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Dr. AMBEDKAR INSTITUTE OF TECHNOLOGY
(An Autonomous Institution, Affiliated to Visveswaraya Technological University, Belagavi)
Near Jnana Bharathi Campus, Mallathahalli, Bengaluru-560056
DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING
Group Activity Report
on
β€œINTERSYMBOL INTERFERENCE,NYQUIST’S CRITERION FOR
BASEBAND,IDEAL SOLUTION FOR ZERO (ISI)”
Submitted in partial fulfillment of the curriculum
DIGITAL COMMUNICATION-18EC53
In
ELECTRONICS AND COMMUNICATION ENGINEERING
For
BACHELOR’S IN ENGINEERING
Submitted By:
AKSHATHA B R 1DA20EC009
ANUSHA CHOWDARY D 1DA20EC016
ARADHANA B 1DA20EC017
CHINMAY D 1DA20EC032
DARSHAN D 1DA21EC403
Dr. AMBEDKAR INSTITUTE OF TECHNOLOGY
(An Autonomous Institution, Affiliated to Visvesvaraya Technological University, Belagavi)
Near Jnana Bharathi Campus, Mallathahalli, Bengaluru-560056
DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING
CERTIFICATE
Certified that the group activity entitled β€œINETRSYMBOL INTERFERENCE,NYQUIST”S CRITERRION FOR
BASEBAND,IDEAL SOLUTION FOR ZERO(ISI)” carried out by Ms. ,AKSHATHA B R bearing USN
1DA20EC009, Ms.,ANUSHA CHOWDARY D bearing USN 1DA20EC016, Ms.,ARADHANA B
bearing USN 1DA20EC017, Mr. CHINMAY D, bearing USN 1DA20EC032, Mr.DARSHAN bearing
USN 1DA21EC403 a bonafide student of Dr. Ambedkar Institute of Technology, Bengaluru-560056 in
partial fulfillment of curriculum in β€œDIGITAL COMMUNICATION” in Bachelor of Engineering in
Electronics and Communication Engineering of Dr. Ambedkar Institute of Technology during the year
2022-23.
The intergroup Activity report has been approved as it satisfies the academic requirements in respect
of the subject prescribed for the said subject.
Signature of Co-ordinator
SPOORTHI P A
Assistant professor
CONTENTS :
1). INTERSYMBOL INTERFERNCE (ISI):
2).NYQUIST CRITERION FOR DISTORTIONLESS BASEBAND
(FOR BINARY TRANSMISSION):
3).IDEAL SOLUTION OR NYQUIST SDOLUTION FOR ZERO
ISI:
1).Intersymbol Interfernce (ISI):
Intersymbol Interferance:
οƒ˜ Inter symbol Interference is a form of a distortion of a signal, in
which one or more symbols interfere with subsequent signals,
causing noise or delivering a poor output.
Block diagram:
Fig: Block Diagram Of Intersymbol Interferance
Let us assume that the channel is free from noise. Let the input to the
transmitting filter be represented in time domain form as
x(t)= βˆ‘ π΄π‘˜π‘”(𝑑 βˆ’ π‘˜π‘‡π‘)
∞
π‘˜=βˆ’βˆž --> (1)
where:
ο‚· g(t) is a rectangular pulse.
ο‚· A discrete random variable taking the value of +a for symbol 1
and -a for symbol 0.
ο‚· T is the time allocated for one bit and is known as the bit
duration.
Hence, the fourier transform of equation gives
X(f)=βˆ‘ π΄π‘˜πΊ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘
∞
π‘˜=βˆ’βˆž --> (2)
Let us denote the output of the receiving filter by
Y(t)=βˆ‘ πœ‡π΄π‘˜π‘(𝑑 βˆ’ π‘˜π‘‡π‘)
∞
π‘˜=βˆ’βˆž --> (3)
Where:
p(t) is the pulse shaping function of y(t).
πœ‡ is the scaling factor.
let the FT of y(t) is
Y(f)=βˆ‘ πœ‡π΄π‘˜π‘ƒ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘
∞
π‘˜=βˆ’βˆž --> (4)
As a second step, the output of the receiving filter in frequency domain
is given by
Y(f)=X(f)Ht(f)Hc(f)Hr(f) -->(5)
Substituting equations 2 and 4 in equation 5, we get
βˆ‘ πœ‡π΄π‘˜π‘ƒ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘
∞
π‘˜=βˆ’βˆž =βˆ‘ π΄π‘˜πΊ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘
∞
π‘˜=βˆ’βˆž Ht(f)Hc(f)Hr(f)
πœ‡P(f) = G(f)Ht(f)Hc(f)Hr(f) -->(6)
Taking inverse FT on both sides of equation 6 ,we can determine the
shape of p(t).
