2011 Scott Baxter
The First Fresnel Zone and
Free-Space Propagation
Most of the signal power sent from one antenna to another travels in an
elliptical, “football” shape called the First Fresnel zone.
• the thickness of the zone depends on the signal frequency
If the First Fresnel zone is free of penetration or obstruction by any objects,
we say “free-space” conditions apply
• this is the desirable condition providing highest received signal strength
Sometimes obstructions are unavoidable, and penetrate the first fresnel zone
• this attenuates the signal and reduces the signal strength received at the
other end of the link
• the amount of attenuation depends on the degree of penetration by the
obstruction, and its absorbing characteristics
Frequency,
GHz.
Path,
Miles
Mid-Pt
Fresnel
R, ft
0.92 10 119
2.4 10 74
5.8 10 47
AP SM
June, 2011 Page 76Course 601-2-3 (c)2011 Scott Baxter
Free-Space Propagation Technical Details
The simplest propagation mode
• Antenna radiates energy which spreads in space
• Path Loss, db (between two isotropic antennas)
= 36.58 +20*Log10(FMHZ)+20Log10(DistMILES )
• Path Loss, db (between two dipole antennas)
= 32.26 +20*Log10(FMHZ)+20Log10(DistMILES )
• Notice the rate of signal decay:
• 6 db per octave of distance change, which is
20 db per decade of distance change
Free-Space propagation is applicable if:
• there is only one signal path (no reflections)
• the path is unobstructed (i.e., first Fresnel zone
is not penetrated by obstacles)
First Fresnel Zone =
{Points P where AP + PB - AB < λ/2 }
Fresnel Zone radius d = 1/2 (λD)^(1/2)
1st Fresnel Zone
B
A
d
D
Free Space
“Spreading” Loss
energy intercepted
by receiving
antenna is
proportional to 1/r2
r
June, 2011 Page 77Course 601-2-3 (c)2011 Scott Baxter
Obstructions and their Effects
When an obstruction penetrates the first fresnel zone, the signal is
attenuated. The degree of attenuation depends on
• how much of the first fresnel zone is obstructed
• the absorptive characteristics of the obstructing object(s)
• whether the signal is also reflecting off of other nearby objects,
possibly providing a degree of “fill-in”
Depending on the length of the path, the transmitter power, and
the receiver sensitivity, the link may still work despite the
obstruction
AP SM
June, 2011 Page 78Course 601-2-3 (c)2011 Scott Baxter
Severe Obstructions
When the path is blocked by a major obstruction (large hill,
downtown building, etc.) there will be substantial signal attenuation
Even under this undesirable condition, if the distance is small there
may be enough signal to make the link usable
• A very small amount of the signal will actually diffract (“bend”)
over the obstruction
• the extra attenuation caused by the obstruction can be
calculated by the “knife edge diffraction” model
• this “diffraction loss” can be considered in the link budget to
see the link is likely to be usable anyway
AP SM
June, 2011 Page 79Course 601-2-3 (c)2011 Scott Baxter
Knife-Edge Diffraction
Sometimes a single well-defined
obstruction blocks the path, introducing
additional loss. This calculation is fairly
easy and can be used as a manual tool
to estimate the effects of individual
obstructions.
First calculate the diffraction parameter
ν from the geometry of the path
Next consult the table to obtain the
obstruction loss in db
Add this loss to the otherwise-
determined path loss to obtain the total
path loss.
Other losses such as free space and
reflection cancellation still apply, but
computed independently for the path as
if the obstruction did not exist
H
R1 R2
ν
atten
dB
0
-5
-10
-15
-20
-25
-4 -3 -2 -1 0 1 2 3-5
( + )ν = -H
2
λ
1 1
R1 R2
June, 2011 Page 80Course 601-2-3 (c)2011 Scott Baxter
Foliage and Building Penetration
Considerations
At broadband wireless
frequencies, the penetration loss
entering a building often exceeds
35 db.
• this restricts range so greatly
that antennas are almost
never located inside a building
At broadband wireless
frequencies, trees and other
vegetation effectively block and
absorb the signal
• typical attenuation for just one
mature tree can be 20 db or
more
Unfortunately, neither building nor
vegetation loss can be predicted
accurately. Measurement is the
only way to know accurately what
is happening.
Building
SM
AP
Building
SM
AP
June, 2011 Page 81Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 82Course 601-2-3 (c)2011 Scott Baxter
In-Building PropagationIn-Building Propagation
iBWAVE: Common Commercial Software
for Indoor Propagation Prediction
AWE Communications offers iBWAVE, a commercial indoor propagation prediction
and design tool. This tool is a good example of the current state of the art.
Large database of building material characteristics
Import walls/floorplans from AutoCAD, images or PDF files.
Propagation module offers dominant path and COST 321 multi-wall models.
• accurate propagation results from antennas and radiating cables
• can increase accuracy by calibrating the prediction model with survey data
The Propagation module provides output maps giving a visual representation of
propagation results, even for different technologies and different bands.
• These include signal strength, field strength, best server and soft handoff
maps.
• evaluate different design configurations and instantly get a clear picture of the
impact on coverage and cost.
• The Propagation module delivers professional documentation about the project
for effective communication with customers to facilitate agreements and
approvals.
June, 2011 Page 83Course 601-2-3 (c)2011 Scott Baxter
iBWAVE Examples
June, 2011 Page 84Course 601-2-3 (c)2011 Scott Baxter
iBWAVE Images
June, 2011 Page 85Course 601-2-3 (c)2011 Scott Baxter
iBWAVE Coverage Map
June, 2011 Page 86Course 601-2-3 (c)2011 Scott Baxter
Equipment List
June, 2011 Page 87Course 601-2-3 (c)2011 Scott Baxter
iBwave Documentation
iBwave also provides
documentation capabilities
• Very useful in large
projects
June, 2011 Page 88Course 601-2-3 (c)2011 Scott Baxter
iBwave System Detail Diagram
June, 2011 Page 89Course 601-2-3 (c)2011 Scott Baxter
Stadium Example
Example of stadium detail and calculation of signal levels on each
element
June, 2011 Page 90Course 601-2-3 (c)2011 Scott Baxter
Network Diagram on Floor Plan
June, 2011 Page 91Course 601-2-3 (c)2011 Scott Baxter
Network Diagram on Detailed Floor Plan
June, 2011 Page 92Course 601-2-3 (c)2011 Scott Baxter
Signal Strength on Floor Plan
June, 2011 Page 93Course 601-2-3 (c)2011 Scott Baxter
iBwave Configuration and Display Examples
June, 2011 Page 94Course 601-2-3 (c)2011 Scott Baxter
3-story DAS
components
June, 2011 Page 95Course 601-2-3 (c)2011 Scott Baxter
Equipment Room of Neutral Host System
June, 2011 Page 96Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 97Course 601-2-3 (c)2011 Scott Baxter
Indoor Best Server Plot
Example Indoor best server plot computed by iBWAVE
June, 2011 Page 98Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 99Course 601-2-3 (c)2011 Scott Baxter
RF Propagation in BDA/DAS
Systems
RF Propagation in BDA/DAS
Systems
June, 2011 Page 100Course 601-2-3 (c)2011 Scott Baxter
Antennas for BDA/DAS SystemsAntennas for BDA/DAS Systems
Understanding Antenna Radiation
The Principle Of Current Moments
An antenna is just a passive
conductor carrying RF current
• RF power causes the current
flow
• Current flowing radiates
electromagnetic fields
• Electromagnetic fields cause
current in receiving antennas
The effect of the total antenna is the
sum of what every tiny “slice” of the
antenna is doing
• Radiation of a tiny “slice” is
proportional to its length times
the magnitude of the current in
it, at the phase of the current
TX RX
Width of band
denotes current
magnitude
Zero current
at each end
Maximum current
at the middle
Current induced in
receiving antenna
is vector sum of
contribution of every
tiny “slice” of
radiating antenna
each tiny
imaginary “slice”
of the antenna
does its share
of radiating
June, 2011 Page 101Course 601-2-3 (c)2011 Scott Baxter
Antenna Gain
Antennas are passive devices: they do not produce
power
• Can only receive power in one form and pass
it on in another, minus incidental losses
• Cannot generate power or “amplify”
However, an antenna can appear to have “gain”
compared against another antenna or condition. This
gain can be expressed in dB or as a power ratio. It
applies both to radiating and receiving
A directional antenna, in its direction of maximum
radiation, appears to have “gain” compared against a
non-directional antenna
Gain in one direction comes at the expense of less
radiation in other directions
Antenna Gain is RELATIVE, not ABSOLUTE
• When describing antenna “gain”, the
comparison condition must be stated or
implied
Omni-directional
Antenna
Directional
Antenna
June, 2011 Page 102Course 601-2-3 (c)2011 Scott Baxter
Reference Antennas
Defining Gain And Effective Radiated Power
Isotropic Radiator
• Truly non-directional -- in 3 dimensions
• Difficult to build or approximate physically,
but mathematically very simple to describe
• A popular reference: 1000 MHz and above
– PCS, microwave, etc.
Dipole Antenna
• Non-directional in 2-dimensional plane only
• Can be easily constructed, physically
practical
• A popular reference: below 1000 MHz
– 800 MHz. cellular, land mobile, TV & FM
Isotropic
Antenna
(watts or dBm) ERPEffective Radiated Power Vs. Dipole
Effective Radiated Power Vs. Isotropic
Gain above Dipole reference
Gain above Isotropic radiator
(watts or dBm) EIRP
dBd
dBi
Quantity Units Dipole Antenna
Notice that a dipole
has 2.15 dB gain
compared to an
isotropic antenna.
June, 2011 Page 103Course 601-2-3 (c)2011 Scott Baxter
Radiation Patterns
Key Features And Terminology
An antenna’s directivity is
expressed as a series of patterns
The Horizontal Plane Pattern graphs
the radiation as a function of azimuth
(i.e..,direction N-E-S-W)
The Vertical Plane Pattern graphs the
radiation as a function of elevation (i.e..,
up, down, horizontal)
Antennas are often compared by noting
specific landmark points on their
patterns:
• -3 dB (“HPBW”), -6 dB, -10 dB
points
• Front-to-back ratio
• Angles of nulls, minor lobes, etc.
Typical Example
Horizontal Plane Pattern
0 (N)
90
(E)
180 (S)
270
(W)
0
-10
-20
-30 dB
Notice -3 dB points
Front-to-back Ratio
10 dB
points
Main
Lobe
a Minor
Lobe
nulls or
minim
June, 2011 Page 104Course 601-2-3 (c)2011 Scott Baxter
In phase
Out of
phase
How Antennas Achieve Their Gain
Quasi-Optical Techniques (reflection, focusing)
• Reflectors can be used to concentrate
radiation
– technique works best at microwave frequencies,
where reflectors are small
• Examples:
– corner reflector used at cellular or higher
frequencies
– parabolic reflector used at microwave
frequencies
– grid or single pipe reflector for cellular
Array techniques (discrete elements)
• Power is fed or coupled to multiple
antenna elements; each element radiates
• Elements’ radiation in phase in some
directions
• In other directions, a phase delay for each
element creates pattern lobes and nulls
June, 2011 Page 105Course 601-2-3 (c)2011 Scott Baxter
Types Of Arrays
Collinear vertical arrays
• Essentially omnidirectional in
horizontal plane
• Power gain approximately
equal to the number of
elements
• Nulls exist in vertical pattern,
unless deliberately filled
Arrays in horizontal plane
• Directional in horizontal
plane: useful for sectorization
• Yagi
– one driven element, parasitic
coupling to others
• Log-periodic
– all elements driven
– wide bandwidth
All of these types of antennas are
used in wireless
RF
power
RF
power
June, 2011 Page 106Course 601-2-3 (c)2011 Scott Baxter
Omni Antennas
Collinear Vertical Arrays
The family of omni-directional wireless
antennas:
Number of elements determines
• Physical size
• Gain
• Beamwidth, first null angle
Models with many elements have
very narrow beamwidths
• Require stable mounting and
careful alignment
• Watch out: be sure nulls do
not fall in important coverage
areas
Rod and grid reflectors are
sometimes added for mild directivity
Examples: 800 MHz.: dB803, PD10017,
BCR-10O, Kathrein 740-198
1900 MHz.: dB-910, ASPP2933
beamwidth
Angle
of
first
null
θ
-3
d
B
Vertical Plane Pattern
Number of
Elements
Power
Gain
Gain,
dB
Angle
θ
0.00 n/a
3.01 26.57°
4.77 18.43°
6.02 14.04°
6.99 11.31°
7.78 9.46°
8.45 8.13°
9.03 7.13°
9.54 6.34°
10.00 5.71°
10.41 5.19°
10.79 4.76°
11.14 4.40°
1
2
3
4
5
6
7
8
9
10
11
12
13
14
1
2
3
4
5
6
7
8
9
10
11
12
13
14 11.46 4.09°
Typical Collinear Arrays
June, 2011 Page 107Course 601-2-3 (c)2011 Scott Baxter
Sector Antennas
Reflectors And Vertical Arrays
Typical commercial sector
antennas are vertical combinations
of dipoles, yagis, or log-periodic
elements with reflector (panel or
grid) backing
• Vertical plane pattern is
determined by number of
vertically-separated
elements
– varies from 1 to 8, affecting
mainly gain and vertical plane
beamwidth
• Horizontal plane pattern is
determined by:
– number of horizontally-spaced
elements
– shape of reflectors (is reflector
folded?)
Vertical Plane Pattern
Up
Down
Horizontal Plane Pattern
N
E
S
W
June, 2011 Page 108Course 601-2-3 (c)2011 Scott Baxter
Pattern of Canopy AP Internal Patch Antenna
June, 2011 Page 109Course 601-2-3 (c)2011 Scott Baxter
Andrew Radiax
June, 2011 Page 110Course 601-2-3 (c)2011 Scott Baxter
Radiax Design Considerations
System Architecture for a specific application will depend on overall objectives
• dictated in large part by the geometry and area that is required for coverage.
• For tunnel applications, the length, construction, and the size of the tunnel will
establish the basic parameters.
• Other key factors include the number of services, providers, and channels
required to meet the objectives.
For tunnel applications, the two primary architectures used are:
• A series of cascaded amplifiers or
• Using a T-feed configuration.
In some implementations, it is smart to use a combination of these two techniques.
• The T-feed structure is appropriate when feeding from multiple base stations or
when using amplifiers that are connected to a common base station using fiber
• The T-feed structure has the advantage that an amplifier can drive a longer
length of cable than can be achieved with the cascaded architecture.
• The T-feed structure generates less downlink intermodulation since the
amplifiers are not cascaded.
• The cascaded configuration has a higher dynamic range on the uplink and is
useful for communication systems that do not use uplink power control.
• The cascade configuration has been used effectively on tunnels where the
communication system employs conventional or trunk radio techniques.
• The T-feed configuration has been particularly well suited for cellular and PCS
applications.
June, 2011 Page 111Course 601-2-3 (c)2011 Scott Baxter
Radiax Applications
Cable Parameters
• Insertion Loss
• Coupling Loss
• Fading Characteristic
• Coherent Bandwidth
• Launch Angle
Insertion Loss
• a measure of the attenuation in the coaxial cable, measured in dB per unit length.
• primarily a result of the copper losses and the amount of power that is radiated from the cable.
• The loss due to radiation is somewhat affected by the proximity of the cable to other surfaces.
• This effect is more pronounced for cables having low coupling loss, however, significant changes will typically not occur until
the spacing is less than 1 inch.
Coupling Loss
• Coupling loss is the ratio between the power in the cable and the amount of power received by a dipole antenna at a specified
distance from the cable.
• For example, if the power in the cable were 0 dBm and the power received by the antenna was -65 dBm, then the coupling loss
would be 65 dB.
• Typically Andrew will use distances of 2 meters (6.6 feet) or 6 meters (20 feet).
• The value specified is the median value measured as the dipole travels parallel to the cable.
• Typically, the radiated energy from the radiating cables is polarized. The degree of polarization is measured for all Andrew
cables. The majority of the Andrew radiating cables have a dominant vertical polarization, however, this may be frequency
dependent.
Fading Characteristic
• Radiating cables exhibit a fading characteristic that is a result of the multipath nature of the cable.
• Typically, a fade will occur approximately every wavelength.
• The depth of the fade is dependant not only on the design of the cable but also on the multipath environment.
• Andrew quantifies the depth of fading by calculating the ratio between the median value of the coupling loss (50%) to the
coupling loss that occurs at least 5%.
• This produces a ratio of the 50 to 95% values.
• For coupled mode RADIAX (RXL), the fading factor is typically 11 dB.
• For RADIAX utilizing the array construction, radiating mode RADIAX (RCT), this value can be as low as 2 to 3 dB.
• In a majority of systems applications, the low fading characteristic is somewhat negated by the environment
June, 2011 Page 112Course 601-2-3 (c)2011 Scott Baxter
Radiax - Tunnels
Coherent Bandwidth
• a measure of instantaneous bandwidth of the signal that can reliably be transmitted from
the cable.
• significant for wide bandwidth signals, especially third generation systems.
• For applications involving wider bandwidths, the radiating mode cables (RCT) are
designed to handle third generation signals.
Launch Angle
• For coupled mode RADIAX®, there is no dominant launch angle as RF energy emits from
the cable at all angles.
• For the radiating mode series of cables there is a dominant launch angle.
• this dominant launch angle contributes to the low fading characteristic and the wider
coherent bandwidth. The launch angle for any particular cable varies as a function of
frequency and will typically be (45 degrees relative to a perpendicular line from the cable.
