9.1 OVERVIEW
• Thecoaxial cable is a transmission line consisting of two coaxial
cylindrical conductors, separated by a dielectric (see Fig. 2.1).
• The two conductors, here shown as homogeneous, are often made of
braided small diameter copper wires.
• If Er denotes the relative permittivity of the insulator, the line
parameters are given by:
4.
• Coaxial Cable.
•The Field Lines Of The Electric
Field Are Shown By Solid Lines,
Those Of The Magnetic Field
By Dashed Lines.
• Geometry Of The Coaxial Cable.
5.
• The MaximumFreq For Which The Coaxial Cable Is Single Mode Is
Approximately:
• Where V (z) Is The Voltage.
• Hence The Maximum Electric Field,
Not To Be Exceeded In Order To Avoid
Sparks, Is On The Surface Of The Inner
Conductor And Has The Value:
6.
• Worked Example
•
•Compute the parameters of a cable, with inner conductor diameter d
=1.6 mm, outer conductor diameter D = 5.8 mm, ²r = 2.3.
• Solution:
• Applying the previous formulas we get L = 0.26 µH/m, C = 99.35 pF/m,
Z∞ = 50.92 Ω, Vf /c = 1/ √ Er = 65.9%, fmax = 17.0 GHz.
• Plse kindly Very these Answers,
• The normalized maximum electric field is Emax = 485.3V/m if the voltage
V is 1V.
9.2 Two-wire line
•Two-Wire Lines The two-wire transmission line consists of two parallel
cylindrical conductors of radius a separated by distance d from each other,
as shown below
• Examples of TL: (a) coaxial cable, (b) two wire line, (c) optical fiber, (d)
microstrip , (e) stripline.
9.
• Shielded two-wireline
• To avoid the electromagnetic compatibility problems of the two-wire line,
the structure below can be used.
• Shielded two-wire line and field configuration of the symmetric (balanced)
TEM mode.
10.
• Note ThatThis Is A Three Conductor Line (Two Plus A Grounded One).
• In This Case There Are Two TEM Modes,
• A Symmetric (Balanced) One Where The Potentials Of The Two Inner Conductors Are
Symmetric With Respect To That Of The Outer One, Connected To Ground,
• And An Asymmetric (Unbalanced) One, With Different Parameters.
• The Parameters For The Symmetric Mode Can Be Computed From The
Following Equations:
11.
9.2 COAXIAL CABLES,TERMINATIONS, CONNECTORS &
TRANSITIONS
COAXIAL CABLES
• The Coaxial Cable Is A Transmission Line Consisting Of Two Coaxial
Cylindrical Conductors, Separated By A Dielectric.
• The Two Conductors, Here Shown As Homogeneous, Are Often Made Of
Braided Small Diameter Copper Wires.
• The Line Parameters Are Given By:
12.
• Coaxial Cable
•The Field Lines Of The Electric Field Are
Solid Lines Shown By ,
• Those Of The Magnetic Field By Dashed Lines.
• Observe That:
• The Electric Field Configuration Is That Of A Cylindrical Capacitor,
• Consistently With The Fact That The TEM Mode Has Zero Cutoff Frequency.
• If The Operation Frequency Increases,
• A Point Is Reached In Which Higher Order Modes Start To Propagate.
13.
• The MaximumFreq For Which The Coaxial Cable Is Single Mode Is Approx:
• Where V (z) Is The Voltage.
14.
• The MaximumElectric Field, Not To Be Exceeded In Order To
Avoid Sparks,
• Is On The Surface Of The Inner Conductor @ Has The Value:
• Note That, Coaxial Cable Is An Unbalanced Line,
• Meaning That,
• The Return Conductor Is Connected To Ground.
• Hence, The Voltage Of The Inner Conductor Is Referred To Ground.
• Please kindly See Worked Example in the Handout.
15.
Coaxial Cables
•These Are Used To:
• Transmit Electrical Energy, Or Signals, From One Location To Another, i.e.,
• To Connect A Source To A Load, Such As A Transmitter To An Antenna.
• This Is Accomplished With A Transverse Electrometic (TEM) Wave Field
Distribution Propagation Within The TL, Or Coaxial Cable,
• Governed By TL Theory.
• Coaxial Cable (Coax) Is Typically Identified Or Classified According To Its
Impedance Or Rg-type.