y(t) = βˆ‘ πœ‡π΄π‘˜π‘(𝑑 βˆ’ π‘˜π‘‡π‘)
∞
π‘˜=βˆ’βˆž
Let t=iTb,
Where
i=0, +1 or -1, +2 or -2
y(iTb)=βˆ‘ πœ‡π΄π‘˜π‘(𝑖𝑇𝑏 βˆ’ π‘˜π‘‡π‘)
∞
π‘˜=βˆ’βˆž
=βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏]
∞
π‘˜=βˆ’βˆž
Therefore,
y(iTb)=πœ‡Aip(0) + βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏]
∞
π‘˜=βˆ’βˆž
π‘˜β‰ π‘–
-->(7)
Since p(0)=1,
y(iTb)=πœ‡Ai + βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏]
∞
π‘˜=βˆ’βˆž
π‘˜β‰ π‘–
--> (8)
Specification:
οƒΌ The first term on the right-hand side of equation 8 represents the
contribution of ith transmitted symbol.
οƒΌ The second term represents the unwanted contribution of all other
transmitted bits on the detection of ith transmitted bit.
οƒΌ This unwanted contribution is called intersymbol interference.
2).NYQUIST’SCRITERION FOR DISTORTIONLESS BASEBAND BINARY
TRANSMISSION (OR ZERO ISI):
οƒ˜ The pulse shaping function p(t) with Fourier transform given by
P(f),
βˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏)
∞
π‘˜=βˆ’βˆž =Tb
has,
p(iTb-Ktb)={
1, 𝑖 = π‘˜
0, 𝑖 β‰  π‘˜
This condition is known as Nyquist criterion for zero ISI.
Proof:
>>> Let us sample p(t) by using a Dirac comb with a period equal to
Tb. The process of ideal sampling may be defined mathematically by
P𝛿(t)=p(t)S𝛿(𝑑)
Applying FT on both sides,
P𝛿(f)=P𝛿(f)*S𝛿(f)
P𝛿(f)=P(f)*fsβˆ‘ 𝛿(𝑓 βˆ’ 𝑛𝑓𝑠)
∞
𝑛=βˆ’βˆž
Let fs = (1/T) = Rb
then above equation
therefore,
P𝛿(f)=P(f)*Rbβˆ‘ 𝛿(𝑓 βˆ’ 𝑛𝑅𝑏)
∞
𝑛=βˆ’βˆž
Applying the convolution property of an impulse function,
P𝛿(f)=Rbβˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏)
∞
𝑛=βˆ’βˆž -->(1)
Using the defining equation of FT,
P𝛿(f)=Rb∫ 𝑝𝛿(𝑑)
∞
βˆ’βˆž
π‘’βˆ’π‘—2πœ‹π‘“π‘‘
dt
Using,
P𝛿(t)=p(t)S𝛿(𝑑)
=𝑝(𝑑) βˆ‘ 𝛿(𝑑 βˆ’ π‘šπ‘‘π‘)
∞
π‘š=βˆ’βˆž
then,
P𝛿(t)=βˆ‘ 𝑝(π‘šπ‘‡π‘)𝛿(𝑑 βˆ’ π‘šπ‘‡π‘)
∞
π‘š=βˆ’βˆž
Then above equation becomes,
P𝛿(f)=∫ βˆ‘ [𝑝(π‘šπ‘‡π‘)𝛿(𝑑 βˆ’ π‘šπ‘‡π‘)]π‘’βˆ’π‘—2πœ‹π‘“π‘‘
∞
π‘š=βˆ’βˆž
∞
βˆ’βˆž
dt -->(2)
Let the integer, m = i-k,
Then,
i = k corresponds to m = 0, and similarly i β‰  k corresponds to m β‰  0.
Using the condition:
p[(i-kTb)] = p[mTb]
then,
p[(i-kTb)] ={
1, 𝑖 = π‘˜
0, 𝑖 β‰  π‘˜
Equation 2 bcomes,
P𝛿(f)=∫ 𝑝(0)𝛿(𝑑)
∞
βˆ’βˆž
π‘’βˆ’π‘—2πœ‹π‘“π‘‘
dt
=p(0) π‘’βˆ’π‘—2πœ‹π‘“π‘‘
|t=0 (using shifting property)
=p(0)
Since p(0) = 1, we get P𝛿(f)= 1,
οƒ˜ As a consequence of this, equation 1 gives P𝛿(f) = 1 only when
βˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏)
∞
𝑛=βˆ’βˆž =Tb
Hence the proof,
οƒ˜ Because of the significance of this theorem in baseband
transmission, the above equation or equivalently
p(iTb-Ktb)={
1, 𝑖 = π‘˜
0, 𝑖 β‰  π‘˜
Finally,it constitutes that Nyquist's criterion for distortionless
baseband transmission (zero ISI).