Cable Orientation
• For most cables, the orientation of the slots is not critical.
• the dominant radiation is not directly from the slots, rather caused by current that flows in
the outer jacket of the cable.
• Directivity of the cable is related to the frequency and the size of the cable. That is, a 1-5/8
inch cable at 2400 MHz will be more directive than at 900 MHz, further the 1-5/8 inch cable
will have a higher directivity than a 7/8" cable.
Link Budget
• basic elements of a link budget can be demonstrated by considering an example that
involves a dual-bore road tunnel that is 800 meters (2620 feet) in length that is to be
configured to handle cellular signals (824 MHz-894 MHz). The power per channel
available for the downlink is 1 watt (+30 dBm). Following is an example link budget:
June, 2011 Page 113Course 601-2-3 (c)2011 Scott Baxter
Radiax – Tunnels (2)
Downlink (Base to Mobile) Link Budget for 95% Coverage
Available Power/Channel 30 dBm
Distribution Loss, Power divider feeds both bores 3.5 dB
Feeder Cable Loss, 30 m (100 ft) LDF5-50 1.6 dB
Insertion Loss, 800 m (2620 ft) RCT7-TC-1 18.4 dB
Coupling Loss @ 2 m 53.0 dB
Antenna Loss, relative to dipole 3 dB
Wide Tunnel Factor, tunnel width 10 m (33 ft),
Wide Tunnel Factor = 20 Log (Width/2) 14 dB
Vehicle Penetration Loss 6 dB
Raleigh Fading, Z(Σ(σil2+σcl2+σant2+σ...)1/2 11 dB
Statistical Variation 3 dB
Tunnel Factors 0 dB
Received Signal Power (Level that will be achieved at least 95% of the
time at the terminated end of the cable) -83.5 dBm
Uplink performance can be computed in a very similar manner.
June, 2011 Page 114Course 601-2-3 (c)2011 Scott Baxter
Radiax – Tunnels (3)
Tunnel Effects on Design
Coupling loss is dependent on the construction and shape of the
tunnel. Typically, steel tunnels will perform appreciably better than
concrete tunnels. Another factor that modifies the performance of
the system is the placement of the cable in the tunnel. The cable
should be mounted in the manner, which provides the best line-of-
sight and proximity to the mobile/portable antenna
June, 2011 Page 115Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 116Course 601-2-3 (c)2011 Scott Baxter
BDA/DAS System Link BudgetsBDA/DAS System Link Budgets
DAS Link Budgets
The Components and Calculations of the RF Link
The Maximum Allowable Path Loss
The Components in the Link Budget
Link Budgets for Indoor Systems
Passive DAS Link Budget
Active DAS Link Budget
The Free Space Loss
The Modified Indoor Model
The PLS Model
Calculating the Antenna Service Radius
June, 2011 Page 117Course 601-2-3 (c)2011 Scott Baxter
Link Budgets
What is a link budget?
A link budget is the calculation of signal strength on a Distributed
Antenna System (DAS) at coax connection points. Example of a
downlink link budget for one indoor antenna DAS; Roof RSSI(-
75dBm) + gain donor antenna (11dB) + loss coax to BDA (3dB) +
gain BDA (62dB) + loss coax to indoor antenna (4.5dB) = -9.5dBm
at indoor antenna port.
June, 2011 Page 118Course 601-2-3 (c)2011 Scott Baxter
Coverage Area of An Antenna
Antenna coverage is determined by
• the building characteristic path loss,
• frequency band(s),
• signal strength at antenna port and antenna type.
For example, in a typical office application, an omni antenna with
an output signal of +9.5dBm will maintain a coverage area of
+85dB or better for 22k square feet on the cellular frequency band,
16k square feet on the PCS frequency band.
June, 2011 Page 119Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 120Course 601-2-3 (c)2011 Scott Baxter
BDA/DAS Equipment
Manufacturers and Products
BDA/DAS Equipment
Manufacturers and Products
Mobile Access Hardware Selection
June, 2011 Page 121Course 601-2-3 (c)2011 Scott Baxter
Mobile Access Hardware (2)
June, 2011 Page 122Course 601-2-3 (c)2011 Scott Baxter
Mobile Access Hardware (3)
June, 2011 Page 123Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 124Course 601-2-3 (c)2011 Scott Baxter
BDA/DAS Installation Techniques
and Practices
BDA/DAS Installation Techniques
and Practices
How to Properly Design an In-Building
Distributed Antenna System (DAS)
A typical in-building coverage system consists of two major components,
• a bi-directional amplifier relaying and amplifying the RF signals
between the remote base station and portable or mobile radios, and
• a network to distribute the signal to every corner of the desired
coverage area.
The most common type of distribution network is a system of coax cables
and indoor antennas called a Distributed Antenna System or DAS.
Most of the reference materials and application notes on in-building
coverage solutions have focused on the booster technologies or system
design architecture.
One often overlooked aspect in the system design is the DAS
implementation.
• This includes connecting all the cables and antennas throughout the
building and balancing the signal levels at each DAS node.
• If ignored, an improperly designed DAS results in degraded
performance and unnecessary cost increases.
June, 2011 Page 125Course 601-2-3 (c)2011 Scott Baxter
The DAS Design Process
The first step of DAS design is to obtain an accurate and up-to-date blueprint of the building.
• An architectural drawing is best, but even a fire exit map will suffice, if drawn to scale.
Be careful when using the scale on any drawing to calculate the real dimensions;
• the drawing may not be the same size as originally printed. .
The second step is to gather all relevant physical information on building and DAS installation.
• What kind of material was used for exterior construction?
• Could some RF signals be present on upper floors and near exterior boundaries that will
reduce the need for the in-building coverage?
• What kind of material was used for interior construction, drywall or concrete?
• Is the building designed for a special application that may result in RF blockage?
• Many hospitals and power generating plants fall into this category.
• Are there any restrictions on the cable runs and antennas installation?
• Some buildings won’t allow any visible hardware for aesthetic reasons.
• Where can the cables go between floors? Where will the head-end booster be located?
• A quick word on another type of DAS: radiating cable. It is essentially a coax cable with
lots of tiny slits cut along the length of the cable. Each slit functions as a tiny antenna with
RF energy leaking out of it, hence the nickname “leaky cable”.
June, 2011 Page 126Course 601-2-3 (c)2011 Scott Baxter
Two Sets of Diagrams
To make it easier to see, a DAS design is often drawn up with 2
sets of diagrams
• one with direct marking on the building blueprint to indicate the
location of the antennas and cable splits,
• a second set of “abstract” drawings (typically in VisioTM or
AutocadTM) showing the cable lengths and coupler models.
how do you connect all the cable segments and antennas to make
them into a network?
• directional couplers are much better alternatives than splitters
at this task.
• They offer various power split ratios to allow the designer
flexibility in balancing the power level at each DAS node.
The main goal of using couplers is to offset the difference in cable
losses by using the different loss ratios between the two outputs of
the coupler.
June, 2011 Page 127Course 601-2-3 (c)2011 Scott Baxter
Balancing Losses Using Couplers
With 15 dB loss in one branch vs. 5 dB loss in the other, let’s select a coupler that has 10 dB of difference in power split ratios.
• Put the lower loss port on the higher loss branch, and the higher loss port on the lower loss branch
• Most manufacturers provide products with different split ratios to allow matching the loss differentials as closely as possible.
In the left Figure, we have a branch with 150 ft and about 3.3 dB of insertion loss, and a branch of 3 ft jumper cable with 0.5 dB of loss.
• select a coupler that can make up the loss differential in the two cable runs.
• Browsing, select a coupler with a 4.8/1.8 dB split ratio as Coupler #1.
• connect the longer cable run to the port with 1.8 dB, and connect the shorter cable run to the 4.8 dB, the total losses from the
input of the coupler to the antennas are 3.3 + 1.8 = 5.1 dB and 0.5 + 4.8 = 5.3 dB respectively.
• If we had used a 3 dB splitter, the total losses would have been 3.3 + 3 = 6.3 dB and 0.5 + 3 = 3.5 dB.
• see the benefit of using a coupler as it manages to balance the signal levels at the two antennas within 0.2 dB of each other.
• Next, work backwards toward the booster. Take the worse number of the two above (5.1 and 5.3 dB, so we use 5.3 dB), and
add the 0.5 dB cable loss between the two couplers, we get 5.8 dB, which is the loss from the output of Coupler #2 to either
Antenna #1 or Antenna #2.
June, 2011 Page 128Course 601-2-3 (c)2011 Scott Baxter
Balancing Losses Using Couplers
Assume there are more floors above this one. The DAS on the upper floor has
been balanced using couplers in the same way as illustrated, and the total loss in
the DAS on the upper floor is 10 dB. See the left figure as we “propagate” the loss
in the DAS backwards toward the booster.
We want to select a coupler that will offset the loss differential and balance the
signal levels.
we find a coupler with a 6/1.2 dB split ratio. If we connect the 6 dB coupled port to
the lower loss DAS on this floor, and the 1.2 dB throughput port to the higher loss
DAS on the upper floor, we get 5.8 + 6 = 11.8 dB and 10 + 1.2 = 11.2 dB.
The total losses from the input of Coupler #2 to the cable runs on this floor and the
cable runs on the upper floor are within 0.6 dB of each other.
June, 2011 Page 129Course 601-2-3 (c)2011 Scott Baxter
Continuing Back to the Booster
If there are more floors below it or more cable splits between this one and
the booster, the same iteration is to be repeated until we work all the way
back to the booster.
A typical in-building coverage system can vary from 10,000 sq ft to
1,000,000 sq ft or more, with the number of couplers from a handful to
hundreds.
However, the rules of calculating the losses and selecting the couplers
stay the same, allowing the designer to balance any DAS and achieve the
optimal signal levels throughout the network.
The total DAS loss should be limited to no more than 25~30 dB, in order
to maintain a sufficient signal to noise ratio.
working backwards toward the booster, eventually the system loss
exceeds the limit.
We know that we will need to insert an in-line booster at that point.
The exact location depends on the practical constraints of the building, but
wherever the in-line booster is, the cumulative loss ends at its output, and
starts from zero again on the other side of the in-line booster.
Another alternative is to use coax with larger diameters with lower
insertion loss. But that option has high material and labor costs, as well as
the physical limitations on bending radius and weight support issues.
June, 2011 Page 130Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 131Course 601-2-3 (c)2011 Scott Baxter
BDA/DAS Example Case StudiesBDA/DAS Example Case Studies
Site Survey
A site survey is performed prior to the final design. Objectives:
• to characterize signal propagation within the building
• investigate donor signal options and to
• investigate equipment space and cable routing issues.
Proper engineering and planning will minimize capital expenditures
while ensuring that coverage goals for each of the mobile service
providers are met.
Several factors must be considered when designing a neutral
hosts system.
• characterize signal propagation within the target area.
• test transmitters are placed at various locations within the
building.
• A receiver and mapping software are used to record the signal
strength at various locations within the building.
A sample transmitter test is shown on the next page.
June, 2011 Page 132Course 601-2-3 (c)2011 Scott Baxter
Site Survey Results Map
June, 2011 Page 133Course 601-2-3 (c)2011 Scott Baxter
Site Survey Results
Various transmitter tests are performed to get a thorough understanding of
the building’s propagation characteristics
In the test just shown, signal loss does not degrade in direct proportion to
the distance from the transmitter but is largely dependant on the building
structure.
• Using the proper tools and procedures to characterize signal loss
helps ensure that the system is not over designed and meets
customer requirements.
Suitable equipment room space and it’s proximity to the coverage
objective strongly affect the type of system installed and its overall cost.
• These issues are investigated at the time of the site survey.
Potential donor signals are also investigated for neutral host opportunities
that may not require dedicated base stations.
• These measurements are generally performed at the roof level.
• A receiver capable of measuring multiple technologies and
frequencies is required for these measurements.
• Alternatively phones from various carriers with an accessible
diagnostic or debug mode can be used.
Potential donor antenna locations and roof penetration issues also need to
be investigated at this stage.
June, 2011 Page 134Course 601-2-3 (c)2011 Scott Baxter
System Design
The building characterization along with available equipment
space determined during the site survey is the basis for system
design.
The propagation model is optimized for accuracy using the
transmitter tests performed in the site survey.
• Each wall type within a building affects signal propagation
differently therefore each wall type must be identified in the
propagation model and assigned attenuation values obtained
from the information in the transmitter tests.
• This allows for optimum transmitter location and minimizes
required capital. The system design determines which OEM
hardware solution is appropriate for the venue. A partial design
(one floor of a multi story building) is shown in the next figure.
June, 2011 Page 135Course 601-2-3 (c)2011 Scott Baxter
One Floor Design
June, 2011 Page 136Course 601-2-3 (c)2011 Scott Baxter
Construction
Once the proposed design is approved for installation by the building
manager, a preconstruction site visit is completed.
• During this visit, equipment locations and cable routes are verified, as
well as acceptable contractors to perform any electrical or roofing
work that may be required.
• If any of the locations proposed in the design are not acceptable to the
building manager, the design is modified to allow for these changes.
• Once final approval is obtained, the actual installation of equipment
begins.
Construction begins with the installation of cabling, typically both fiberoptic
and coaxial.
• Cabling is routed from the main equipment room throughout the
building to all the antenna locations.
A DAS system allows for the reuse of many network elements - trunking
and hubbing minimize the amount of new cable required. Cable is run in
existing cable trays or utility chases where available.
The equipment deployment is fairly straight forward. The main equipment
room typically needs dedicated electrical services to handle both the DAS
equipment and the carrier equipment. The remote units and the antenna
use minimal power and usually only involve a 110v outlet.
June, 2011 Page 137Course 601-2-3 (c)2011 Scott Baxter
Optimization and Verification
When the construction phase is complete, the system is tested and
optimized.
• Each coax and fiber optic cable is swept,
• isolation tests are performed,
• sources of interference are investigated,
• donor signal levels are verified, and
• a final coverage assessment is performed.
• The results of the coverage analysis reflect both coverage
provided by the external macro cell and enhanced coverage
provided by the DAS.
The next page show is a sample plot that can be used to measure
the success of the installation.
June, 2011 Page 138Course 601-2-3 (c)2011 Scott Baxter
Signal Levels After Activation
June, 2011 Page 139Course 601-2-3 (c)2011 Scott Baxter
DAS Reduce Interference to Medical Devices
Interference Concerns
Much has been written about cellular devices interfering with medical
equipment. Generally, the use of a DAS will greatly lower the power
output of the mobile device, reducing the risk of interference.
Poor coverage inside a building means that a mobile device has to
transmit at a higher power setting to ensure that a connection with the cell
site is made.
Cellular devices can transmit at relatively high power levels (perhaps 1 W)
for short periods of time such as during the ring cycle. However, if the
cellular device is in a reasonably good coverage location, it will transmit at
much lower levels (potentially under 5 mW), which is not a real concern.
In addition if you have good coverage, the battery life of the device will be
greatly enhanced. Essentially a DAS provides 5 bars all the time, thus less
power is required to enable the up-link from the mobile devices. The use
of DAS in healthcare will actually decrease electromagnetic interference
and improve battery life of these devices.
June, 2011 Page 140Course 601-2-3 (c)2011 Scott Baxter
June, 2011 Page 141Course 601-2-3 (c)2011 Scott Baxter
Course 603
Wireless BDA and DAS
Advanced Topics
Wireless BDA and DAS
Advanced Topics
June, 2011 Page 142Course 601-2-3 (c)2011 Scott Baxter
603 Course Outline
Traffic Capacity of BDA/DAS Systems
Intermodulation Distortion and Interference
External Interference Interference Sources
MIMO – Multiple Input-Output Broadband Data Systems
Femtocells
• Comparison of function and performance against BDA/DAS
technologies
• Differences and advantages
June, 2011 Page 143Course 601-2-3 (c)2011 Scott Baxter
Intermodulation Distortion and
Interference
Intermodulation Distortion and
Interference
Modulation and Mixing vs. Intermodulation
When two signals are intentionally combined in a non-
linear device we call the effect modulation
• Amplitude modulator, or quad phase modulator
• Mixer, down or up converter in superheterodyne
When two (or more) signals are unintentionally combined
in a non-linear device, we call the effect intermodulation (a
pejorative term)
An analogy: Botanists use soil to grow plants. But on your living
room carpet, soil is just dirt.
IM signals increase system noise, or cause distinctive
recognizable interference signals
June, 2011 Page 144Course 601-2-3 (c)2011 Scott Baxter
Intermod Basics
Definition: Intermodulation (“IM”) is
the unintended mixing of legitimate
RF signals, producing undesired
signals (‘intermodulation products’) on
unrelated frequencies possibly
already being used for other services
• IM can devastate reception on
certain frequencies at base
stations and other communication
facilities
Intermodulation occurs because
signals are passing through a
nonlinear device, allowing each signal
to alter the waveshape of the others
• the frequencies of the intermod
products are sums and
differences of multiples of the
original signal frequencies, and
can be calculated exactly
• the strength of the intermod
products depends on the degree
of nonlinearity of the circuits
involved, and can be predicted
with good accuracy using
measured “intercept” levels
Power transfer characteristics
of typical amplifier or other device
Noise floor
Input power (dBm)
Output
power
(dBm)
Third order
intercept
point
Third order
intermodulation
products
Predicted
power
f
f1 f2
Non-linear deviceInput Output
f
3f1-2f2 3f2-2f1f1 f2
2f2-f12f1-f2
June, 2011 Page 145Course 601-2-3 (c)2011 Scott Baxter
Intermodulation Interference Analysis
There are three basic categories of
Intermodulation (IM) interference:
Transmitter produced IM is the result of
one or more transmitters impressing a signal
in the non-linear final output stage circuitry of
another transmitter, usually via antenna
coupling. The IM product frequency is then
re-radiated from the transmitter's antenna.