• E.g., A 50-ohm Coax Or An RG-8 Type Coax.
16.
• Construction:
• ATypical Coaxial
Cable is as shown
• The Center Conductor May Be Made Of Various Materials & Constructions.
• Most Common Constructions Are Solid Or Seven-strand Conductors.
• Solid Conductors Are Used In:
• Permanent, Infrequently Handled Or Low Flex Applications &
• Stranded Conductors Are Used In Flexible Cable Appns.
• Common Materials Include:
• Copper, Tinned Or Silver Plated Copper, Copper Clad Steel & Copper Clad Aluminum, Details are in
the Handout.
17.
•Electrical Properties:
• TheMost Common Electrical Property Referred To In Coax Cable Is The
Characteristic Impedance, Or Simply Impedance.
• Coax Cable Is Typically Designed As 50 Ohm, 75 Ohm, And 93 Ohm
Depending Upon The Application.
• A Simple Formula To Determine The Impedance Of A Coaxial Is:
18.
• The PropagationDelay in Coaxial Cable is given By:
Physical Properties:
• The Mechanical & Physical Properties May Be Critical In Selecting The Appropriate
Cable For The Appn.
• Physical Dimensions Are Critical To Assure That An Industry Standard Connector Is
Available.
• Other Odd-size Dimensions Will Require The Use Of A Custom Termination.
• Diameter Of The Center Conductor, Core, & Jacket Are Critical Values
19.
• Applications:
• OneOf The Broadest Uses Of Coaxial Cable Is For Video Distribution.
• From Catv Signals Around The Neighborhood To Precision Digital Signals In A
Post-production Studio,
• These Signals Are Routed On 75 Ohm Coaxial Cable.
• Widely Used In Wireless & Antenna Applications,
20.
COAXIAL TERMINATIONS
• ToAvoid Confusing Reflections From The Ends Of Cables, It Is Essential
That:
• All Cables Carrying Fast Pulses Be Terminated At Their Outputs By Their
Characteristic Impedance Of 50 Ohms,
oEither With A Terminating Plug On A T-connector, Or By An Internal
Termination At The Input Of A Circuit.
21.
• When usingcoaxial cables it is usually important to avoid reflections at the
end of the cable.
• If a cable is terminated with an impedance Z ,
• The ratio of the incoming voltage Vi to the reflected voltage Vr is given by:
Vr/Vi = [Z - Zo]/[Z + Zo].
• The total voltage across the terminating resistance is V = Vi + Vr.
• Three cases are of interest:
1. If Z = 0: Then Vi = - Vr and V = 0, as you would expect for a short
circuit.
2. If Z = 8: Then Vi = + Vr and V = 2 Vi.
3. If Z = Ro: Then Vi = 0 and V = Vi.
22.
•When Z =Zo = 50 Ohms,
• The Cable Is Properly Terminated And There Is No Reflected Signal.
•Proper Termination Is Also Important For Maintaining The
Line Shape For Sharply Rising Pulses;
•If The Termination Is Not Proper,
• The Rise & Fall Times For A Square Pulse Will Be Slowed &
• The Pulse Will Be Broadened.
23.
9.3 COAXIAL CONNECTORS
•For HF Operations The Average Circumference Of A Coaxial Cable Must Be
Limited To About One Wavelength,
• In Order To Reduce Multimodal Propagation & Eliminate Erratic Reflection
Coefficients, Power Losses, & Signal Distortion.
Seven types of microwave coaxial connectors are described below.
• APC-3.5 The APC-3.5 (Amphenol Precision Connector-3.5 mm.
• It provides repeatable connections and has a very low voltage standing-wave
ratio (VSWR).
24.
2. APC-7: TheAPC-7 (Amphenol Precision Connector-7 mm)
• Provides A Coupling Mechanism Without Male Or Female Distinction
• The Most Repeatable Connecting Device Used For Very Accurate 5o-Ohm Measurement
Applications. Its VSWR Is Extremely Low, In The Range Of 1.02 to 18 GHz.
3. BNC: The BNC (Bayonet Navy Connector) Operates Very Well At Freq Up To About 4 GHz;
• Beyond That It Tends To Radiate Electromagnetic Energy.
