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Sampling and Hilbert Transform
Prof. Satheesh Monikandan.B
INDIAN NAVAL ACADEMY (INDIAN NAVY)
EZHIMALA
sathy24@gmail.com
101 INAC-AT19
Syllabus Contents
• Introduction to Signals and Systems
• Time-domain Analysis of LTI Systems
• Frequency-domain Representations of Signals and
Systems
• Sampling and Hilbert Transform
• Laplace Transform
Sampling

Sampling is the reduction of a CT signal to a DT
signal.

A sampler is a subsystem or operation that extracts
samples from a continuous signal.

Sampling theorem specifies the minimum-sampling
rate at which a CT signal needs to be uniformly
sampled so that the original signal can be
completely recovered or reconstructed by these
samples alone.

Sampling rate must be at least 2fmax, or twice the
highest analog frequency component.
Sampling

Nyquist rate is defined as the minimum sampling
rate required to represent complete information
about continuous signal f(t) in its sampled form, f*(t).

Sampling Rate is the number of samples per unit
time.

Higher the sample frequency obtains a signal which
is similar to original analog signal for good audio
quality.

Statement: A continuous time signal can be
represented in its samples and can be recovered
back when sampling frequency fs
is greater than or
equal to the twice the highest frequency component
of message signal.
Sampling
Sampling
Types of Sampling

Impulse Sampling
– Performed by multiplying input signal x(t) with impulse
train of period 'T'.
– Amplitude of impulse changes with respect to
amplitude of input signal x(t).

Natural Sampling

Flat Top Sampling
8
Impulse Train Sampling
We need to have a convenient way in
which to represent the sampling of a CT
signal at regular intervals
A common/useful way to do this is through
the use of a periodic impulse train
signal, p(t), multiplied by the CT signal
T is the sampling period
s=2 /T is the sampling
frequency
This is known as impulse train sampling.
Note xp(t) is still a continuous time signal





n
p
nTttp
tptxtx
)()(
)()()(

T
Types of Sampling

Natural Sampling
– Similar to impulse sampling, except the impulse train is replaced
by pulse train of period T.
– Multiplying input signal x(t) to pulse train.
Types of Sampling

Flat Top / Practical Sampling
– During transmission, noise is introduced at top of the
transmission pulse which can be easily removed if the
pulse is in the form of flat top.
– Here, the top of the samples are flat i.e. they have
constant amplitude.
Sampling Theorem
●
Processing a signal in digital domain gives several
advantages like immunity to temperature drift, accuracy,
predictability, ease of design, ease of implementation etc.
over analog domain processing.
●
Sampling operation samples the incoming signal at
regular interval called “Sampling Rate” (Ts
).
● Sampling Rate is determined by Sampling Frequency (Fs
).
●
��=1/��
●
Categories: 1. Baseband Sampling
2. Bandpass Sampling
Baseband Sampling
●
Applicable for LP signals in the baseband (useful
frequency components extending from 0Hz to some Fm
Hz).
●
Theorem: For a faithful reproduction and reconstruction of
an analog signal that is confined to a maximum frequency
Fm
, the signal should be sampled at a Sampling frequency
Fs
that is greater than or equal to twice the maximum
frequency of the signal.
●
≥�� 2��
●
Higher the sampling frequency, higher is the accuracy of
representation of the signal.
●
Higher sampling frequency implies more samples, which
implies more storage space or more memory requirements.
Baseband Sampling
●
In time domain, the process of sampling can be viewed as
multiplying the signal with a series of pulses (“pulse train)
at regular interval, Ts.
●
In frequency domain, the output of the sampling process
gives the components of Fm (original frequency content of
the signal), Fs±Fm,2Fs±Fm,3Fs±Fm,4Fs±Fm and so on.
CT Signals by its Samples
4.Sampling and Hilbert Transform
16
Sampling a CT Signal
Clearly for a finite sample period T, it is not possible to represent every
uncountable, infinite-dimensional continuous-time signal with a
countable, infinite-dimensional discrete-time signal.
In general, an infinite number of CT signals can generate a DT signal.
However, if the signal is band (frequency) limited, and the samples are
sufficiently close, it is possible to uniquely reconstruct the original CT
signal from the sampled signal.
x1(t),
x2(t),
x3(t),
x[n]
t=nT
Reconstruction of Signals from its
Samples
Aliasing
●
Effect that causes different signals to become
indistinguishable (or aliases of one another) when
sampled.
●
Sampling rate for an analog signal must be at least two
times as high as the highest frequency in the analog
signal in order to avoid aliasing.
Types of Aliasing
●
Consequence of disobeying the sampling theorem.
●
Types: 1. Harmful aliasing that distorts the signal and
must be avoided for proper representation of signal in
discrete domain. This is when Fs
<2B.
2. Useful aliasing that shifts the signal spectral bands up
and down for free to our desired frequency through careful
system design. This is employed in systems operating at
multiple clock rates.
3. Harmless aliasing that is neither good nor bad for the
system. This occurs during band-limited pulse shape
design to avoid inter-symbol interference (ISI).
4.Sampling and Hilbert Transform
4.Sampling and Hilbert Transform
4.Sampling and Hilbert Transform
DT Processing of CT Signals
4.Sampling and Hilbert Transform
DT Processing of CT Signals
Sampling of DT Signals
4.Sampling and Hilbert Transform
4.Sampling and Hilbert Transform
Hilbert Transform
The FT of the 1/πt term is –jsgn(ω)
This can be verified by the reciprocity theorem:
if f(t) and F(jω) are transform pairs, then f(jω)
and F(t) are also transform pairs
30
)t(x*
t
1
)t(X)]t(x[H