Receiver produced IM is the result of two or
more transmitter signals mixing in a receiver
RF amplifier or mixer stage when operating
in a non-linear range.
“Other" radiated IM is the result of
transmitter signals mixing in other non-linear
junctions. These junctions are usually
metallic, such as rusty bolts on a tower,
dissimilar metallic junctions, or other non-
linear metallic junctions in the area. IM
products can also be caused by non-linearity
in the transmission system such as antenna,
transmission line, or connectors.
BPF Preamp Splitter RX
TXCircDuplexer Comb
TXCircDuplexer Comb
June, 2011 Page 146Course 601-2-3 (c)2011 Scott Baxter
Intermodulation Interference Analysis
Communication sites with co-located transmitters, usually have RF
coupling between each transmitter and antenna system.
• This results in the signals of each transmitter entering the
nonlinear final output (PA) circuitry of the other transmitters.
When intermodulation (IM) products are created in the output
circuitry and they fall within the passband of the final amplifier, the IM
products are re-radiated and may interfere with receivers at the
same site or at other nearby sites.
Additionally, these strong transmitter signals may directly enter a
receiver and drive the RF amplifier into a nonlinear operation, or
• if not filtered effectively by the receiver input circuitry, these
signals could mix in the nonlinear circuitry of the receiver front-
end or mixer, creating IM products directly in the receiver.
June, 2011 Page 147Course 601-2-3 (c)2011 Scott Baxter
Transmitter Noise Analysis
Transmitter noise interference occurs because a transmitter
radiates energy on its operating frequency as well as frequencies
above and below the assigned frequency.
The energy that is radiated above and below the assigned
frequency is known as sideband noise energy and extends for
several megahertz on either side of the operating frequency.
This undesired noise energy can fall within the passband of a
nearby receiver even if the receiver's operating frequency is
several megahertz away.
The transmitter noise appears as "on-channel" noise interference
and cannot be filtered out at the receiver.
• It is on the receiver's operating frequency and competes with
the desired signal, which in effect, degrades the operational
performance.
June, 2011 Page 148Course 601-2-3 (c)2011 Scott Baxter
Transmitter Noise Analysis
The analysis predicts each transmitter’s noise signal level present
at the input of each receiver.
• It takes into account the transmitter’s noise characteristics,
frequency separation, power output, transmission line losses,
filters, duplexers, combiners, isolators, multi-couplers and
other RF devices that are present in both systems.
• Additionally, the analysis considers the antenna separation
space loss, horizontal and vertical gain components of the
antennas as well as how they are mounted on the structure.
The gain components are derived from antenna pattern data
published by each manufacturer.
June, 2011 Page 149Course 601-2-3 (c)2011 Scott Baxter
Transmitter Noise Analysis
The analysis determines how much isolation is required, if any, to
prevent receiver performance degradation caused by transmitter
noise interference.
The Table below depicts the results of this analysis. For each
receiver, the transmitter that has the worst-case impact is
displayed.
The Signal Margin represents the margin in dB, before the
receiver’s performance is degraded.
A negative number indicates that the performance is degraded and
the value indicates how much additional isolation is required to
prevent receiver performance degradation
June, 2011 Page 150Course 601-2-3 (c)2011 Scott Baxter
Receiver Desensitization Analysis
Receiver desensitization interference occurs when an
undesired signal from a nearby "off-frequency" transmitter is
sufficiently close to a receiver's operating frequency.
The signal may get through the RF selectivity of the receiver.
If this undesired signal is of sufficient amplitude, the
receiver's critical voltage and current levels are altered and
the performance of the receiver is degraded at its operating
frequency.
The gain of the receiver is reduced, thereby reducing the
performance of the receiver.
June, 2011 Page 151Course 601-2-3 (c)2011 Scott Baxter
Receiver Desensitization Analysis
A transmitter can be operating several megahertz away from the
receiver frequency and/or its antenna can be located several
thousand feet from the receiver's antenna and still cause
interference.
The analysis predicts each transmitter’s signal level present at the
input of each receiver. It takes into account the transmitter’s
power output, frequency separation, transmission line losses,
filters, duplexers, combiners, isolators, multi-couplers and other
RF devices that are present in both systems. Additionally, the
analysis considers the antenna separation space loss, horizontal
and vertical gain components of the antennas as well as how they
are mounted on the structure. The gain components are derived
from antenna pattern data published by each manufacturer.
June, 2011 Page 152Course 601-2-3 (c)2011 Scott Baxter
Receiver Desensitization Analysis
The analysis determines how much isolation is required, if any, to
prevent receiver performance degradation caused by receiver
desensitization interference.
The Table provided separately depicts the results of this analysis.
• For each receiver, the transmitter that has the worst-case
impact is displayed.
• The Signal Margin represents the margin in dB, before the
receiver’s performance is degraded.
• A negative number indicates that the performance is degraded
and the value indicates how much additional isolation is
required to prevent receiver performance degradation.
June, 2011 Page 153Course 601-2-3 (c)2011 Scott Baxter
Intermodulation Interference Analysis
The frequencies of IM products are derived from mathematical
formulae. IM products are classified by their "order" (2nd, 3rd, 4th,
...Nth). Some of the more common forms of mixing are illustrated
in the following examples. Note that The "A", "B", and "C"
designations are the mixing frequencies. The numerical number
assigned to the letter designation indicates the harmonic
relationship of the frequency. Thus, 2A means the 2nd harmonic
of frequency A.
Order Mixing Formulae
First A=B, A=C, etc.
Second A ± B, A ± C, etc.
Third A + B - C, A ± 2B, 2A ± B, etc.
Fourth A ± 3B, 2A ± 2B, 3A ± B, etc.
Fifth A ± 4B, 2A ± 3B, 3A ± 2B, 4A ± B, etc.
Sixth A ± 3B ± 2C, 2A ± 2B ± 2C, 3A ± 2B ± C, etc.
Seventh A ± 6B, 2A ± 5B, 3A ± 4B, 4A ± 3B, 5A ± 2B, etc.
Eighth A ± 7B, 2A ± 6B, 3A ± 5B, 4A ± 4B, 5A ± 3B, 6A ± 2B,
Ninth A ± 8B, 2A ± 7B, 3A ± 6B, 4A ± 5B, 5A ± 4B, 6A ± 3B, c.
June, 2011 Page 154Course 601-2-3 (c)2011 Scott Baxter
Intermodulation Interference Analysis
The IM product formulae are just a few of the many possible
combinations. When there are four frequencies involved at one
time, the mixing possibilities increase tremendously. Not all of the
mixing possibilities are significant in creating interference signals.
Some fall “out-of-band” of the receiver and the higher order IM
products are usually weaker in signal strength.
June, 2011 Page 155Course 601-2-3 (c)2011 Scott Baxter
Transmitter Spurious Output Interference
Analysis
Transmitter spurious output interference can be attributed to many
different factors in a transmitter. The generation of spurious
frequencies could be due to non-linear characteristics in a
transmitter or possibly the physical placement of components and
unwanted coupling. If a spurious signal falls within the passband of
a nearby receiver and the signal level is of sufficient amplitude, it
can degrade the performance of the receiver.
June, 2011 Page 156Course 601-2-3 (c)2011 Scott Baxter
Transmitter Spurious Output Interference
Analysis
The analysis takes into account a transmitter’s spurious output
specification, output levels, transmission line losses, filters,
duplexers, combiners, isolators, multi-couplers and other RF
devices that are present in each system. Additionally, the analysis
considers the antenna separation space loss, horizontal and
vertical gain components of the antennas as well as how they are
mounted on the structure. The gain components are derived from
antenna pattern data published by each manufacturer.
The analysis determines how much isolation is required to prevent
receiver performance degradation for any transmitter spurious
signals that fall within a receiver’s passband.
June, 2011 Page 157Course 601-2-3 (c)2011 Scott Baxter
Non-linear Effects and Intermodulation
Almost “everything” is slightly (or extremely) non-linear. Only free
space is theoretically a true linear medium. Particularly non-linear are:
• all active semiconductor devices
• corroded electrical connections, etc.
When high RF current levels are present in non-linear devices,
waveform distortion occurs
• A distorted (clipped, peaked, etc.) non-sinusoidal waveform is
equivalent to a sum of sine waves of several different frequencies
(Fourier series)
• Product waveforms can also occur when two frequencies are
“mixed” due to the non-linearity
• if the nonlinear device characteristics are accurately known
(intercept point, etc.), IM amplitudes can be accurately computed.
• If nonlinear device characteristics are unknown, the worst-case
intermod mechanism will have a conversion loss of at least 6 dB.
June, 2011 Page 158Course 601-2-3 (c)2011 Scott Baxter
What to do about IM
Try to prevent or reduce the amplitude of strong RF signals
reaching receivers in wireless systems
• Reduce or eliminate at the source, if feasible (spurious
emissions from electric lamps, signs, elevator motors, etc.)
• Shielding, enclosure, modification of antenna directionality to
reduce the penetration of electromagnetic waves
• Identify and eliminate secondary non-linear radiators: parallel
metal joints with conductive connections, ground all parts of
metal fences, rain gutters, etc. (also improves lightning
protection)
• Conducted RF from wires, etc. entering receiver can be
reduced via low pass or band pass filters, ferrite beads, etc.
• Notch filters to remove source RF, or specific harmonics or
products
June, 2011 Page 159Course 601-2-3 (c)2011 Scott Baxter
Intermod “Forensics”Intermod “Forensics”
June, 2011 Page 160Course 601-2-3 (c)2011 Scott Baxter
Intermod “Forensics” and Detective Work
“Detective” Work to identify
• the likely creation paths for an observed intermod problem
• methods of reducing the intermod production or delivery to
non-problematic levels
Identify source and victim destination
• analyze each conceivable path
– gains, isolations, line losses, conversion losses, bandpass
filters in the path
– compute the likely intermod amplitude at the victim due to
that path
– the path with the largest calculated amplitude at the victim
is the most suspect and should be investigated or mitigated
first
June, 2011 Page 161Course 601-2-3 (c)2011 Scott Baxter
Truth Serum for a Witchhunt:
a lowly attenuator
Often the source of intermod is unclear – it could be anywhere:
• In the affected victim receiver
• In a transmitter of one of the source signals
• In some other nonlinear device nearby
A simple attenuator (usually 3, 6 or 10 db “pad”) can be used to help
isolate where the intermod is occuring
• Place pad in front of the victim receiver
– If the intermod decreases the same amount as the pad
attenuation, it is coming in from outside, beyond the pad
Keep looking elsewhere
– If the intermod decreases by a multiple of the pad attenuation, it
is being generated in the receiver
Consider additional filtering for the receiver
• Place high power pad in front of the transmitters, one by one
– When the intermod is reduced by the maximum amount, the pad
is on the transmitter producing most of the intermod
June, 2011 Page 162Course 601-2-3 (c)2011 Scott Baxter
Using an Attenuator for Intermodulation
Location
TX1
TX2
RX
IM
-90 dbm
Troublesome intermod
is received on a
product frequency of
TX1 and TX2. Where
is the source?
TX1
TX2
RX
IM
-96 dbm
A 6 db pad on the
receiver merely
reduces all signals
including the intermod
by 6 db. The intermod
is originating outside
this receiver.
6 db
TX1
TX2
RX
IM
-102 dbm
With a 6 db pad on
TX1, the intermod
goes down 12 db. The
intermod is reduced,
but this does not prove
where the IM is
generated.
6 db
TX1
RX
IM
-114 dbm
With a 6 db pad on TX2,
the intermod goes down
lower than anywhere
else. TX2 is an intermod
generator.Now consider
additional flitering for
TX2 to suppress the IM.
6 db
TX2
June, 2011 Page 163Course 601-2-3 (c)2011 Scott Baxter
Working With Repeaters
AKA Re-Radiators, Cell Enhancers, Boosters
Working With Repeaters
AKA Re-Radiators, Cell Enhancers, Boosters
June, 2011 Page 164Course 601-2-3 (c)2011 Scott Baxter
Cell RR
Wireless Reradiators
Reradiators (also called “boosters”,
“repeaters”, “cell enhancers”) are amplifying
devices intended to add coverage to a cell site
Reradiators are transparent to the host
Wireless system
• A reradiator amplifies RF signals in both
directions, uplink and downlink
• The system does not control reradiators and
has no knowledge of anything they do to the
signals they amplify, on either uplink or
downlink
Careful attention is required when using
reradiators to solve coverage problems
• to achieve the desired coverage
improvement
• to avoid creating interference
• to ensure the active search window is large
enough to accommodate both donor signal
and reradiator signal as seen by mobiles
Reradiators are a
‘“crutch” with
definite application
restrictions. Many
operators prefer not
to use re-radiators at
all. However,
reradiators are a
cost-effective
solution for some
problems.
June, 2011 Page 165Course 601-2-3 (c)2011 Scott Baxter
Consideration Checklist for Reradiators
Must not overdrive Repeater to output levels above max
• Forward link case
• Reverse link case
Repeater gain must not exceed antenna isolation plus safety cushion
• Forward link case
• Reverse link case
Repeater output noise floor must not raise BTS noise floor more than 1 db
Repeater Donor must be dominant, so no other defacto donors appear
Windows of mobile and BTS must span both the BTS-mobile direct signal
and BTS-RR-mobile signal (see separate page and diagrams)
Donor must have sufficient capacity to handle intercepted traffic
Power budgets and levels must take into account maximum carriers
maximum loading situation
General: Don’t allow “foldback” coverage from RR in direction of donor
BTS unless absolutely required by unavoidable situation
• Life is so much better downrange – relatively narrow windows are
adequate
• Wide windows are needed if you get between donor and RR
June, 2011 Page 166Course 601-2-3 (c)2011 Scott Baxter
Wireless Reradiators
Propagation Path Loss Considerations
To solve a coverage problem using a reradiator, path loss and link
budget must be considered
• how much reradiator gain is required?
• how much reradiator output power is required?
• what type of antennas would be best?
• how much antenna isolation is needed?
• how big will the reradiator footprint be?
• how far can the reradiator be from the cell?
• will the reradiator interfere with the cell in other areas?
• What is the propagation delay through the reradiator, in chips?
• Will search windows need to be adjusted for compensation?
Cell
RR
ERP
GainPath Loss
Path Loss (free space??)