3).IDEAL SOLUTION OR NYQUIST SOLUTION
FOR ZERO ISI:
οƒ˜ The ISI can be minimized by controlling p(t) in time-domain and
P(f) in frequency domain.
One of the functions that gives zero ISI is
>> p(t) = sinc(2Bot) shown in fig 1
And spectrum of same signal is shown in fig 2
Where:
Bo = 1/2Tb is called Nyquist bandwidth.
β€œNyquist bandwidth is defined as the minimum transmission bandwidth
for zero ISI”.
The FT of p(t) gives
P(f)={
1
2π΅π‘œ
, |𝑓| < π΅π‘œ
0, |𝑓| > π΅π‘œ
οƒ  1
οƒ˜ The above equation implies that frequencies of absolute value
greater than half the bit rate are not needed.
Equation 1:
οƒ˜ Suggests that P(f) is the frequency response of an ideal low pass
filterand p(t) = sinc(2Bot) is the impulse response of an ideal low
pass filter.
οƒ˜ Since p(t) is a sinc function, it goes through zero at integer
multiples of Tb.
Thus if,
Tb = 1/2Bo.
οƒ˜ Then,it is clear that p(t β€” kTb) = sinc[2Bo(tβ€” kTb)] for integer
values of k will appear as shown in fig 3.
Also fig 3 implies that if y(t) is sampled at instants of time t= 0, +Tb
or –Tb , +2Tb or -2Tb….., will have zero ISI.
Fig 1: Impulse response of an ideal Low pass filter
Fig 2: Frequency response of an ideal low pass filter
Fig 3: Demonstration of Sampling Instants For Zero ISI
But,we know that
οƒ˜ The first term on the right–hand side of the above equation gives the
desired symbol.
οƒ˜ The second term represents the ISI caused by timing error βˆ†(𝑑) due to
inaccurate synchronisation of the clock in receiver sampling circuit.
Nyquist's criterion for zero intersymbol interference
Nyquist's criterion for zero intersymbol interference

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Nyquist's criterion for zero intersymbol interference

  • 1. Dr. AMBEDKAR INSTITUTE OF TECHNOLOGY (An Autonomous Institution, Affiliated to Visveswaraya Technological University, Belagavi) Near Jnana Bharathi Campus, Mallathahalli, Bengaluru-560056 DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING Group Activity Report on β€œINTERSYMBOL INTERFERENCE,NYQUIST’S CRITERION FOR BASEBAND,IDEAL SOLUTION FOR ZERO (ISI)” Submitted in partial fulfillment of the curriculum DIGITAL COMMUNICATION-18EC53 In ELECTRONICS AND COMMUNICATION ENGINEERING For BACHELOR’S IN ENGINEERING Submitted By: AKSHATHA B R 1DA20EC009 ANUSHA CHOWDARY D 1DA20EC016 ARADHANA B 1DA20EC017 CHINMAY D 1DA20EC032 DARSHAN D 1DA21EC403
  • 2. Dr. AMBEDKAR INSTITUTE OF TECHNOLOGY (An Autonomous Institution, Affiliated to Visvesvaraya Technological University, Belagavi) Near Jnana Bharathi Campus, Mallathahalli, Bengaluru-560056 DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING CERTIFICATE Certified that the group activity entitled β€œINETRSYMBOL INTERFERENCE,NYQUIST”S CRITERRION FOR BASEBAND,IDEAL SOLUTION FOR ZERO(ISI)” carried out by Ms. ,AKSHATHA B R bearing USN 1DA20EC009, Ms.,ANUSHA CHOWDARY D bearing USN 1DA20EC016, Ms.,ARADHANA B bearing USN 1DA20EC017, Mr. CHINMAY D, bearing USN 1DA20EC032, Mr.DARSHAN bearing USN 1DA21EC403 a bonafide student of Dr. Ambedkar Institute of Technology, Bengaluru-560056 in partial fulfillment of curriculum in β€œDIGITAL COMMUNICATION” in Bachelor of Engineering in Electronics and Communication Engineering of Dr. Ambedkar Institute of Technology during the year 2022-23. The intergroup Activity report has been approved as it satisfies the academic requirements in respect of the subject prescribed for the said subject. Signature of Co-ordinator SPOORTHI P A Assistant professor
  • 3. CONTENTS : 1). INTERSYMBOL INTERFERNCE (ISI): 2).NYQUIST CRITERION FOR DISTORTIONLESS BASEBAND (FOR BINARY TRANSMISSION): 3).IDEAL SOLUTION OR NYQUIST SDOLUTION FOR ZERO ISI:
  • 4. 1).Intersymbol Interfernce (ISI): Intersymbol Interferance: οƒ˜ Inter symbol Interference is a form of a distortion of a signal, in which one or more symbols interfere with subsequent signals, causing noise or delivering a poor output. Block diagram: Fig: Block Diagram Of Intersymbol Interferance Let us assume that the channel is free from noise. Let the input to the transmitting filter be represented in time domain form as x(t)= βˆ‘ π΄π‘˜π‘”(𝑑 βˆ’ π‘˜π‘‡π‘) ∞ π‘˜=βˆ’βˆž --> (1) where: ο‚· g(t) is a rectangular pulse. ο‚· A discrete random variable taking the value of +a for symbol 1 and -a for symbol 0. ο‚· T is the time allocated for one bit and is known as the bit duration.