Hilbert transform
These are
FT
transform
pairs
31
Hilbert Transform Pairs
)tdcos(tAe   )tdsin(
t
Ae  
x(t) X(t)
Special interest
in dynamic
studies of all
kinds of linear
systems
Properties of Hilbert Transform
33
PROPERTIES HILBERT TRANSFORM
Energy
• The energy content of a signal is equal to the energy c
ontent of its Hilbert transform
Proof
• Using Rayleigh's theorem of the Fourier transform,
• Using the fact that |-jsgn(f)|2 = 1 except for f = 0, and t
he fact that X(f) does not contain any impulses at the
origin completes the proof





 dffXdttxEx
22
)()(







 dffXdffXfjdttxEx
222
ˆ )()()sgn()(ˆ
Examples of Hilbert Transform
Examples of Hilbert Transform
Pre-envelope
Pre-envelope
Spectrum of Pre-envelope
Complex Envelope
Real-envelope
Bandpass Signals
Bandpass Signals
Bandpass Signals
Bandpass Signals
Bandpass Signals and System Representation

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4.Sampling and Hilbert Transform

  • 1. Sampling and Hilbert Transform Prof. Satheesh Monikandan.B INDIAN NAVAL ACADEMY (INDIAN NAVY) EZHIMALA [email protected] 101 INAC-AT19
  • 2. Syllabus Contents • Introduction to Signals and Systems • Time-domain Analysis of LTI Systems • Frequency-domain Representations of Signals and Systems • Sampling and Hilbert Transform • Laplace Transform
  • 3. Sampling  Sampling is the reduction of a CT signal to a DT signal.  A sampler is a subsystem or operation that extracts samples from a continuous signal.  Sampling theorem specifies the minimum-sampling rate at which a CT signal needs to be uniformly sampled so that the original signal can be completely recovered or reconstructed by these samples alone.  Sampling rate must be at least 2fmax, or twice the highest analog frequency component.
  • 4. Sampling  Nyquist rate is defined as the minimum sampling rate required to represent complete information about continuous signal f(t) in its sampled form, f*(t).  Sampling Rate is the number of samples per unit time.  Higher the sample frequency obtains a signal which is similar to original analog signal for good audio quality.  Statement: A continuous time signal can be represented in its samples and can be recovered back when sampling frequency fs is greater than or equal to the twice the highest frequency component of message signal.
  • 7. Types of Sampling  Impulse Sampling – Performed by multiplying input signal x(t) with impulse train of period 'T'. – Amplitude of impulse changes with respect to amplitude of input signal x(t).  Natural Sampling  Flat Top Sampling
  • 8. 8 Impulse Train Sampling We need to have a convenient way in which to represent the sampling of a CT signal at regular intervals A common/useful way to do this is through the use of a periodic impulse train signal, p(t), multiplied by the CT signal T is the sampling period s=2 /T is the sampling frequency This is known as impulse train sampling. Note xp(t) is still a continuous time signal      n p nTttp tptxtx )()( )()()(  T
  • 9. Types of Sampling  Natural Sampling – Similar to impulse sampling, except the impulse train is replaced by pulse train of period T. – Multiplying input signal x(t) to pulse train.
  • 10. Types of Sampling  Flat Top / Practical Sampling – During transmission, noise is introduced at top of the transmission pulse which can be easily removed if the pulse is in the form of flat top. – Here, the top of the samples are flat i.e. they have constant amplitude.