Gain
RR
Gain
Line Loss
Signal Level
in target area
(free space
usually applies)
June, 2011 Page 167Course 601-2-3 (c)2011 Scott Baxter
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601602603

  • 1. June, 2011 Page 1Course 601-2-3 (c)2011 Scott Baxter Course 601 Intro to Wireless BDA, DAS, and Repeater Technologies Intro to Wireless BDA, DAS, and Repeater Technologies
  • 2. June, 2011 Page 2Course 601-2-3 (c)2011 Scott Baxter 601 Course Outline Specialized Coverage Expansion Techniques – The Family Tree Explained • Repeaters, Boosters, Cell Enhancers: broadband, narrowband, channelized, high power, frequency translating • Distributed Antenna Systems Bi-Directional Amplifiers: The engine inside most systems • Linearity and Power Output Requirements • The danger of oscillation/feedback • output-input coupling and stability considerations • modern DSP cancellation technologies Examples of common BDA/DAS Applications and Systems • Outdoor operator-licensed repeaters • Indoor One-Operator Systems • passive re-radiators • Frequency-specific, stand-alone solutions (one cellular operator, medical data, etc.) • Neutral Host (Multi Frequency, Multi-Cellular Operator, Local Wireless Systems)
  • 3. June, 2011 Page 3Course 601-2-3 (c)2011 Scott Baxter Specialized Coverage Expansion Techniques – The Family Tree Specialized Coverage Expansion Techniques – The Family Tree
  • 4. The Family Tree of Special RF Distribution Re-radiators (boosters, cell enhancers, repeaters) • Passive – Coax-fed • Active (bi-directional amplifiers, on-frequency) – Coax-fed – Fiber-fed • Active, Frequency-Converting Distributed Antenna Systems • Passive – Coax-fed – Fiber-fed • Active – Cable fed – Fiber fed with active remote nodes • Single User • Community/Co-operative These are just the major branches of the tree – there are many variations June, 2011 Page 4Course 601-2-3 (c)2011 Scott Baxter
  • 5. Cell RR Wireless Reradiators Reradiators (also called “boosters”, “repeaters”, “cell enhancers”) are amplifying devices intended to add coverage to a cell site Reradiators are transparent to the host Wireless system • A reradiator amplifies RF signals in both directions, uplink and downlink • The system does not control reradiators and has no knowledge of anything they do to the signals they amplify, on either uplink or downlink Careful attention is required when using reradiators to solve coverage problems • to achieve the desired coverage improvement • to avoid creating interference • to ensure the active search window is large enough to accommodate both donor signal and reradiator signal as seen by mobiles Reradiators are a ‘“crutch” with definite application restrictions. Many operators prefer not to use re-radiators at all. However, reradiators are a cost-effective solution for some problems. June, 2011 Page 5Course 601-2-3 (c)2011 Scott Baxter
  • 6. Home or Small Office Reradiator Setup Opposing Requirements: • Reradiator must have enough gain to deliver coverage to its whole intended coverage area • But the reradiator transmits on the same frequency it is receiving • To prevent oscillation, the gain of the reradiator must be at least 10 db less than the isolation (loss) between its serving and donor antennas Isolation June, 2011 Page 6Course 601-2-3 (c)2011 Scott Baxter
  • 7. Wilson Electronics Signal Booster Wilson Electronics is probably the best-known consumer-level provider of bidirectional amplifiers for deployment by end-users. Wilson’s early models often oscillated and caused serious interference to wireless systems. • Customers often mounted the antennas close together, producing very low isolation • Wilson’s current products are better protected against oscillation, but non-technical end-users still make bad installation choices June, 2011 Page 7Course 601-2-3 (c)2011 Scott Baxter
  • 8. What is a DAS? A Distributed Antenna System, or DAS, is a network of spatially separated antenna nodes connected to a common source via a transport medium that provides wireless service within a geographic area or structure. 1. Building-wide wireless services (cellular/PCS, 2-way radio, paging) connect to integrated access device (IAD) through either base stations or off-air repeaters 2. IAD combines radio signals for applications and services, filters them and sends them into a single wired backbone or trunk running up the building riser 3. The trunk (typ. 7/8”) distributes service to every floor of building 4. WLAN, building automation, security, etc. are added on floor-by-floor basis via applications portals. Access points are in locked closets on each floor 5. Antenna components, radiating cable, standard cables, and omni and directional antennas branch off the trunk on each floor. June, 2011 Page 8Course 601-2-3 (c)2011 Scott Baxter
  • 9. Types of Distributed Antenna Systems There are several kinds of Distributed Antenna Systems, each with their own characteristics : Passive DAS – where RF signals are combined using passive components such as filters, splitters and couplers. Great for multiple bands and small to medium size locations • no power consumed, just off-air pickup and redistribution Active DAS – RF signals are converted and distributed over fiber. Easy to serve larger installations but more costly since each band and operator must be filtered/amplified/processed individually. Hybrid DAS – combination of active and passive techniques DAS can be employed purely within a large building (In-building DAS) or across a large urban area (Street Level DAS). Street Level DAS can provide a very efficient solution for large urban regeneration projects which require dense coverage. They can also be provided in other busy areas such as Metros, Airports or Railway Stations June, 2011 Page 9Course 601-2-3 (c)2011 Scott Baxter
  • 10. A Cable-Distributed DAS June, 2011 Page 10Course 601-2-3 (c)2011 Scott Baxter
  • 11. Fiber-distributed DAS: Lake Nona, FL Block flow diagram of an actual Neutral-Host DAS serving three wireless operators as well as public-safety systems June, 2011 Page 11Course 601-2-3 (c)2011 Scott Baxter
  • 12. Detailed Functions: Lake Nona, FL Device functional diagram showing hardware detail for Lake Nona DAS June, 2011 Page 12Course 601-2-3 (c)2011 Scott Baxter
  • 13. Equipment List for Lake Nona DAS This list includes the major active RF devices in the Lake Nona DAS, broken out by project June, 2011 Page 13Course 601-2-3 (c)2011 Scott Baxter
  • 14. Elements of an In-Building DAS Installation June, 2011 Page 14Course 601-2-3 (c)2011 Scott Baxter
  • 15. Elements of an Outdoor DAS Installation June, 2011 Page 15Course 601-2-3 (c)2011 Scott Baxter
  • 16. Typical Equipment of Neutral-Host DAS With Operator’s BTSs On-Site June, 2011 Page 16Course 601-2-3 (c)2011 Scott Baxter
  • 17. Passive DAS System June, 2011 Page 17Course 601-2-3 (c)2011 Scott Baxter
  • 18. Off-Air vs. Direct Feed A DAS which connects with outside radio systems through antennas over the air is said to be in the “Off Air” mode A DAS which has actual base stations of outside radio systems located in its equipment rooms, and connects directly to them, is said to operate by “Direct Feed” Off-air operation is certainly less expensive, but the reliability and quality of the connection is affected by possible changes in propagation and interference. • Since an off-air DAS merely uses existing capacity from the wireless networks it carries, this places a practical limit on the amount of total traffic the DAS is able to handle Direct Feed brings more complicated and expensive Base Stations onto the DAS headend premises, but the DAS operator is usually not responsible for their cost. The connection is more reliable and the entire capacity of the base stations is available for use on the DAS system. • Most large DAS systems use Direct Feed mainly because of traffic considerations. June, 2011 Page 18Course 601-2-3 (c)2011 Scott Baxter
  • 19. June, 2011 Page 19Course 601-2-3 (c)2011 Scott Baxter Bi-Directional Amplifiers: The engine inside most systems Bi-Directional Amplifiers: The engine inside most systems
  • 20. Bi-Directional Amplifiers Depending upon the size of the desired coverage and the expected traffic levels, most repeaters and DAS systems use some form of Bi-Directional Amplifiers (BDAs) to boost the signal level in both directions • If the external signals are picked up using antennas aimed at external cellsites, then the system is called “off-air” • If base stations of the external operators are actually placed at the DAS head end and connected directly to DAS equipment, we say the system is “direct feed”. June, 2011 Page 20Course 601-2-3 (c)2011 Scott Baxter
  • 21. Linearity and Power Output Requirements Power output of system amplifiers is determined by the needed coverage and the gains and losses of other system components • A formal link budget is used for design of the system Amplifier linearity is expressed by the following specifications • Third-order intercept • Noise floor • Levels of Intermodulation products June, 2011 Page 21Course 601-2-3 (c)2011 Scott Baxter
  • 22. Avoiding Oscillation and Feedback What is BDA oscillation? Oscillation is when the outside antenna hears the amplified signal from the indoor antenna or the indoor antenna hears the amplified signal from the outside antenna. This event is similar to microphone/speaker feedback in audio. Prior to about 2000, bidirectional amplifiers used automatic sensing to gauge the level of isolation between their input and output signal lines • The amplifiers would automatically reduce their gain to keep it below the point of oscillation Beginning around 2000, several manufacturers began using DSP technology to do RF sensing and automatically inject oppositely-phased RF energy into their input circuitry • This technique can provide roughly an additional 30 db of cancellation • For example, a reradiator with 100 db isolation between its antennas would have been able to use only about 90 db of gain • With the DSP cancellation, at the same 100 db isolation the advanced amplifier is able to operate stably with about 120 db gain June, 2011 Page 22Course 601-2-3 (c)2011 Scott Baxter
  • 23. June, 2011 Page 23Course 601-2-3 (c)2011 Scott Baxter Course 602 Wireless BDA/DAS Application and Design Wireless BDA/DAS Application and Design
  • 24. June, 2011 Page 24Course 601-2-3 (c)2011 Scott Baxter 602 Course Outline Classes of BDA/DAS Devices and Systems Wireless Services and Frequencies Wireless Technologies: Signal Types carried by BDA/DAS Systems Quality Criteria For BDA/DAS Systems Basic BDA/DAS Coverage Requirements In-Building Propagation RF Propagation in BDA/DAS Systems Antennas for BDA/DAS Systems BDA/DAS System Link Budgets System design to satisfy link budget requirements BDA/DAS Equipment Manufacturers and Product Offerings BDA/DAS Installation Techniques and Practices BDA/DAS Example Case Studies
  • 25. June, 2011 Page 25Course 601-2-3 (c)2011 Scott Baxter Classes of BDA/DAS Devices and Systems Classes of BDA/DAS Devices and Systems
  • 26. Experimental 40 km Fiber DAS June, 2011 Page 26Course 601-2-3 (c)2011 Scott Baxter
  • 27. A Unique Kind of DAS Cable Distribution: Using HVAC metal Ducting as Waveguide! Wireless RF Distribution in Buildings using Heating and Ventilation Ducts • http://citeseerx.ist.psu.edu/viewdoc /download?doi=10.1.1.81.368&rep =rep1&type=pdf June, 2011 Page 27Course 601-2-3 (c)2011 Scott Baxter
  • 28. June, 2011 Page 28Course 601-2-3 (c)2011 Scott Baxter Wireless Services and Frequencies Wireless Services and Frequencies
  • 29. June, 2011 Page 29Course 601-2-3 (c)2011 Scott Baxter Frequencies Used by Wireless Systems Overview of the Radio Spectrum 3 4 5 6 7 8 9 10 12 14 16 18 20 22 24 26 28 30 GHz 30,000,000,000 i.e., 3x1010 Hz Broadcasting Land-Mobile Aeronautical Mobile Telephony Terrestrial Microwave Satellite 0.3 0.4 0.5 0/6 0.7 0.8 0.9 1.0 1.2 1.4 1.6 1.8 2.0 2.4 3.0 GHz 3,000,000,000 i.e., 3x109 Hz UHF TV 14-59UHF GPS DCS, PCS, AWS700 + Cellular 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.2 1.4 1.6 1.8 2.0 2.4 3.0 MHz 3,000,000 i.e., 3x106 Hz AM LORAN Marine 3 4 5 6 7 8 9 10 12 14 16 18 20 22 24 26 28 30 MHz 30,000,000 i.e., 3x107 Hz Short Wave -- International Broadcast -- Amateur CB 30 40 50 60 70 80 90 100 120 140 160 180 200 240 300 MHz 300,000,000 i.e., 3x108 Hz FM VHF TV 7-13VHF LOW Band VHFVHF TV 2-6
  • 30. June, 2011 Page 30Course 601-2-3 (c)2011 Scott Baxter Current Wireless Spectrum in the US Modern wireless began in the 800 MHz. range, when the US FCC reallocated UHF TV channels 70-83 for wireless use and AT&T’s Analog technology “AMPS” was chosen. Nextel bought many existing 800 MHz. Enhanced Specialized Mobile Radio (ESMR) systems and converted to Motorola’s “IDEN” technology The FCC allocated 1900 MHz. spectrum for Personal Communications Services, “PCS”, auctioning the frequencies for over $20 billion dollars With the end of Analog TV broadcasting in 2009, the FCC auctioned former TV channels 52-69 for wireless use, “700 MHz.” The FCC also auctioned spectrum near 1700 and 2100 MHz. for Advanced Wireless Services, “AWS”. Technically speaking, any technology can operate in any band. The choice of technology is largely a business decision. 700 MHz 800 900 1700 1800 1900 2000 2100 2200 700 MHz. IDEN IDEN CELLDNLNK CELLUPLINK AWS Uplink AWS Down- Link PCS Uplink PCS Down- Link Proposed AWS-2 AWS? SAT SAT Frequency, MegaHertz
  • 31. June, 2011 Page 31Course 601-2-3 (c)2011 Scott Baxter North American Cellular Spectrum In each MSA and RSA, eligibility for ownership was restricted • “A” licenses awarded to non-telephone-company applicants only • “B” licenses awarded to existing telephone companies only • subsequent sales are unrestricted after system in actual operation Downlink Frequencies (“Forward Path”) Uplink Frequencies (“Reverse Path”) Frequency, MHz824 835 845 870 880 894 869 849 846.5825 890 891.5 Paging, ESMR, etc. A B Ownership and Licensing Frequencies used by “A” Cellular Operator Initial ownership by Non-Wireline companies Frequencies used by “B” Cellular Operator Initial ownership by Wireline companies
  • 32. June, 2011 Page 32Course 601-2-3 (c)2011 Scott Baxter By 1994, US cellular systems were seriously overloaded and looking for capacity relief • The FCC allocated 120 MHz. of spectrum around 1900 MHz. for new wireless telephony known as PCS (Personal Communications Systems), and 20 MHz. for unlicensed services • allocation was divided into 6 blocks; 10-year licenses were auctioned to highest bidders Development of North America PCS 51 MTAs 493 BTAs PCS Licensing and Auction Details • A & B spectrum blocks licensed in 51 MTAs (Major Trading Areas ) • Revenue from auction: $7.2 billion (1995) • C, D, E, F blocks were licensed in 493 BTAs (Basic Trading Areas) • C-block auction revenue: $10.2 B, D-E-F block auction: $2+ B (1996) • Auction winners are free to choose any desired technology A D B E F C unlic. data unlic. voice A D B E F C 1850 MHz. 1910 MHz. 1990 MHz. 1930 MHz. 15 15 155 5 5 15 15 155 5 5 PCS SPECTRUM ALLOCATIONS IN NORTH AMERICA
  • 33. June, 2011 Page 33Course 601-2-3 (c)2011 Scott Baxter The US 700 MHz. Spectrum and Its Blocks To satisfy growing demand for wireless data services as well as traditional voice, the FCC has also taken the spectrum formerly used as TV channels 52-69 and allocated them for wireless The TV broadcasters will completely vacate these frequencies when analog television broadcasting ends in February, 2009 At that time, the winning wireless bidders may begin building and operating their networks In many cases, 700 MHz. spectrum will be used as an extension of existing operators networks. In other cases, entirely new service will be provided.