  • 5. Hence, the fourier transform of equation gives X(f)=βˆ‘ π΄π‘˜πΊ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘ ∞ π‘˜=βˆ’βˆž --> (2) Let us denote the output of the receiving filter by Y(t)=βˆ‘ πœ‡π΄π‘˜π‘(𝑑 βˆ’ π‘˜π‘‡π‘) ∞ π‘˜=βˆ’βˆž --> (3) Where: p(t) is the pulse shaping function of y(t). πœ‡ is the scaling factor. let the FT of y(t) is Y(f)=βˆ‘ πœ‡π΄π‘˜π‘ƒ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘ ∞ π‘˜=βˆ’βˆž --> (4) As a second step, the output of the receiving filter in frequency domain is given by Y(f)=X(f)Ht(f)Hc(f)Hr(f) -->(5) Substituting equations 2 and 4 in equation 5, we get βˆ‘ πœ‡π΄π‘˜π‘ƒ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘ ∞ π‘˜=βˆ’βˆž =βˆ‘ π΄π‘˜πΊ(𝑓)π‘’βˆ’π‘—2πœ‹π‘“π‘˜π‘‡π‘ ∞ π‘˜=βˆ’βˆž Ht(f)Hc(f)Hr(f) πœ‡P(f) = G(f)Ht(f)Hc(f)Hr(f) -->(6)
  • 6. Taking inverse FT on both sides of equation 6 ,we can determine the shape of p(t). y(t) = βˆ‘ πœ‡π΄π‘˜π‘(𝑑 βˆ’ π‘˜π‘‡π‘) ∞ π‘˜=βˆ’βˆž Let t=iTb, Where i=0, +1 or -1, +2 or -2 y(iTb)=βˆ‘ πœ‡π΄π‘˜π‘(𝑖𝑇𝑏 βˆ’ π‘˜π‘‡π‘) ∞ π‘˜=βˆ’βˆž =βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏] ∞ π‘˜=βˆ’βˆž Therefore, y(iTb)=πœ‡Aip(0) + βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏] ∞ π‘˜=βˆ’βˆž π‘˜β‰ π‘– -->(7) Since p(0)=1, y(iTb)=πœ‡Ai + βˆ‘ πœ‡π΄π‘˜π‘[(𝑖 βˆ’ π‘˜)𝑇𝑏] ∞ π‘˜=βˆ’βˆž π‘˜β‰ π‘– --> (8) Specification: οƒΌ The first term on the right-hand side of equation 8 represents the contribution of ith transmitted symbol. οƒΌ The second term represents the unwanted contribution of all other transmitted bits on the detection of ith transmitted bit. οƒΌ This unwanted contribution is called intersymbol interference.