  • 11. Sampling Theorem ● Processing a signal in digital domain gives several advantages like immunity to temperature drift, accuracy, predictability, ease of design, ease of implementation etc. over analog domain processing. ● Sampling operation samples the incoming signal at regular interval called “Sampling Rate” (Ts ). ● Sampling Rate is determined by Sampling Frequency (Fs ). ● ��=1/�� ● Categories: 1. Baseband Sampling 2. Bandpass Sampling
  • 12. Baseband Sampling ● Applicable for LP signals in the baseband (useful frequency components extending from 0Hz to some Fm Hz). ● Theorem: For a faithful reproduction and reconstruction of an analog signal that is confined to a maximum frequency Fm , the signal should be sampled at a Sampling frequency Fs that is greater than or equal to twice the maximum frequency of the signal. ● ≥�� 2�� ● Higher the sampling frequency, higher is the accuracy of representation of the signal. ● Higher sampling frequency implies more samples, which implies more storage space or more memory requirements.
  • 13. Baseband Sampling ● In time domain, the process of sampling can be viewed as multiplying the signal with a series of pulses (“pulse train) at regular interval, Ts. ● In frequency domain, the output of the sampling process gives the components of Fm (original frequency content of the signal), Fs±Fm,2Fs±Fm,3Fs±Fm,4Fs±Fm and so on.
  • 14. CT Signals by its Samples
  • 16. 16 Sampling a CT Signal Clearly for a finite sample period T, it is not possible to represent every uncountable, infinite-dimensional continuous-time signal with a countable, infinite-dimensional discrete-time signal. In general, an infinite number of CT signals can generate a DT signal. However, if the signal is band (frequency) limited, and the samples are sufficiently close, it is possible to uniquely reconstruct the original CT signal from the sampled signal. x1(t), x2(t), x3(t), x[n] t=nT
  • 17. Reconstruction of Signals from its Samples
  • 18. Aliasing ● Effect that causes different signals to become indistinguishable (or aliases of one another) when sampled. ● Sampling rate for an analog signal must be at least two times as high as the highest frequency in the analog signal in order to avoid aliasing.
  • 19. Types of Aliasing ● Consequence of disobeying the sampling theorem. ● Types: 1. Harmful aliasing that distorts the signal and must be avoided for proper representation of signal in discrete domain. This is when Fs <2B. 2. Useful aliasing that shifts the signal spectral bands up and down for free to our desired frequency through careful system design. This is employed in systems operating at multiple clock rates. 3. Harmless aliasing that is neither good nor bad for the system. This occurs during band-limited pulse shape design to avoid inter-symbol interference (ISI).
  • 23. DT Processing of CT Signals
  • 25. DT Processing of CT Signals
  • 26. Sampling of DT Signals
  • 30. The FT of the 1/πt term is –jsgn(ω) This can be verified by the reciprocity theorem: if f(t) and F(jω) are transform pairs, then f(jω) and F(t) are also transform pairs 30 )t(x* t 1 )t(X)]t(x[H   Hilbert transform These are FT transform pairs
  • 31. 31 Hilbert Transform Pairs )tdcos(tAe   )tdsin( t Ae   x(t) X(t) Special interest in dynamic studies of all kinds of linear systems
  • 33. 33 PROPERTIES HILBERT TRANSFORM Energy • The energy content of a signal is equal to the energy c ontent of its Hilbert transform Proof • Using Rayleigh's theorem of the Fourier transform, • Using the fact that |-jsgn(f)|2 = 1 except for f = 0, and t he fact that X(f) does not contain any impulses at the origin completes the proof       dffXdttxEx 22 )()(         dffXdffXfjdttxEx 222 ˆ )()()sgn()(ˆ
  • 34. Examples of Hilbert Transform
  • 35. Examples of Hilbert Transform
  • 45. Bandpass Signals and System Representation