  • 34. June, 2011 Page 34Course 601-2-3 (c)2011 Scott Baxter Advanced Wireless Services: The AWS Spectrum To further satisfy growing demand for wireless data services as well as traditional voice, the FCC has also allocated more spectrum for wireless in the 1700 and 2100 MHz. ranges The US AWS spectrum lines up with International wireless spectrum allocations, making “world” wireless handsets more practical than in the past Many AWS licensees will simply use their AWS spectrum to add more capacity to their existing networks; some will use it to introduce their service to new areas
  • 35. June, 2011 Page 35Course 601-2-3 (c)2011 Scott Baxter AWS Spectrum Blocks The AWS spectrum is divided into “blocks” Different wireless operator companies are licensed to use specific blocks in specific areas This is the same arrangement used in original 800 MHz. cellular, 1900 MHz. PCS, and the new 700 MHz. allocations
  • 36. June, 2011 Page 36Course 601-2-3 (c)2011 Scott Baxter Wireless Technologies: Signal Types carried by BDA/DAS Wireless Technologies: Signal Types carried by BDA/DAS
  • 37. Characteristics of a Radio Signal The purpose of telecommunications is to send information from one place to another Our civilization exploits the transmissible nature of radio signals, using them in a sense as our “carrier pigeons” To convey information, some characteristic of the radio signal must be altered (I.e., ‘modulated’) to represent the information The sender and receiver must have a consistent understanding of what the variations mean to each other RF signal characteristics which can be varied for information transmission: • Amplitude • Frequency • Phase SIGNAL CHARACTERISTICS S(t) = A cos [ ωc t + ϕ ] The complete, time- varying radio signal Amplitude (strength) of the signal Natural Frequency of the signal Phase of the signal Compare these Signals: Different Amplitudes Different Frequencies Different Phases June, 2011 Page 37Course 601-2-3 (c)2011 Scott Baxter
  • 38. Modulation and Occupied Bandwidth The bandwidth occupied by a signal depends on: • input information bandwidth • modulation method Information to be transmitted, called “input” or “baseband” • bandwidth usually is small, much lower than frequency of carrier Unmodulated carrier • the carrier itself has Zero bandwidth!! AM-modulated carrier • Notice the upper & lower sidebands • total bandwidth = 2 x baseband FM-modulated carrier • Many sidebands! bandwidth is a complex mathematical function PM-modulated carrier • Many sidebands! bandwidth is a complex mathematical function Voltage Time Time-Domain (as viewed on an Oscilloscope) Frequency-Domain (as viewed on a Spectrum Analyzer) Voltage Frequency0 fc fc Upper Sideband Lower Sideband fc fc June, 2011 Page 38Course 601-2-3 (c)2011 Scott Baxter
  • 39. The Emergence of AM: A bit of History The early radio pioneers first used binary transmission, turning their crude transmitters on and off to form the dots and dashes of Morse code. The first successful demonstrations of radio occurred during the mid-1890’s by experimenters in Italy, England, Kentucky, and elsewhere. Amplitude modulation was the first method used to transmit voice over radio. The early experimenters couldn’t foresee other methods (FM, etc.), or today’s advanced digital devices and techniques. Commercial AM broadcasting to the public began in the early 1920’s. Despite its disadvantages and antiquity, AM is still alive: • AM broadcasting continues today in 540-1600 KHz. • AM modulation remains the international civil aviation standard, used by all commercial aircraft (108-132 MHz. band). • AM modulation is used for the visual portion of commercial television signals (sound portion carried by FM modulation) • Citizens Band (“CB”) radios use AM modulation • Special variations of AM featuring single or independent sidebands, with carrier suppressed or attenuated, are used for marine, commercial, military, and amateur communicationsSSBLSB USB June, 2011 Page 39Course 601-2-3 (c)2011 Scott Baxter
  • 40. Frequency Modulation (“FM”) Frequency Modulation (FM) is a type of angle modulation • in FM, the instantaneous frequency of the signal is varied by the modulating waveform Advantages of FM • the amplitude is constant – simple saturated amplifiers can be used – the signal is relatively immune to external noise – the signal is relatively robust; required C/I values are typically 17-18 dB. in wireless applications Disadvantages of FM • relatively complex detectors are required • a large number of sidebands are produced, requiring even larger bandwidth than AM TIME-DOMAIN VIEW sFM(t) =A cos [ωc t + mω m(x)dx+ϕ0 ] t t0 where: A = signal amplitude (constant) ωc = radian carrier frequency mω = frequency deviation index m(x) = modulating signal ϕ0 = initial phase FREQUENCY-DOMAIN VIEW Voltage Frequency0 fc SFM(t) UPPER SIDEBANDS LOWER SIDEBANDS June, 2011 Page 40Course 601-2-3 (c)2011 Scott Baxter
  • 41. The Digital Advantage The modulating signals shown in previous slides were all analog. It is also possible to quantize modulating signals, restricting them to discrete values, and use such signals to perform digital modulation. Digital modulation has several advantages over analog modulation: Digital signals can be more easily regenerated than analog • in analog systems, the effects of noise and distortion are cumulative: each demodulation and remodulation introduces new noise and distortion, added to the noise and distortion from previous demodulations/remodulations. • in digital systems, each demodulation and remodulation produces a clean output signal free of past noise and distortion Digital bit streams are ideally suited to many flexible multiplexing schemes transmission demodulation-remodulation transmission demodulation-remodulation transmission demodulation-remodulation June, 2011 Page 41Course 601-2-3 (c)2011 Scott Baxter
  • 42. Theory of Digital Modulation: Sampling Voice and other analog signals first must be sampled (converted to digital form) for digital modulation and transmission The sampling theorem gives the criteria necessary for successful sampling, digital modulation, and demodulation • The analog signal must be band- limited (low-pass filtered) to contain no frequencies higher than fM • Sampling must occur at least twice as fast as fM in the analog signal. This is called the Nyquist Rate Required Bandwidth for p(t) • If each sample p(t) is expressed as an n-bit binary number, the bandwidth required to convey p(t) as a digital signal is at least N*2* fM • this follows Shannon’s Theorem: at least one Hertz of bandwidth is required to convey one bit per second of data The Sampling Theorem: Two Parts •If the signal contains no frequency higher than fM Hz., it is comletely described by specifying its samples taken at instants of time spaced 1/2 fM s. •The signal can be completely recovered from its samples taken at the rate of 2 fM samples per second or higher. m(t) Sampling Recovery m(t) p(t) June, 2011 Page 42Course 601-2-3 (c)2011 Scott Baxter
  • 43. Sampling Example: the 64 kb/s DS-0 Telephony has adopted a world-wide PCM standard digital signal employing a 64 kb/s stream derived from sampled voice data Voice waveforms are band-limited • upper cutoff between 3500-4000 Hz. to avoid aliasing • rolloff below 300 Hz. to minimize vulnerability to “hum” from AC power mains Voice waveforms sampled at 8000/second rate • 8000 samples x 1 byte = 64,000 bits/second • A>D conversion is non-linear, one byte per sample, thus 256 quantized levels are possible • Levels are defined logarithmically rather than linearly to accommodate a wider range of audio levels with minimum distortion – µ-law companding (popular in North America & Japan) – A-law companding (used in most other countries) A>D and D>A functions are performed in a CODEC (coder-decoder) (see following figure) -10dB -20dB -30dB -40dB 0 dB 100 300 1000 3000 10000 Frequency, Hz C-Message Weighting t 0 1 2 3 4 5 6 87 910 11 12 13 14 15 16 4 16 1 3 15 8 3 4 8 A-LAW y= sgn(x) A|x| ln(1+ A) for 0≤ x≤ 1 A (where A = 87.6) y= sgn(x) ln(1+ A|x)| ln(1+ A) for 1 A < x ≤1 µ-Law y = sgn(x) ln(1+ µ|x|) ln(1 + µ) (whereµ = 255) Companding Band-Limiting x = analog audio voltage y = quantized level (digital) June, 2011 Page 43Course 601-2-3 (c)2011 Scott Baxter
  • 44. Digital ModulationDigital Modulation June, 2011 Page 44Course 601-2-3 (c)2011 Scott Baxter
  • 45. Modulation by Digital Inputs For example, modulate a signal with this digital waveform. No more continuous analog variations, now we’re “shifting” between discrete levels. We call this “shift keying”. • The user gets to decide what levels mean “0” and “1” -- there are no inherent values Steady Carrier without modulation Amplitude Shift Keying ASK applications: digital microwave Frequency Shift Keying FSK applications: control messages in AMPS cellular; TDMA cellular Phase Shift Keying PSK applications: TDMA cellular, GSM & PCS-1900 Our previous modulation examples used continuously-variable analog inputs. If we quantize the inputs, restricting them to digital values, we will produce digital modulation. Voltage Time 1 0 1 0 1 0 1 0 1 0 1 0 1 0 1 0 June, 2011 Page 45Course 601-2-3 (c)2011 Scott Baxter
  • 46. Claude Shannon: The “Einstein” of Information Theory and Signal Science The core idea that makes CDMA possible was first explained by Claude Shannon, a Bell Labs research mathematician Shannon's work relates amount of information carried, channel bandwidth, signal-to-noise-ratio, and detection error probability • It shows the theoretical upper limit attainable In 1948 Claude Shannon published his landmark paper on information theory, A Mathematical Theory of Communication. He observed that "the fundamental problem of communication is that of reproducing at one point either exactly or approximately a message selected at another point." His paper so clearly established the foundations of information theory that his framework and terminology are standard today. Shannon died Feb. 24, 2001, at age 84. June, 2011 Page 46Course 601-2-3 (c)2011 Scott Baxter
  • 47. Modulation Techniques of 1xEV Technologies 1xEV, “1x Evolution”, is a family of alternative fast-data schemes that can be implemented on a 1x CDMA carrier. 1xEV DO means “1x Evolution, Data Only”, originally proposed by Qualcomm as “High Data Rates” (HDR). • Up to 2.4576 Mbps forward, 153.6 kbps reverse • A 1xEV DO carrier holds only packet data, and does not support circuit-switched voice • Commercially available in 2003 1xEV DV means “1x Evolution, Data and Voice”. • Max throughput of 5 Mbps forward, 307.2k reverse • Backward compatible with IS-95/1xRTT voice calls on the same carrier as the data • Not yet commercially available; work continues All versions of 1xEV use advanced modulation techniques to achieve high throughputs. QPSK CDMA IS-95, IS-2000 1xRTT, and lower rates of 1xEV-DO, DV 16QAM 1xEV-DO at highest rates 64QAM 1xEV-DV at highest rates June, 2011 Page 47Course 601-2-3 (c)2011 Scott Baxter
  • 48. Digital Modulation Systems Each symbol of a digitally modulated RF signal conveys a number of bits of information • determined by the number of degrees of modulation freedom More complex modulation schemes can carry more bits per symbol in a given bandwidth, but require better signal-to-noise ratios The actual number of bits per second which can be conveyed in a given bandwidth under given signal-to-noise conditions is described by Shannon’s equations Modulation Scheme Shannon Limit, BitsHz BPSK 1 b/s/hz QPSK 2 b/s/hz 8PSK 3 b/s/hz 16 QAM 4 b/s/hz 32 QAM 5 b/s/hz 64 QAM 6 b/s/hz 256 QAM 8 b/s/hz SHANNON’S CAPACITY EQUATION C = Bω log2 [ 1 + ]S N Bω = bandwidth in Hertz C = channel capacity in bits/second S = signal power N = noise power June, 2011 Page 48Course 601-2-3 (c)2011 Scott Baxter
  • 49. Digital Modulation Schemes There are many different schemes for digital modulation, each a compromise between complexity, immunity to errors in transmission, required channel bandwidth, and possible requirement for linear amplifiers Linear Modulation Techniques • BPSK Binary Phase Shift Keying • DPSK Differential Phase Shift Keying • QPSK Quadrature Phase Shift Keying IS-95 CDMA forward link – Offset QPSK IS-95 CDMA reverse link – Pi/4 DQPSK IS-54, IS-136 control and traffic channels Constant Envelope Modulation Schemes • BFSK Binary Frequency Shift Keying AMPS control channels • MSK Minimum Shift Keying • GMSK Gaussian Minimum Shift Keying GSM systems, CDPD Hybrid Combinations of Linear and Constant Envelope Modulation • MPSK M-ary Phase Shift Keying • QAM M-ary Quadrature Amplitude Modulation • MFSK M-ary Frequency Shift Keying FLEX paging protocol Spread Spectrum Multiple Access Techniques • DSSS Direct-Sequence Spread Spectrum IS-95 CDMA • FHSS Frequency-Hopping Spread Spectrum June, 2011 Page 49Course 601-2-3 (c)2011 Scott Baxter
  • 50. Error Vulnerabilities of Higher-Order Modulation Schemes Higher-Order Modulation Schemes (16PSK, 32QAM, 64QAM...) are more vulnerable to transmission errors than the simpler, more rugged schemes (BPSK, QPSK) • Closely-packed constellations leave little room for vector error Non-linearities (gain compression, clipping, reflections within antenna system) “warp” the constellation Noise and long-delayed echoes cause “scatter” around constellation points Interference blurs constellation points into “rings” of error Q I Normal 64QAM Q I Distortion (Gain Compression) Q I Noise Q I Interference June, 2011 Page 50Course 601-2-3 (c)2011 Scott Baxter
  • 51. Error Vector Magnitude and ρ (“Rho”) A common measurement of overall error is Error Vector Magnitude “EVM” • usually a small fraction of total vector amplitude, ~0.1 EVM is usually averaged over a large number of symbols • Root-mean-square (RMS) Commercial test equipment for BTS maintenance measures EVM Signal quality is often expressed as 1-EVM • normally called ρ (“Rho”) • typically 0.89-0.96 June, 2011 Page 51Course 601-2-3 (c)2011 Scott Baxter
  • 52. Modulation used in IS-95 CDMA Systems CDMA mobiles use offset QPSK modulation • the Q-sequence is delayed half a chip, so that I and Q never change simultaneously and the mobile TX never passes through (0,0) CDMA base stations use QPSK modulation • every signal (voice, pilot, sync, paging) has its own amplitude, so the transmitter is unavoidably going through (0,0) sometimes; no reason to include 1/2 chip delay Base Stations: QPSK Q Axis I Axis Short PN Q Σ cos ωt sin ωt User’s chips Short PN I Mobiles: OQPSK Q Axis I Axis Short PN Q Σ cos ωt sin ωt User’s chips 1/2 chip Short PN I June, 2011 Page 52Course 601-2-3 (c)2011 Scott Baxter
  • 53. CDMA Base Station Modulation Views The view at top right shows the actual measured QPSK phase constellation of a CDMA base station in normal service The view at bottom right shows the measured power in the code domain for each walsh code on a CDMA BTS in actual service • Notice that not all walsh codes are active • Pilot, Sync, Paging, and certain traffic channels are in use June, 2011 Page 53Course 601-2-3 (c)2011 Scott Baxter
  • 54. June, 2011 Page 54Course 601-2-3 (c)2011 Scott Baxter
  • 55. June, 2011 Page 55Course 601-2-3 (c)2011 Scott Baxter Multiple Access Methods Frequency Time Power TDMA Frequency Time Power FDMA Frequency Time Power CDMA CODE FDMA: AMPS & NAMPS •Each user occupies a private Frequency, protected from interference through physical separation from other users on the same frequency TDMA: IS-136, GSM •Each user occupies a specific frequency but only during an assigned time slot. The frequency is used by other users during other time slots. CDMA •Each user uses a signal on a particular frequency at the same time as many other users, but it can be separated out when receiving because it contains a special code of its own
  • 56. June, 2011 Page 56Course 601-2-3 (c)2011 Scott Baxter Multiple Access Methods MIMO OFDM OFDM, OFDMA •Orthogonal Frequency Division Multiplexing; Orthogonal Frequency Division Muliple Access •The signal consists of many (from dozens to thousands) of thin carriers carrying symbols •In OFDMA, the symbols are for multiple users •OFDM provides dense spectral efficiency and robust resistance to fading, with great flexibility of use MIMO •Multiple Input Multiple Output •An ideal companion to OFDM, MIMO allows exploitation of multiple antennas at the base station and the mobile to effectively multiply the throughput for the base station and users Frequency Tim e Power
  • 57. June, 2011 Page 57Course 601-2-3 (c)2011 Scott Baxter Quality Criteria For BDA/DAS Systems Quality Criteria For BDA/DAS Systems
  • 58. Signal Quality Criteria C/I Carrier-to-Interference • Ratio of power of desired signal to power of undesired signals in the background S/N Signal-to-Noise Ratio • Ratio of power of desired signal to the noise in the background Linearity • Purity of the signal. Typically expressed as Rho or Error Vector Magnitude. • Typical specification: Rho >= 0.9, or EVM <0.1 Amplitude “tilt” over frequency • Variable frequency response causing some parts of the signal to be amplified more than others, distorting the waveform Intersymbol Interference (ISI) • The process of a 1 or 0 in the signal getting overlapped with adjoining 1’s or 0’s, potentially causing incorrect decoding • ISI can be caused by distortion in equipment and by external interference June, 2011 Page 58Course 601-2-3 (c)2011 Scott Baxter
  • 59. Phase Constellation ‘Argand’ Diagram If a transmitter were perfect, it would transmit exactly the proper strength and phase and the diagram at right would have only clean little dots. Real transmitters have variable phase and amplitude errors and instead of precise dots, the diagram at right looks like a paintball target. If the error is large enough, the dots will splatter enough to cause mistakes in the decoding process. June, 2011 Page 59Course 601-2-3 (c)2011 Scott Baxter
  • 60. Spectrum Display showing Noise Floor On this spectrum analyzer, the noise floor is below the specified maximum. If the amplifier were nonlinear, or there were corroded connections involved, locally-generated noise would drive the noise floor up above spec and potentially interfere with other communications. June, 2011 Page 60Course 601-2-3 (c)2011 Scott Baxter
  • 61. Working in DecibelsWorking in Decibels June, 2011 Page 61Course 601-2-3 (c)2011 Scott Baxter
  • 62. Decibels (DB) Calculations of transmitted and received power on radio links and many other electronic circuits always encounters very large and very small numbers • Multiplying and dividing these numbers is tedious Fortunately, there is a simpler way to perform the needed calculations: a logarithmic system which expresses the powers, gains and losses of the circuits in units called decibels (db) Decibels offer two big advantages over straight arithmetic: • in decibels, the numbers are never very large or small • working in arithmetic, power calculations always involve multiplying. Working in decibels, only addition or subtraction are needed. Working in decibels • can be performed using a calculator, or • by remembering two or three key values in a table and knowing how to apply them June, 2011 Page 62Course 601-2-3 (c)2011 Scott Baxter
  • 63. Using Decibels In manual calculation of RF power levels, unwieldy large and small numbers occur as a product of painful multiplication and division. It is popular and much easier to work in Decibels (dB). • rather than multiply and divide RF power ratios, in dB we can just add & subtract Decibel Examples Number N dB 1,000,000,000 +90 100,000,000 +80 10,000,000 +70 1,000,000 +60 100,000 +50 10,000 +40 1,000 +30 100 +20 10 +10 4 +6 2 +3 1 0 0.5 -3 0.25 -6 0.1 -10 0.01 -20 0.001 -30 0.0001 -40 0.00001 -50 0.000001 -60 0.0000001 -70 0.00000001 -80 0.000000001 -90 db = 10 * Log ( X ) Ratio to Decibels X = 10 (db/10) Decibels to Ratio June, 2011 Page 63Course 601-2-3 (c)2011 Scott Baxter