• The BNC can accept flexible cables with diameters of up to 6.35 mm (0.25
in.) Zo of 50 to 75 ohms.
• It is now the most commonly used connector for frequencies under 1 GHz.
Please Refer to Handout for the Remaining 4 Types
•COAXIAL TRANSITIONS
•
• CoaxialTransitions Are Components Used To Move From One Tx
Medium Type To A Different Tx Medium.
• This Could Be From One Waveguide Size To Another Or
• From Full Height To Reduced Height Waveguide Or From Waveguide
Tube To Coaxial Line Or From Coaxial Line To Waveguide Tube.
• Typical Examples are the transition of RF signals from:
• Coaxial Cables to Waveguides &
• From Waveguides to A Coaxial Cables
Coaxial Attenuators
• Acoaxial attenuator is a linear passive bidirectional TL component designed
to be inserted b/n two coaxial lines,
• In order to reduce the Pin in a matched system by a predetermined ratio without
otherwise disturbing the behaviour of the equipment.
• The ratio of input to output power is expressed in logarithmic terms where 3
dB as a power ratio is 2, 6 dB is 10, 20 dB is 100 and 30 dB is 1000 etc...
• The power absorbed by an attenuator is returned to the environment
through heat transfer by convection or conduction cooling.
• Attenuator RelatedParameters
• "NOMINAL ATTENUATION OR ATTENUATION VALUE:
• The nominal value of attenuation is the standard value determined by
the manufacturer.
• This parameter is a representation of the power ratio b/n the input &
the ouput of the attenuator.
• It is expressed in dB :
• P out (W) Attenuation in dB = 10 log P in (W)
32.
• "ATTENUATION DEVIATION
•The attenuation over full specified bandwidth does not exceed
the nominal value ¦ attenuation deviation.
• This parameter is expressed in dB.
• For example, an attenuator with 6 dB nominal value and ¦ 0.3 dB
deviation
• Do not exceed 5.7dB minimum value and 6.3 dB maximum value.
33.
• " TEMPERATURESENSITIVITY
• The maximum change of attenuation in dB per dB per °C over the
operating temperature range.
• Example:
• If temperature sensitivity is 5.10--4 dB/dB/°C,
• For a 20 dB attenuator over a 20* 20* 5.10--4 = 0.2 dB Attenuation
Variation.
34.
• " FREQUENCYRANGE
• The Freq range indicated for each device is the range which RADIALL
specifies the device performance.
• " AVERAGE POWER HANDLING
• It is the maximum Continues Wave input power applied for a long time at
room temperature, or at the maximum temperature of 75°C.
• That the attenuator can handle whithout permanently changing the specifications
of the component.
• Any overpowering beyond this limit can significantly alter the input power
handling of the attenuator.
35.
• " PEAKPOWER HANDLING
• It Is The Maximum Peak Power Which, When Applied At Maximum
Room Temperature Under A Pulse Of One Microsecond Every
Millisecond,
• Will Not Permanently Change The Specifications Of The Attenuator.
• Any Overpowering Beyond This Limit Will Alter The Input Power
Handling Of The Attenuator.
36.
•Coaxial Phase Shifters
•Phase Shifters Are Used To Change The Transmission Phase Angle (Phase Of S21) Of A Network.
• Ideal Phase Shifters Provide Low Insertion Loss, & Equal Amplitude (Or Loss) In All Phase States.
• While The Loss Of A Phase Shifter Is Often Overcome Using An Amplifier Stage, The Less Loss,
The Less Power That Is Needed To Overcome It.
• Most Phase Shifters Are Reciprocal Networks,
• Meaning That They Work Effectively On Signals Passing In Either Direction.
• Phase Shifters Can Be Controlled Electrically, Magnetically Or Mechanically.
• Can Be Analogue / Digital
• Coaxial Baluns
•A Balun Is An Electrical Device That Converts Between A Balanced Signal (Two
Signals Working Against Each Other Where Ground Is Irrelevant) & An
Unbalanced Signal (A Single Signal Working Against Ground Or Pseudo-ground).
• A Balun Can Take Many Forms & May Include Devices That Also Transform
Impedances But Need Not Do So.
• Transformer Baluns Can Also Be Used To Connect Lines Of Differing Impedance.
• The Origin Of The Word Balun Is “Balanced To Unbalanced”.