  • 7. 2).NYQUIST’SCRITERION FOR DISTORTIONLESS BASEBAND BINARY TRANSMISSION (OR ZERO ISI): οƒ˜ The pulse shaping function p(t) with Fourier transform given by P(f), βˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏) ∞ π‘˜=βˆ’βˆž =Tb has, p(iTb-Ktb)={ 1, 𝑖 = π‘˜ 0, 𝑖 β‰  π‘˜ This condition is known as Nyquist criterion for zero ISI. Proof: >>> Let us sample p(t) by using a Dirac comb with a period equal to Tb. The process of ideal sampling may be defined mathematically by P𝛿(t)=p(t)S𝛿(𝑑) Applying FT on both sides, P𝛿(f)=P𝛿(f)*S𝛿(f) P𝛿(f)=P(f)*fsβˆ‘ 𝛿(𝑓 βˆ’ 𝑛𝑓𝑠) ∞ 𝑛=βˆ’βˆž Let fs = (1/T) = Rb then above equation
  • 8. therefore, P𝛿(f)=P(f)*Rbβˆ‘ 𝛿(𝑓 βˆ’ 𝑛𝑅𝑏) ∞ 𝑛=βˆ’βˆž Applying the convolution property of an impulse function, P𝛿(f)=Rbβˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏) ∞ 𝑛=βˆ’βˆž -->(1) Using the defining equation of FT, P𝛿(f)=Rb∫ 𝑝𝛿(𝑑) ∞ βˆ’βˆž π‘’βˆ’π‘—2πœ‹π‘“π‘‘ dt Using, P𝛿(t)=p(t)S𝛿(𝑑) =𝑝(𝑑) βˆ‘ 𝛿(𝑑 βˆ’ π‘šπ‘‘π‘) ∞ π‘š=βˆ’βˆž then, P𝛿(t)=βˆ‘ 𝑝(π‘šπ‘‡π‘)𝛿(𝑑 βˆ’ π‘šπ‘‡π‘) ∞ π‘š=βˆ’βˆž Then above equation becomes, P𝛿(f)=∫ βˆ‘ [𝑝(π‘šπ‘‡π‘)𝛿(𝑑 βˆ’ π‘šπ‘‡π‘)]π‘’βˆ’π‘—2πœ‹π‘“π‘‘ ∞ π‘š=βˆ’βˆž ∞ βˆ’βˆž dt -->(2) Let the integer, m = i-k, Then, i = k corresponds to m = 0, and similarly i β‰  k corresponds to m β‰  0. Using the condition: p[(i-kTb)] = p[mTb]
  • 9. then, p[(i-kTb)] ={ 1, 𝑖 = π‘˜ 0, 𝑖 β‰  π‘˜ Equation 2 bcomes, P𝛿(f)=∫ 𝑝(0)𝛿(𝑑) ∞ βˆ’βˆž π‘’βˆ’π‘—2πœ‹π‘“π‘‘ dt =p(0) π‘’βˆ’π‘—2πœ‹π‘“π‘‘ |t=0 (using shifting property) =p(0) Since p(0) = 1, we get P𝛿(f)= 1, οƒ˜ As a consequence of this, equation 1 gives P𝛿(f) = 1 only when βˆ‘ 𝑃(𝑓 βˆ’ 𝑛𝑅𝑏) ∞ 𝑛=βˆ’βˆž =Tb Hence the proof, οƒ˜ Because of the significance of this theorem in baseband transmission, the above equation or equivalently p(iTb-Ktb)={ 1, 𝑖 = π‘˜ 0, 𝑖 β‰  π‘˜ Finally,it constitutes that Nyquist's criterion for distortionless baseband transmission (zero ISI).
  • 10. 3).IDEAL SOLUTION OR NYQUIST SOLUTION FOR ZERO ISI: οƒ˜ The ISI can be minimized by controlling p(t) in time-domain and P(f) in frequency domain. One of the functions that gives zero ISI is >> p(t) = sinc(2Bot) shown in fig 1 And spectrum of same signal is shown in fig 2 Where: Bo = 1/2Tb is called Nyquist bandwidth. β€œNyquist bandwidth is defined as the minimum transmission bandwidth for zero ISI”. The FT of p(t) gives P(f)={ 1 2π΅π‘œ , |𝑓| < π΅π‘œ 0, |𝑓| > π΅π‘œ οƒ  1 οƒ˜ The above equation implies that frequencies of absolute value greater than half the bit rate are not needed.
  • 11. Equation 1: οƒ˜ Suggests that P(f) is the frequency response of an ideal low pass filterand p(t) = sinc(2Bot) is the impulse response of an ideal low pass filter. οƒ˜ Since p(t) is a sinc function, it goes through zero at integer multiples of Tb. Thus if, Tb = 1/2Bo. οƒ˜ Then,it is clear that p(t β€” kTb) = sinc[2Bo(tβ€” kTb)] for integer values of k will appear as shown in fig 3. Also fig 3 implies that if y(t) is sampled at instants of time t= 0, +Tb or –Tb , +2Tb or -2Tb….., will have zero ISI. Fig 1: Impulse response of an ideal Low pass filter Fig 2: Frequency response of an ideal low pass filter
  • 12. Fig 3: Demonstration of Sampling Instants For Zero ISI But,we know that
  • 13. οƒ˜ The first term on the right–hand side of the above equation gives the desired symbol. οƒ˜ The second term represents the ISI caused by timing error βˆ†(𝑑) due to inaccurate synchronisation of the clock in receiver sampling circuit.