  • 64. Example Link Budget, NOT Using DB Let’s track the power flow from transmitter to receiver in a radio link. We’re going to use typical values that commonly occur in real links. Receiver Antenna Antenna Trans. Line Transmitter Trans. Line 20 Watts TX output x 0.50 line efficiency = 10 watts to antenna x 20 antenna gain = 200 watts ERP x 0.000,000,000,000,000,1585 path attenuation = 0.000,000,000,000,031,7 watts if intercepted by dipole antenna x 20 antenna gain = 0.000,000,000,000,634 watts into line x 0.50 line efficiency = 0.000,000,000,000,317 watts to receiver Did you enjoy that arithmetic? (No!) Let’s go back and do it a better and less painful way. Why Use Decibels? For convenience and speed. Here’s an example of why, then we’ll see how. June, 2011 Page 64Course 601-2-3 (c)2011 Scott Baxter
  • 65. Example Link Budget Using DB Let’s track the power flow again, using decibels. Receiver Antenna Antenna Trans. Line Transmitter Trans. Line +43 dBm TX output -3 dB line efficiency = +40 dBm to antenna +13 dB antenna gain = +53 dBm ERP -158 dB path attenuation = -105 dBm if intercepted by dipole antenna +13 dB antenna gain = -92 dBm into line -3 dB line efficiency = -95 dBm to receiver Wasn’t that better?! How to do it -- next. June, 2011 Page 65Course 601-2-3 (c)2011 Scott Baxter
  • 66. Decibels - Relative and Absolute Decibels normally refer to power ratios -- in other words, the numbers we represent in dB usually are a ratio of two powers. Examples: • A certain amplifier amplifies its input by a factor of 1,000. (Pout/Pin = 1,000). That amplifier has 30 dB gain. • A certain transmission line has an efficiency of only 10 percent. (Pout/Pin = 0.1) The transmission line has a loss of -10 dB. Often decibels are used to express an absolute number of watts, milliwatts, kilowatts, etc.... When used this way, we always append a letter (W, m, or K) after “db” to show the unit we’re using. For example, • 20 dBK = 50 dBW = 80 dBm = 100,000 watts • 0 dBm = 1 milliwatt 1 watt.001 w x 1000 0 dBm 30 dBm +30 dB 100 w +50 dBm x 0.10 -10 dB 10 w +40 dBm June, 2011 Page 66Course 601-2-3 (c)2011 Scott Baxter
  • 67. Decibels Two Other Popular Absolute References dBrnc: a common telephone noise measurement • “db above reference noise, C-weighted” • “Reference Noise” is 1000 Hz. tone at -90 dBm • “C-weighting”, an arbitrary frequency response, matches the response best suited for intelligible toll quality speech • this standard measures through a “C-message” filter dBu: a common electric field strength expression • dBu is “shorthand” for dBµV/m • “decibels above one microvolt per meter field strength” • often we must convert between E-field strength in dBu and the power recovered by a dipole antenna bathed in such a field strength: FSdBu = 20 * Log10(FMHZ) + 75 + PwrDBM PwrDBM = FSdBu - 20 * Log10(FMHZ)-75 -10dB -20dB -30dB -40dB 0 dB 100 300 1000 3000 10000 Frequency, Hz C-Message Weighting Electro- magnetic Field dBµV/m @ FMHZ Dipole Antenna Pwr dBm June, 2011 Page 67Course 601-2-3 (c)2011 Scott Baxter
  • 68. Decibels referring to Voltage or Current By convention, decibels are based on power ratios. However, decibels are occasionally used to express to voltage or current ratios. When doing this, be sure to use these alternate formulas: db = 20 x Log10 (V or I) (V or I) = 10 ^ (db/20) • Example: a signal of 4 volts is 6 db. greater than a signal of 2 volts db = 20 x Log10 (4/2) = 20 x Log10 (2) = 20 x 0.3 = 6.0 db June, 2011 Page 68Course 601-2-3 (c)2011 Scott Baxter
  • 69. Prefixes for Large and Small Units Large and small quantities pop up all over telecommunications and the world in general. We like to work in units we can easily handle, both in math and in concept. So, when large or small numbers arise, we often use prefixes to scale them into something more comfortable: • Kilometers • Megahertz • Milliwatts – etc.... Summary of Units Number N x10y Prefix 1,000,000,000,000 x1012 Tera 1,000,000,000 x109 Giga- 1,000,000 x106 Mega- 1,000 x103 Kilo- 100 x102 hecto- 10 x101 deca- 1 x100 0.1 x10-1 deci- 0.01 x10-2 centi- 0.001 x10-3 milli- 0.000001 x10-6 micro- 0.000000001 x10-9 nano- 0.000000000001 x10-12 pico- 0.000000000000001 x10-15 femto- June, 2011 Page 69Course 601-2-3 (c)2011 Scott Baxter
  • 70. June, 2011 Page 70Course 601-2-3 (c)2011 Scott Baxter Basic BDA/DAS Coverage Requirements Basic BDA/DAS Coverage Requirements
  • 71. Coverage Tradeoffs After the desired coverage area is known, the next step is to determine how many antennas will be required to serve it Alternatives will be available for antennas of different gains and transmitters of different power outputs In general, the solution with the maximum number of antennas will have the fewest significant coverage holes June, 2011 Page 71Course 601-2-3 (c)2011 Scott Baxter
  • 72. A Resource for Indoor Radio Planning A new version of the bestseller, updated with an introduction to LTE and treatments of modulation principle, DAS systems for MIMO/LTE , designing repeater systems and elevator coverage Addresses the challenge of providing coverage inside train, and high speed rail Outlines the key parameters and metrics for designing DAS for GSM, DCS, UMTS, HSPA & LTE Essential reading for engineering and planning personnel at mobile operators, also giving a sound grounding in indoor radio planning for equipment manufacturers Written by a leading practitioner in the field with more than 20 years of practical experience June, 2011 Page 72Course 601-2-3 (c)2011 Scott Baxter
  • 73. Radio PropagationRadio Propagation June, 2011 Page 73Course 601-2-3 (c)2011 Scott Baxter
  • 74. Some Physics: Wavelength of the Signal and Its Influence on Propagation Radio signals in the atmosphere travel at the speed of light λ = wavelength C = distance traveled in 1 second F = frequency, Hertz The wavelength of a radio signal determines many of its propagation characteristics • Internal antenna elements’ size are typically in the order of 1/4 to 1/2 wavelength • Objects bigger than a wavelength can reflect or obstruct RF energy • RF energy can penetrate into a building or vehicle if it has openings the size of a wavelength, or larger λ = C / F Frequency, GHz. Wavelength cm. in. 0.92 32.6 12.8 2.4 12.5 4.9 5.8 5.2 2.0 λ/2 June, 2011 Page 74Course 601-2-3 (c)2011 Scott Baxter
  • 75. Propagation: Getting the Signal to the Customer “Propagation” is the name for the general process of getting a radio signal from one place to another During propagation, the signal gets weaker because of several natural processes. This weakening is called “attenuation”. Point-to-point radio links work best when there is “line-of-sight” between the two antennas. This is the condition of least attenuation • nothing along the way to block the signal AP SM June, 2011 Page 75Course 601-2-3 (c)2011 Scott Baxter
  • 76. The First Fresnel Zone and Free-Space Propagation Most of the signal power sent from one antenna to another travels in an elliptical, “football” shape called the First Fresnel zone. • the thickness of the zone depends on the signal frequency If the First Fresnel zone is free of penetration or obstruction by any objects, we say “free-space” conditions apply • this is the desirable condition providing highest received signal strength Sometimes obstructions are unavoidable, and penetrate the first fresnel zone • this attenuates the signal and reduces the signal strength received at the other end of the link • the amount of attenuation depends on the degree of penetration by the obstruction, and its absorbing characteristics Frequency, GHz. Path, Miles Mid-Pt Fresnel R, ft 0.92 10 119 2.4 10 74 5.8 10 47 AP SM June, 2011 Page 76Course 601-2-3 (c)2011 Scott Baxter
  • 77. Free-Space Propagation Technical Details The simplest propagation mode • Antenna radiates energy which spreads in space • Path Loss, db (between two isotropic antennas) = 36.58 +20*Log10(FMHZ)+20Log10(DistMILES ) • Path Loss, db (between two dipole antennas) = 32.26 +20*Log10(FMHZ)+20Log10(DistMILES ) • Notice the rate of signal decay: • 6 db per octave of distance change, which is 20 db per decade of distance change Free-Space propagation is applicable if: • there is only one signal path (no reflections) • the path is unobstructed (i.e., first Fresnel zone is not penetrated by obstacles) First Fresnel Zone = {Points P where AP + PB - AB < λ/2 } Fresnel Zone radius d = 1/2 (λD)^(1/2) 1st Fresnel Zone B A d D Free Space “Spreading” Loss energy intercepted by receiving antenna is proportional to 1/r2 r June, 2011 Page 77Course 601-2-3 (c)2011 Scott Baxter
  • 78. Obstructions and their Effects When an obstruction penetrates the first fresnel zone, the signal is attenuated. The degree of attenuation depends on • how much of the first fresnel zone is obstructed • the absorptive characteristics of the obstructing object(s) • whether the signal is also reflecting off of other nearby objects, possibly providing a degree of “fill-in” Depending on the length of the path, the transmitter power, and the receiver sensitivity, the link may still work despite the obstruction AP SM June, 2011 Page 78Course 601-2-3 (c)2011 Scott Baxter
  • 79. Severe Obstructions When the path is blocked by a major obstruction (large hill, downtown building, etc.) there will be substantial signal attenuation Even under this undesirable condition, if the distance is small there may be enough signal to make the link usable • A very small amount of the signal will actually diffract (“bend”) over the obstruction • the extra attenuation caused by the obstruction can be calculated by the “knife edge diffraction” model • this “diffraction loss” can be considered in the link budget to see the link is likely to be usable anyway AP SM June, 2011 Page 79Course 601-2-3 (c)2011 Scott Baxter
  • 80. Knife-Edge Diffraction Sometimes a single well-defined obstruction blocks the path, introducing additional loss. This calculation is fairly easy and can be used as a manual tool to estimate the effects of individual obstructions. First calculate the diffraction parameter ν from the geometry of the path Next consult the table to obtain the obstruction loss in db Add this loss to the otherwise- determined path loss to obtain the total path loss. Other losses such as free space and reflection cancellation still apply, but computed independently for the path as if the obstruction did not exist H R1 R2 ν atten dB 0 -5 -10 -15 -20 -25 -4 -3 -2 -1 0 1 2 3-5 ( + )ν = -H 2 λ 1 1 R1 R2 June, 2011 Page 80Course 601-2-3 (c)2011 Scott Baxter
  • 81. Foliage and Building Penetration Considerations At broadband wireless frequencies, the penetration loss entering a building often exceeds 35 db. • this restricts range so greatly that antennas are almost never located inside a building At broadband wireless frequencies, trees and other vegetation effectively block and absorb the signal • typical attenuation for just one mature tree can be 20 db or more Unfortunately, neither building nor vegetation loss can be predicted accurately. Measurement is the only way to know accurately what is happening. Building SM AP Building SM AP June, 2011 Page 81Course 601-2-3 (c)2011 Scott Baxter
  • 82. June, 2011 Page 82Course 601-2-3 (c)2011 Scott Baxter In-Building PropagationIn-Building Propagation
  • 83. iBWAVE: Common Commercial Software for Indoor Propagation Prediction AWE Communications offers iBWAVE, a commercial indoor propagation prediction and design tool. This tool is a good example of the current state of the art. Large database of building material characteristics Import walls/floorplans from AutoCAD, images or PDF files. Propagation module offers dominant path and COST 321 multi-wall models. • accurate propagation results from antennas and radiating cables • can increase accuracy by calibrating the prediction model with survey data The Propagation module provides output maps giving a visual representation of propagation results, even for different technologies and different bands. • These include signal strength, field strength, best server and soft handoff maps. • evaluate different design configurations and instantly get a clear picture of the impact on coverage and cost. • The Propagation module delivers professional documentation about the project for effective communication with customers to facilitate agreements and approvals. June, 2011 Page 83Course 601-2-3 (c)2011 Scott Baxter
  • 84. iBWAVE Examples June, 2011 Page 84Course 601-2-3 (c)2011 Scott Baxter
  • 85. iBWAVE Images June, 2011 Page 85Course 601-2-3 (c)2011 Scott Baxter
  • 86. iBWAVE Coverage Map June, 2011 Page 86Course 601-2-3 (c)2011 Scott Baxter
  • 87. Equipment List June, 2011 Page 87Course 601-2-3 (c)2011 Scott Baxter
  • 88. iBwave Documentation iBwave also provides documentation capabilities • Very useful in large projects June, 2011 Page 88Course 601-2-3 (c)2011 Scott Baxter
  • 89. iBwave System Detail Diagram June, 2011 Page 89Course 601-2-3 (c)2011 Scott Baxter
  • 90. Stadium Example Example of stadium detail and calculation of signal levels on each element June, 2011 Page 90Course 601-2-3 (c)2011 Scott Baxter
  • 91. Network Diagram on Floor Plan June, 2011 Page 91Course 601-2-3 (c)2011 Scott Baxter
  • 92. Network Diagram on Detailed Floor Plan June, 2011 Page 92Course 601-2-3 (c)2011 Scott Baxter
  • 93. Signal Strength on Floor Plan June, 2011 Page 93Course 601-2-3 (c)2011 Scott Baxter
  • 94. iBwave Configuration and Display Examples June, 2011 Page 94Course 601-2-3 (c)2011 Scott Baxter
  • 95. 3-story DAS components June, 2011 Page 95Course 601-2-3 (c)2011 Scott Baxter
  • 96. Equipment Room of Neutral Host System June, 2011 Page 96Course 601-2-3 (c)2011 Scott Baxter
  • 97. June, 2011 Page 97Course 601-2-3 (c)2011 Scott Baxter
  • 98. Indoor Best Server Plot Example Indoor best server plot computed by iBWAVE June, 2011 Page 98Course 601-2-3 (c)2011 Scott Baxter
  • 99. June, 2011 Page 99Course 601-2-3 (c)2011 Scott Baxter RF Propagation in BDA/DAS Systems RF Propagation in BDA/DAS Systems
  • 100. June, 2011 Page 100Course 601-2-3 (c)2011 Scott Baxter Antennas for BDA/DAS SystemsAntennas for BDA/DAS Systems
  • 101. Understanding Antenna Radiation The Principle Of Current Moments An antenna is just a passive conductor carrying RF current • RF power causes the current flow • Current flowing radiates electromagnetic fields • Electromagnetic fields cause current in receiving antennas The effect of the total antenna is the sum of what every tiny “slice” of the antenna is doing • Radiation of a tiny “slice” is proportional to its length times the magnitude of the current in it, at the phase of the current TX RX Width of band denotes current magnitude Zero current at each end Maximum current at the middle Current induced in receiving antenna is vector sum of contribution of every tiny “slice” of radiating antenna each tiny imaginary “slice” of the antenna does its share of radiating June, 2011 Page 101Course 601-2-3 (c)2011 Scott Baxter
  • 102. Antenna Gain Antennas are passive devices: they do not produce power • Can only receive power in one form and pass it on in another, minus incidental losses • Cannot generate power or “amplify” However, an antenna can appear to have “gain” compared against another antenna or condition. This gain can be expressed in dB or as a power ratio. It applies both to radiating and receiving A directional antenna, in its direction of maximum radiation, appears to have “gain” compared against a non-directional antenna Gain in one direction comes at the expense of less radiation in other directions Antenna Gain is RELATIVE, not ABSOLUTE • When describing antenna “gain”, the comparison condition must be stated or implied Omni-directional Antenna Directional Antenna June, 2011 Page 102Course 601-2-3 (c)2011 Scott Baxter
  • 103. Reference Antennas Defining Gain And Effective Radiated Power Isotropic Radiator • Truly non-directional -- in 3 dimensions • Difficult to build or approximate physically, but mathematically very simple to describe • A popular reference: 1000 MHz and above – PCS, microwave, etc. Dipole Antenna • Non-directional in 2-dimensional plane only • Can be easily constructed, physically practical • A popular reference: below 1000 MHz – 800 MHz. cellular, land mobile, TV & FM Isotropic Antenna (watts or dBm) ERPEffective Radiated Power Vs. Dipole Effective Radiated Power Vs. Isotropic Gain above Dipole reference Gain above Isotropic radiator (watts or dBm) EIRP dBd dBi Quantity Units Dipole Antenna Notice that a dipole has 2.15 dB gain compared to an isotropic antenna. June, 2011 Page 103Course 601-2-3 (c)2011 Scott Baxter
  • 104. Radiation Patterns Key Features And Terminology An antenna’s directivity is expressed as a series of patterns The Horizontal Plane Pattern graphs the radiation as a function of azimuth (i.e..,direction N-E-S-W) The Vertical Plane Pattern graphs the radiation as a function of elevation (i.e.., up, down, horizontal) Antennas are often compared by noting specific landmark points on their patterns: • -3 dB (“HPBW”), -6 dB, -10 dB points • Front-to-back ratio • Angles of nulls, minor lobes, etc. Typical Example Horizontal Plane Pattern 0 (N) 90 (E) 180 (S) 270 (W) 0 -10 -20 -30 dB Notice -3 dB points Front-to-back Ratio 10 dB points Main Lobe a Minor Lobe nulls or minim June, 2011 Page 104Course 601-2-3 (c)2011 Scott Baxter
  • 105. In phase Out of phase How Antennas Achieve Their Gain Quasi-Optical Techniques (reflection, focusing) • Reflectors can be used to concentrate radiation – technique works best at microwave frequencies, where reflectors are small • Examples: – corner reflector used at cellular or higher frequencies – parabolic reflector used at microwave frequencies – grid or single pipe reflector for cellular Array techniques (discrete elements) • Power is fed or coupled to multiple antenna elements; each element radiates • Elements’ radiation in phase in some directions • In other directions, a phase delay for each element creates pattern lobes and nulls June, 2011 Page 105Course 601-2-3 (c)2011 Scott Baxter
  • 106. Types Of Arrays Collinear vertical arrays • Essentially omnidirectional in horizontal plane • Power gain approximately equal to the number of elements • Nulls exist in vertical pattern, unless deliberately filled Arrays in horizontal plane • Directional in horizontal plane: useful for sectorization • Yagi – one driven element, parasitic coupling to others • Log-periodic – all elements driven – wide bandwidth All of these types of antennas are used in wireless RF power RF power June, 2011 Page 106Course 601-2-3 (c)2011 Scott Baxter
  • 107. Omni Antennas Collinear Vertical Arrays The family of omni-directional wireless antennas: Number of elements determines • Physical size • Gain • Beamwidth, first null angle Models with many elements have very narrow beamwidths • Require stable mounting and careful alignment • Watch out: be sure nulls do not fall in important coverage areas Rod and grid reflectors are sometimes added for mild directivity Examples: 800 MHz.: dB803, PD10017, BCR-10O, Kathrein 740-198 1900 MHz.: dB-910, ASPP2933 beamwidth Angle of first null θ -3 d B Vertical Plane Pattern Number of Elements Power Gain Gain, dB Angle θ 0.00 n/a 3.01 26.57° 4.77 18.43° 6.02 14.04° 6.99 11.31° 7.78 9.46° 8.45 8.13° 9.03 7.13° 9.54 6.34° 10.00 5.71° 10.41 5.19° 10.79 4.76° 11.14 4.40° 1 2 3 4 5 6 7 8 9 10 11 12 13 14 1 2 3 4 5 6 7 8 9 10 11 12 13 14 11.46 4.09° Typical Collinear Arrays June, 2011 Page 107Course 601-2-3 (c)2011 Scott Baxter
  • 108. Sector Antennas Reflectors And Vertical Arrays Typical commercial sector antennas are vertical combinations of dipoles, yagis, or log-periodic elements with reflector (panel or grid) backing • Vertical plane pattern is determined by number of vertically-separated elements – varies from 1 to 8, affecting mainly gain and vertical plane beamwidth • Horizontal plane pattern is determined by: – number of horizontally-spaced elements – shape of reflectors (is reflector folded?) Vertical Plane Pattern Up Down Horizontal Plane Pattern N E S W June, 2011 Page 108Course 601-2-3 (c)2011 Scott Baxter
  • 109. Pattern of Canopy AP Internal Patch Antenna June, 2011 Page 109Course 601-2-3 (c)2011 Scott Baxter
  • 110. Andrew Radiax June, 2011 Page 110Course 601-2-3 (c)2011 Scott Baxter
  • 111. Radiax Design Considerations System Architecture for a specific application will depend on overall objectives • dictated in large part by the geometry and area that is required for coverage. • For tunnel applications, the length, construction, and the size of the tunnel will establish the basic parameters. • Other key factors include the number of services, providers, and channels required to meet the objectives. For tunnel applications, the two primary architectures used are: • A series of cascaded amplifiers or • Using a T-feed configuration. In some implementations, it is smart to use a combination of these two techniques. • The T-feed structure is appropriate when feeding from multiple base stations or when using amplifiers that are connected to a common base station using fiber • The T-feed structure has the advantage that an amplifier can drive a longer length of cable than can be achieved with the cascaded architecture. • The T-feed structure generates less downlink intermodulation since the amplifiers are not cascaded. • The cascaded configuration has a higher dynamic range on the uplink and is useful for communication systems that do not use uplink power control. • The cascade configuration has been used effectively on tunnels where the communication system employs conventional or trunk radio techniques. • The T-feed configuration has been particularly well suited for cellular and PCS applications. June, 2011 Page 111Course 601-2-3 (c)2011 Scott Baxter
  • 112. Radiax Applications Cable Parameters • Insertion Loss • Coupling Loss • Fading Characteristic • Coherent Bandwidth • Launch Angle Insertion Loss • a measure of the attenuation in the coaxial cable, measured in dB per unit length. • primarily a result of the copper losses and the amount of power that is radiated from the cable. • The loss due to radiation is somewhat affected by the proximity of the cable to other surfaces. • This effect is more pronounced for cables having low coupling loss, however, significant changes will typically not occur until the spacing is less than 1 inch. Coupling Loss • Coupling loss is the ratio between the power in the cable and the amount of power received by a dipole antenna at a specified distance from the cable. • For example, if the power in the cable were 0 dBm and the power received by the antenna was -65 dBm, then the coupling loss would be 65 dB. • Typically Andrew will use distances of 2 meters (6.6 feet) or 6 meters (20 feet). • The value specified is the median value measured as the dipole travels parallel to the cable. • Typically, the radiated energy from the radiating cables is polarized. The degree of polarization is measured for all Andrew cables. The majority of the Andrew radiating cables have a dominant vertical polarization, however, this may be frequency dependent. Fading Characteristic • Radiating cables exhibit a fading characteristic that is a result of the multipath nature of the cable. • Typically, a fade will occur approximately every wavelength. • The depth of the fade is dependant not only on the design of the cable but also on the multipath environment. • Andrew quantifies the depth of fading by calculating the ratio between the median value of the coupling loss (50%) to the coupling loss that occurs at least 5%. • This produces a ratio of the 50 to 95% values. • For coupled mode RADIAX (RXL), the fading factor is typically 11 dB. • For RADIAX utilizing the array construction, radiating mode RADIAX (RCT), this value can be as low as 2 to 3 dB. • In a majority of systems applications, the low fading characteristic is somewhat negated by the environment June, 2011 Page 112Course 601-2-3 (c)2011 Scott Baxter
  • 113. Radiax - Tunnels Coherent Bandwidth • a measure of instantaneous bandwidth of the signal that can reliably be transmitted from the cable. • significant for wide bandwidth signals, especially third generation systems. • For applications involving wider bandwidths, the radiating mode cables (RCT) are designed to handle third generation signals. Launch Angle • For coupled mode RADIAX®, there is no dominant launch angle as RF energy emits from the cable at all angles. • For the radiating mode series of cables there is a dominant launch angle. • this dominant launch angle contributes to the low fading characteristic and the wider coherent bandwidth. The launch angle for any particular cable varies as a function of frequency and will typically be (45 degrees relative to a perpendicular line from the cable. Cable Orientation • For most cables, the orientation of the slots is not critical. • the dominant radiation is not directly from the slots, rather caused by current that flows in the outer jacket of the cable. • Directivity of the cable is related to the frequency and the size of the cable. That is, a 1-5/8 inch cable at 2400 MHz will be more directive than at 900 MHz, further the 1-5/8 inch cable will have a higher directivity than a 7/8" cable. Link Budget • basic elements of a link budget can be demonstrated by considering an example that involves a dual-bore road tunnel that is 800 meters (2620 feet) in length that is to be configured to handle cellular signals (824 MHz-894 MHz). The power per channel available for the downlink is 1 watt (+30 dBm). Following is an example link budget: June, 2011 Page 113Course 601-2-3 (c)2011 Scott Baxter
  • 114. Radiax – Tunnels (2) Downlink (Base to Mobile) Link Budget for 95% Coverage Available Power/Channel 30 dBm Distribution Loss, Power divider feeds both bores 3.5 dB Feeder Cable Loss, 30 m (100 ft) LDF5-50 1.6 dB Insertion Loss, 800 m (2620 ft) RCT7-TC-1 18.4 dB Coupling Loss @ 2 m 53.0 dB Antenna Loss, relative to dipole 3 dB Wide Tunnel Factor, tunnel width 10 m (33 ft), Wide Tunnel Factor = 20 Log (Width/2) 14 dB Vehicle Penetration Loss 6 dB Raleigh Fading, Z(Σ(σil2+σcl2+σant2+σ...)1/2 11 dB Statistical Variation 3 dB Tunnel Factors 0 dB Received Signal Power (Level that will be achieved at least 95% of the time at the terminated end of the cable) -83.5 dBm Uplink performance can be computed in a very similar manner. June, 2011 Page 114Course 601-2-3 (c)2011 Scott Baxter
  • 115. Radiax – Tunnels (3) Tunnel Effects on Design Coupling loss is dependent on the construction and shape of the tunnel. Typically, steel tunnels will perform appreciably better than concrete tunnels. Another factor that modifies the performance of the system is the placement of the cable in the tunnel. The cable should be mounted in the manner, which provides the best line-of- sight and proximity to the mobile/portable antenna June, 2011 Page 115Course 601-2-3 (c)2011 Scott Baxter
  • 116. June, 2011 Page 116Course 601-2-3 (c)2011 Scott Baxter BDA/DAS System Link BudgetsBDA/DAS System Link Budgets
  • 117. DAS Link Budgets The Components and Calculations of the RF Link The Maximum Allowable Path Loss The Components in the Link Budget Link Budgets for Indoor Systems Passive DAS Link Budget Active DAS Link Budget The Free Space Loss The Modified Indoor Model The PLS Model Calculating the Antenna Service Radius June, 2011 Page 117Course 601-2-3 (c)2011 Scott Baxter
  • 118. Link Budgets What is a link budget? A link budget is the calculation of signal strength on a Distributed Antenna System (DAS) at coax connection points. Example of a downlink link budget for one indoor antenna DAS; Roof RSSI(- 75dBm) + gain donor antenna (11dB) + loss coax to BDA (3dB) + gain BDA (62dB) + loss coax to indoor antenna (4.5dB) = -9.5dBm at indoor antenna port. June, 2011 Page 118Course 601-2-3 (c)2011 Scott Baxter
  • 119. Coverage Area of An Antenna Antenna coverage is determined by • the building characteristic path loss, • frequency band(s), • signal strength at antenna port and antenna type. For example, in a typical office application, an omni antenna with an output signal of +9.5dBm will maintain a coverage area of +85dB or better for 22k square feet on the cellular frequency band, 16k square feet on the PCS frequency band. June, 2011 Page 119Course 601-2-3 (c)2011 Scott Baxter
  • 120. June, 2011 Page 120Course 601-2-3 (c)2011 Scott Baxter BDA/DAS Equipment Manufacturers and Products BDA/DAS Equipment Manufacturers and Products
  • 121. Mobile Access Hardware Selection June, 2011 Page 121Course 601-2-3 (c)2011 Scott Baxter
  • 122. Mobile Access Hardware (2) June, 2011 Page 122Course 601-2-3 (c)2011 Scott Baxter
  • 123. Mobile Access Hardware (3) June, 2011 Page 123Course 601-2-3 (c)2011 Scott Baxter
  • 124. June, 2011 Page 124Course 601-2-3 (c)2011 Scott Baxter BDA/DAS Installation Techniques and Practices BDA/DAS Installation Techniques and Practices
  • 125. How to Properly Design an In-Building Distributed Antenna System (DAS) A typical in-building coverage system consists of two major components, • a bi-directional amplifier relaying and amplifying the RF signals between the remote base station and portable or mobile radios, and • a network to distribute the signal to every corner of the desired coverage area. The most common type of distribution network is a system of coax cables and indoor antennas called a Distributed Antenna System or DAS. Most of the reference materials and application notes on in-building coverage solutions have focused on the booster technologies or system design architecture. One often overlooked aspect in the system design is the DAS implementation. • This includes connecting all the cables and antennas throughout the building and balancing the signal levels at each DAS node. • If ignored, an improperly designed DAS results in degraded performance and unnecessary cost increases. June, 2011 Page 125Course 601-2-3 (c)2011 Scott Baxter
  • 126. The DAS Design Process The first step of DAS design is to obtain an accurate and up-to-date blueprint of the building. • An architectural drawing is best, but even a fire exit map will suffice, if drawn to scale. Be careful when using the scale on any drawing to calculate the real dimensions; • the drawing may not be the same size as originally printed. . The second step is to gather all relevant physical information on building and DAS installation. • What kind of material was used for exterior construction? • Could some RF signals be present on upper floors and near exterior boundaries that will reduce the need for the in-building coverage? • What kind of material was used for interior construction, drywall or concrete? • Is the building designed for a special application that may result in RF blockage? • Many hospitals and power generating plants fall into this category. • Are there any restrictions on the cable runs and antennas installation? • Some buildings won’t allow any visible hardware for aesthetic reasons. • Where can the cables go between floors? Where will the head-end booster be located? • A quick word on another type of DAS: radiating cable. It is essentially a coax cable with lots of tiny slits cut along the length of the cable. Each slit functions as a tiny antenna with RF energy leaking out of it, hence the nickname “leaky cable”. June, 2011 Page 126Course 601-2-3 (c)2011 Scott Baxter
  • 127. Two Sets of Diagrams To make it easier to see, a DAS design is often drawn up with 2 sets of diagrams • one with direct marking on the building blueprint to indicate the location of the antennas and cable splits, • a second set of “abstract” drawings (typically in VisioTM or AutocadTM) showing the cable lengths and coupler models. how do you connect all the cable segments and antennas to make them into a network? • directional couplers are much better alternatives than splitters at this task. • They offer various power split ratios to allow the designer flexibility in balancing the power level at each DAS node. The main goal of using couplers is to offset the difference in cable losses by using the different loss ratios between the two outputs of the coupler. June, 2011 Page 127Course 601-2-3 (c)2011 Scott Baxter
  • 128. Balancing Losses Using Couplers With 15 dB loss in one branch vs. 5 dB loss in the other, let’s select a coupler that has 10 dB of difference in power split ratios. • Put the lower loss port on the higher loss branch, and the higher loss port on the lower loss branch • Most manufacturers provide products with different split ratios to allow matching the loss differentials as closely as possible. In the left Figure, we have a branch with 150 ft and about 3.3 dB of insertion loss, and a branch of 3 ft jumper cable with 0.5 dB of loss. • select a coupler that can make up the loss differential in the two cable runs. • Browsing, select a coupler with a 4.8/1.8 dB split ratio as Coupler #1. • connect the longer cable run to the port with 1.8 dB, and connect the shorter cable run to the 4.8 dB, the total losses from the input of the coupler to the antennas are 3.3 + 1.8 = 5.1 dB and 0.5 + 4.8 = 5.3 dB respectively. • If we had used a 3 dB splitter, the total losses would have been 3.3 + 3 = 6.3 dB and 0.5 + 3 = 3.5 dB. • see the benefit of using a coupler as it manages to balance the signal levels at the two antennas within 0.2 dB of each other. • Next, work backwards toward the booster. Take the worse number of the two above (5.1 and 5.3 dB, so we use 5.3 dB), and add the 0.5 dB cable loss between the two couplers, we get 5.8 dB, which is the loss from the output of Coupler #2 to either Antenna #1 or Antenna #2. June, 2011 Page 128Course 601-2-3 (c)2011 Scott Baxter
  • 129. Balancing Losses Using Couplers Assume there are more floors above this one. The DAS on the upper floor has been balanced using couplers in the same way as illustrated, and the total loss in the DAS on the upper floor is 10 dB. See the left figure as we “propagate” the loss in the DAS backwards toward the booster. We want to select a coupler that will offset the loss differential and balance the signal levels. we find a coupler with a 6/1.2 dB split ratio. If we connect the 6 dB coupled port to the lower loss DAS on this floor, and the 1.2 dB throughput port to the higher loss DAS on the upper floor, we get 5.8 + 6 = 11.8 dB and 10 + 1.2 = 11.2 dB. The total losses from the input of Coupler #2 to the cable runs on this floor and the cable runs on the upper floor are within 0.6 dB of each other. June, 2011 Page 129Course 601-2-3 (c)2011 Scott Baxter
  • 130. Continuing Back to the Booster If there are more floors below it or more cable splits between this one and the booster, the same iteration is to be repeated until we work all the way back to the booster. A typical in-building coverage system can vary from 10,000 sq ft to 1,000,000 sq ft or more, with the number of couplers from a handful to hundreds. However, the rules of calculating the losses and selecting the couplers stay the same, allowing the designer to balance any DAS and achieve the optimal signal levels throughout the network. The total DAS loss should be limited to no more than 25~30 dB, in order to maintain a sufficient signal to noise ratio. working backwards toward the booster, eventually the system loss exceeds the limit. We know that we will need to insert an in-line booster at that point. The exact location depends on the practical constraints of the building, but wherever the in-line booster is, the cumulative loss ends at its output, and starts from zero again on the other side of the in-line booster. Another alternative is to use coax with larger diameters with lower insertion loss. But that option has high material and labor costs, as well as the physical limitations on bending radius and weight support issues. June, 2011 Page 130Course 601-2-3 (c)2011 Scott Baxter
  • 131. June, 2011 Page 131Course 601-2-3 (c)2011 Scott Baxter BDA/DAS Example Case StudiesBDA/DAS Example Case Studies
  • 132. Site Survey A site survey is performed prior to the final design. Objectives: • to characterize signal propagation within the building • investigate donor signal options and to • investigate equipment space and cable routing issues. Proper engineering and planning will minimize capital expenditures while ensuring that coverage goals for each of the mobile service providers are met. Several factors must be considered when designing a neutral hosts system. • characterize signal propagation within the target area. • test transmitters are placed at various locations within the building. • A receiver and mapping software are used to record the signal strength at various locations within the building. A sample transmitter test is shown on the next page. June, 2011 Page 132Course 601-2-3 (c)2011 Scott Baxter
  • 133. Site Survey Results Map June, 2011 Page 133Course 601-2-3 (c)2011 Scott Baxter
  • 134. Site Survey Results Various transmitter tests are performed to get a thorough understanding of the building’s propagation characteristics In the test just shown, signal loss does not degrade in direct proportion to the distance from the transmitter but is largely dependant on the building structure. • Using the proper tools and procedures to characterize signal loss helps ensure that the system is not over designed and meets customer requirements. Suitable equipment room space and it’s proximity to the coverage objective strongly affect the type of system installed and its overall cost. • These issues are investigated at the time of the site survey. Potential donor signals are also investigated for neutral host opportunities that may not require dedicated base stations. • These measurements are generally performed at the roof level. • A receiver capable of measuring multiple technologies and frequencies is required for these measurements. • Alternatively phones from various carriers with an accessible diagnostic or debug mode can be used. Potential donor antenna locations and roof penetration issues also need to be investigated at this stage. June, 2011 Page 134Course 601-2-3 (c)2011 Scott Baxter
  • 135. System Design The building characterization along with available equipment space determined during the site survey is the basis for system design. The propagation model is optimized for accuracy using the transmitter tests performed in the site survey. • Each wall type within a building affects signal propagation differently therefore each wall type must be identified in the propagation model and assigned attenuation values obtained from the information in the transmitter tests. • This allows for optimum transmitter location and minimizes required capital. The system design determines which OEM hardware solution is appropriate for the venue. A partial design (one floor of a multi story building) is shown in the next figure. June, 2011 Page 135Course 601-2-3 (c)2011 Scott Baxter
  • 136. One Floor Design June, 2011 Page 136Course 601-2-3 (c)2011 Scott Baxter
  • 137. Construction Once the proposed design is approved for installation by the building manager, a preconstruction site visit is completed. • During this visit, equipment locations and cable routes are verified, as well as acceptable contractors to perform any electrical or roofing work that may be required. • If any of the locations proposed in the design are not acceptable to the building manager, the design is modified to allow for these changes. • Once final approval is obtained, the actual installation of equipment begins. Construction begins with the installation of cabling, typically both fiberoptic and coaxial. • Cabling is routed from the main equipment room throughout the building to all the antenna locations. A DAS system allows for the reuse of many network elements - trunking and hubbing minimize the amount of new cable required. Cable is run in existing cable trays or utility chases where available. The equipment deployment is fairly straight forward. The main equipment room typically needs dedicated electrical services to handle both the DAS equipment and the carrier equipment. The remote units and the antenna use minimal power and usually only involve a 110v outlet. June, 2011 Page 137Course 601-2-3 (c)2011 Scott Baxter
  • 138. Optimization and Verification When the construction phase is complete, the system is tested and optimized. • Each coax and fiber optic cable is swept, • isolation tests are performed, • sources of interference are investigated, • donor signal levels are verified, and • a final coverage assessment is performed. • The results of the coverage analysis reflect both coverage provided by the external macro cell and enhanced coverage provided by the DAS. The next page show is a sample plot that can be used to measure the success of the installation. June, 2011 Page 138Course 601-2-3 (c)2011 Scott Baxter
  • 139. Signal Levels After Activation June, 2011 Page 139Course 601-2-3 (c)2011 Scott Baxter
  • 140. DAS Reduce Interference to Medical Devices Interference Concerns Much has been written about cellular devices interfering with medical equipment. Generally, the use of a DAS will greatly lower the power output of the mobile device, reducing the risk of interference. Poor coverage inside a building means that a mobile device has to transmit at a higher power setting to ensure that a connection with the cell site is made. Cellular devices can transmit at relatively high power levels (perhaps 1 W) for short periods of time such as during the ring cycle. However, if the cellular device is in a reasonably good coverage location, it will transmit at much lower levels (potentially under 5 mW), which is not a real concern. In addition if you have good coverage, the battery life of the device will be greatly enhanced. Essentially a DAS provides 5 bars all the time, thus less power is required to enable the up-link from the mobile devices. The use of DAS in healthcare will actually decrease electromagnetic interference and improve battery life of these devices. June, 2011 Page 140Course 601-2-3 (c)2011 Scott Baxter
  • 141. June, 2011 Page 141Course 601-2-3 (c)2011 Scott Baxter Course 603 Wireless BDA and DAS Advanced Topics Wireless BDA and DAS Advanced Topics
  • 142. June, 2011 Page 142Course 601-2-3 (c)2011 Scott Baxter 603 Course Outline Traffic Capacity of BDA/DAS Systems Intermodulation Distortion and Interference External Interference Interference Sources MIMO – Multiple Input-Output Broadband Data Systems Femtocells • Comparison of function and performance against BDA/DAS technologies • Differences and advantages
  • 143. June, 2011 Page 143Course 601-2-3 (c)2011 Scott Baxter Intermodulation Distortion and Interference Intermodulation Distortion and Interference
  • 144. Modulation and Mixing vs. Intermodulation When two signals are intentionally combined in a non- linear device we call the effect modulation • Amplitude modulator, or quad phase modulator • Mixer, down or up converter in superheterodyne When two (or more) signals are unintentionally combined in a non-linear device, we call the effect intermodulation (a pejorative term) An analogy: Botanists use soil to grow plants. But on your living room carpet, soil is just dirt. IM signals increase system noise, or cause distinctive recognizable interference signals June, 2011 Page 144Course 601-2-3 (c)2011 Scott Baxter
  • 145. Intermod Basics Definition: Intermodulation (“IM”) is the unintended mixing of legitimate RF signals, producing undesired signals (‘intermodulation products’) on unrelated frequencies possibly already being used for other services • IM can devastate reception on certain frequencies at base stations and other communication facilities Intermodulation occurs because signals are passing through a nonlinear device, allowing each signal to alter the waveshape of the others • the frequencies of the intermod products are sums and differences of multiples of the original signal frequencies, and can be calculated exactly • the strength of the intermod products depends on the degree of nonlinearity of the circuits involved, and can be predicted with good accuracy using measured “intercept” levels Power transfer characteristics of typical amplifier or other device Noise floor Input power (dBm) Output power (dBm) Third order intercept point Third order intermodulation products Predicted power f f1 f2 Non-linear deviceInput Output f 3f1-2f2 3f2-2f1f1 f2 2f2-f12f1-f2 June, 2011 Page 145Course 601-2-3 (c)2011 Scott Baxter
  • 146. Intermodulation Interference Analysis There are three basic categories of Intermodulation (IM) interference: Transmitter produced IM is the result of one or more transmitters impressing a signal in the non-linear final output stage circuitry of another transmitter, usually via antenna coupling. The IM product frequency is then re-radiated from the transmitter's antenna. Receiver produced IM is the result of two or more transmitter signals mixing in a receiver RF amplifier or mixer stage when operating in a non-linear range. “Other" radiated IM is the result of transmitter signals mixing in other non-linear junctions. These junctions are usually metallic, such as rusty bolts on a tower, dissimilar metallic junctions, or other non- linear metallic junctions in the area. IM products can also be caused by non-linearity in the transmission system such as antenna, transmission line, or connectors. BPF Preamp Splitter RX TXCircDuplexer Comb TXCircDuplexer Comb June, 2011 Page 146Course 601-2-3 (c)2011 Scott Baxter
  • 147. Intermodulation Interference Analysis Communication sites with co-located transmitters, usually have RF coupling between each transmitter and antenna system. • This results in the signals of each transmitter entering the nonlinear final output (PA) circuitry of the other transmitters. When intermodulation (IM) products are created in the output circuitry and they fall within the passband of the final amplifier, the IM products are re-radiated and may interfere with receivers at the same site or at other nearby sites. Additionally, these strong transmitter signals may directly enter a receiver and drive the RF amplifier into a nonlinear operation, or • if not filtered effectively by the receiver input circuitry, these signals could mix in the nonlinear circuitry of the receiver front- end or mixer, creating IM products directly in the receiver. June, 2011 Page 147Course 601-2-3 (c)2011 Scott Baxter
  • 148. Transmitter Noise Analysis Transmitter noise interference occurs because a transmitter radiates energy on its operating frequency as well as frequencies above and below the assigned frequency. The energy that is radiated above and below the assigned frequency is known as sideband noise energy and extends for several megahertz on either side of the operating frequency. This undesired noise energy can fall within the passband of a nearby receiver even if the receiver's operating frequency is several megahertz away. The transmitter noise appears as "on-channel" noise interference and cannot be filtered out at the receiver. • It is on the receiver's operating frequency and competes with the desired signal, which in effect, degrades the operational performance. June, 2011 Page 148Course 601-2-3 (c)2011 Scott Baxter
  • 149. Transmitter Noise Analysis The analysis predicts each transmitter’s noise signal level present at the input of each receiver. • It takes into account the transmitter’s noise characteristics, frequency separation, power output, transmission line losses, filters, duplexers, combiners, isolators, multi-couplers and other RF devices that are present in both systems. • Additionally, the analysis considers the antenna separation space loss, horizontal and vertical gain components of the antennas as well as how they are mounted on the structure. The gain components are derived from antenna pattern data published by each manufacturer. June, 2011 Page 149Course 601-2-3 (c)2011 Scott Baxter
  • 150. Transmitter Noise Analysis The analysis determines how much isolation is required, if any, to prevent receiver performance degradation caused by transmitter noise interference. The Table below depicts the results of this analysis. For each receiver, the transmitter that has the worst-case impact is displayed. The Signal Margin represents the margin in dB, before the receiver’s performance is degraded. A negative number indicates that the performance is degraded and the value indicates how much additional isolation is required to prevent receiver performance degradation June, 2011 Page 150Course 601-2-3 (c)2011 Scott Baxter
  • 151. Receiver Desensitization Analysis Receiver desensitization interference occurs when an undesired signal from a nearby "off-frequency" transmitter is sufficiently close to a receiver's operating frequency. The signal may get through the RF selectivity of the receiver. If this undesired signal is of sufficient amplitude, the receiver's critical voltage and current levels are altered and the performance of the receiver is degraded at its operating frequency. The gain of the receiver is reduced, thereby reducing the performance of the receiver. June, 2011 Page 151Course 601-2-3 (c)2011 Scott Baxter
  • 152. Receiver Desensitization Analysis A transmitter can be operating several megahertz away from the receiver frequency and/or its antenna can be located several thousand feet from the receiver's antenna and still cause interference. The analysis predicts each transmitter’s signal level present at the input of each receiver. It takes into account the transmitter’s power output, frequency separation, transmission line losses, filters, duplexers, combiners, isolators, multi-couplers and other RF devices that are present in both systems. Additionally, the analysis considers the antenna separation space loss, horizontal and vertical gain components of the antennas as well as how they are mounted on the structure. The gain components are derived from antenna pattern data published by each manufacturer. June, 2011 Page 152Course 601-2-3 (c)2011 Scott Baxter
  • 153. Receiver Desensitization Analysis The analysis determines how much isolation is required, if any, to prevent receiver performance degradation caused by receiver desensitization interference. The Table provided separately depicts the results of this analysis. • For each receiver, the transmitter that has the worst-case impact is displayed. • The Signal Margin represents the margin in dB, before the receiver’s performance is degraded. • A negative number indicates that the performance is degraded and the value indicates how much additional isolation is required to prevent receiver performance degradation. June, 2011 Page 153Course 601-2-3 (c)2011 Scott Baxter
  • 154. Intermodulation Interference Analysis The frequencies of IM products are derived from mathematical formulae. IM products are classified by their "order" (2nd, 3rd, 4th, ...Nth). Some of the more common forms of mixing are illustrated in the following examples. Note that The "A", "B", and "C" designations are the mixing frequencies. The numerical number assigned to the letter designation indicates the harmonic relationship of the frequency. Thus, 2A means the 2nd harmonic of frequency A. Order Mixing Formulae First A=B, A=C, etc. Second A ± B, A ± C, etc. Third A + B - C, A ± 2B, 2A ± B, etc. Fourth A ± 3B, 2A ± 2B, 3A ± B, etc. Fifth A ± 4B, 2A ± 3B, 3A ± 2B, 4A ± B, etc. Sixth A ± 3B ± 2C, 2A ± 2B ± 2C, 3A ± 2B ± C, etc. Seventh A ± 6B, 2A ± 5B, 3A ± 4B, 4A ± 3B, 5A ± 2B, etc. Eighth A ± 7B, 2A ± 6B, 3A ± 5B, 4A ± 4B, 5A ± 3B, 6A ± 2B, Ninth A ± 8B, 2A ± 7B, 3A ± 6B, 4A ± 5B, 5A ± 4B, 6A ± 3B, c. June, 2011 Page 154Course 601-2-3 (c)2011 Scott Baxter
  • 155. Intermodulation Interference Analysis The IM product formulae are just a few of the many possible combinations. When there are four frequencies involved at one time, the mixing possibilities increase tremendously. Not all of the mixing possibilities are significant in creating interference signals. Some fall “out-of-band” of the receiver and the higher order IM products are usually weaker in signal strength. June, 2011 Page 155Course 601-2-3 (c)2011 Scott Baxter
  • 156. Transmitter Spurious Output Interference Analysis Transmitter spurious output interference can be attributed to many different factors in a transmitter. The generation of spurious frequencies could be due to non-linear characteristics in a transmitter or possibly the physical placement of components and unwanted coupling. If a spurious signal falls within the passband of a nearby receiver and the signal level is of sufficient amplitude, it can degrade the performance of the receiver. June, 2011 Page 156Course 601-2-3 (c)2011 Scott Baxter
  • 157. Transmitter Spurious Output Interference Analysis The analysis takes into account a transmitter’s spurious output specification, output levels, transmission line losses, filters, duplexers, combiners, isolators, multi-couplers and other RF devices that are present in each system. Additionally, the analysis considers the antenna separation space loss, horizontal and vertical gain components of the antennas as well as how they are mounted on the structure. The gain components are derived from antenna pattern data published by each manufacturer. The analysis determines how much isolation is required to prevent receiver performance degradation for any transmitter spurious signals that fall within a receiver’s passband. June, 2011 Page 157Course 601-2-3 (c)2011 Scott Baxter
  • 158. Non-linear Effects and Intermodulation Almost “everything” is slightly (or extremely) non-linear. Only free space is theoretically a true linear medium. Particularly non-linear are: • all active semiconductor devices • corroded electrical connections, etc. When high RF current levels are present in non-linear devices, waveform distortion occurs • A distorted (clipped, peaked, etc.) non-sinusoidal waveform is equivalent to a sum of sine waves of several different frequencies (Fourier series) • Product waveforms can also occur when two frequencies are “mixed” due to the non-linearity • if the nonlinear device characteristics are accurately known (intercept point, etc.), IM amplitudes can be accurately computed. • If nonlinear device characteristics are unknown, the worst-case intermod mechanism will have a conversion loss of at least 6 dB. June, 2011 Page 158Course 601-2-3 (c)2011 Scott Baxter
  • 159. What to do about IM Try to prevent or reduce the amplitude of strong RF signals reaching receivers in wireless systems • Reduce or eliminate at the source, if feasible (spurious emissions from electric lamps, signs, elevator motors, etc.) • Shielding, enclosure, modification of antenna directionality to reduce the penetration of electromagnetic waves • Identify and eliminate secondary non-linear radiators: parallel metal joints with conductive connections, ground all parts of metal fences, rain gutters, etc. (also improves lightning protection) • Conducted RF from wires, etc. entering receiver can be reduced via low pass or band pass filters, ferrite beads, etc. • Notch filters to remove source RF, or specific harmonics or products June, 2011 Page 159Course 601-2-3 (c)2011 Scott Baxter
  • 160. Intermod “Forensics”Intermod “Forensics” June, 2011 Page 160Course 601-2-3 (c)2011 Scott Baxter
  • 161. Intermod “Forensics” and Detective Work “Detective” Work to identify • the likely creation paths for an observed intermod problem • methods of reducing the intermod production or delivery to non-problematic levels Identify source and victim destination • analyze each conceivable path – gains, isolations, line losses, conversion losses, bandpass filters in the path – compute the likely intermod amplitude at the victim due to that path – the path with the largest calculated amplitude at the victim is the most suspect and should be investigated or mitigated first June, 2011 Page 161Course 601-2-3 (c)2011 Scott Baxter
  • 162. Truth Serum for a Witchhunt: a lowly attenuator Often the source of intermod is unclear – it could be anywhere: • In the affected victim receiver • In a transmitter of one of the source signals • In some other nonlinear device nearby A simple attenuator (usually 3, 6 or 10 db “pad”) can be used to help isolate where the intermod is occuring • Place pad in front of the victim receiver – If the intermod decreases the same amount as the pad attenuation, it is coming in from outside, beyond the pad Keep looking elsewhere – If the intermod decreases by a multiple of the pad attenuation, it is being generated in the receiver Consider additional filtering for the receiver • Place high power pad in front of the transmitters, one by one – When the intermod is reduced by the maximum amount, the pad is on the transmitter producing most of the intermod June, 2011 Page 162Course 601-2-3 (c)2011 Scott Baxter
  • 163. Using an Attenuator for Intermodulation Location TX1 TX2 RX IM -90 dbm Troublesome intermod is received on a product frequency of TX1 and TX2. Where is the source? TX1 TX2 RX IM -96 dbm A 6 db pad on the receiver merely reduces all signals including the intermod by 6 db. The intermod is originating outside this receiver. 6 db TX1 TX2 RX IM -102 dbm With a 6 db pad on TX1, the intermod goes down 12 db. The intermod is reduced, but this does not prove where the IM is generated. 6 db TX1 RX IM -114 dbm With a 6 db pad on TX2, the intermod goes down lower than anywhere else. TX2 is an intermod generator.Now consider additional flitering for TX2 to suppress the IM. 6 db TX2 June, 2011 Page 163Course 601-2-3 (c)2011 Scott Baxter
  • 164. Working With Repeaters AKA Re-Radiators, Cell Enhancers, Boosters Working With Repeaters AKA Re-Radiators, Cell Enhancers, Boosters June, 2011 Page 164Course 601-2-3 (c)2011 Scott Baxter
  • 165. Cell RR Wireless Reradiators Reradiators (also called “boosters”, “repeaters”, “cell enhancers”) are amplifying devices intended to add coverage to a cell site Reradiators are transparent to the host Wireless system • A reradiator amplifies RF signals in both directions, uplink and downlink • The system does not control reradiators and has no knowledge of anything they do to the signals they amplify, on either uplink or downlink Careful attention is required when using reradiators to solve coverage problems • to achieve the desired coverage improvement • to avoid creating interference • to ensure the active search window is large enough to accommodate both donor signal and reradiator signal as seen by mobiles Reradiators are a ‘“crutch” with definite application restrictions. Many operators prefer not to use re-radiators at all. However, reradiators are a cost-effective solution for some problems. June, 2011 Page 165Course 601-2-3 (c)2011 Scott Baxter
  • 166. Consideration Checklist for Reradiators Must not overdrive Repeater to output levels above max • Forward link case • Reverse link case Repeater gain must not exceed antenna isolation plus safety cushion • Forward link case • Reverse link case Repeater output noise floor must not raise BTS noise floor more than 1 db Repeater Donor must be dominant, so no other defacto donors appear Windows of mobile and BTS must span both the BTS-mobile direct signal and BTS-RR-mobile signal (see separate page and diagrams) Donor must have sufficient capacity to handle intercepted traffic Power budgets and levels must take into account maximum carriers maximum loading situation General: Don’t allow “foldback” coverage from RR in direction of donor BTS unless absolutely required by unavoidable situation • Life is so much better downrange – relatively narrow windows are adequate • Wide windows are needed if you get between donor and RR June, 2011 Page 166Course 601-2-3 (c)2011 Scott Baxter
  • 167. Wireless Reradiators Propagation Path Loss Considerations To solve a coverage problem using a reradiator, path loss and link budget must be considered • how much reradiator gain is required? • how much reradiator output power is required? • what type of antennas would be best? • how much antenna isolation is needed? • how big will the reradiator footprint be? • how far can the reradiator be from the cell? • will the reradiator interfere with the cell in other areas? • What is the propagation delay through the reradiator, in chips? • Will search windows need to be adjusted for compensation? Cell RR ERP GainPath Loss Path Loss (free space??) Gain RR Gain Line Loss Signal Level in target area (free space usually applies) June, 2011 Page 167Course 601-2-3 (c)2011 Scott Baxter