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ECE 8443 – Pattern Recognition
EE 3512 – Signals: Continuous and Discrete
• Objectives:
Generalized Fourier Transform
Analog Modulation
Amplitude Modulation
Angle Modulation
Demodulation and Demultiplexing
• Resources:
Wiki: The Fourier Transform
Celier: Generalized Fourier Transform
MIT 6.003: Lecture 15
Wiki: Amplitude Modulation
RE: AM Demodulation
Wiki: Electromagnetic Spectrum
Wiki: 700 MHz Auction
LECTURE 11: SIGNAL MODULATION
AND DEMODULATION
URL:
EE 3512: Lecture 12, Slide 1
• Consider a DC or constant signal:
• Compute its Fourier Transform:
• Unfortunately, the limit is not finite, and the integral does not converge.
• Consider an alternate approach based on an impulse function:
• Apply the duality property:
• This is known as the Generalized Fourier transform. It allows us to extend the
Fourier transform to some additional useful signals such as periodic signals:
The Fourier transform of a periodic signal is a train of impulse functions (and
is a line spectrum).
Generalized Fourier Transform
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EE 3512: Lecture 12, Slide 2
• The electromagnetic spectrum is the most expensive “real estate” in the
world. Hence, we would like to make as efficient use of it as possible (e.g.,
time and frequency domain multiplexing).
• It is more efficient (e.g., less power for a given SNR) to transmit signals at
higher frequencies.
• Modulation: send multiple signals
through the same medium (e.g. air,
cables, fibers) by simply shifting
them to different places in the
spectrum.
• Amplitude Modulation: carry the
information in the amplitude of the
signal; use a sinusoidal carrier, c(t).
• Angle Modulation: alternate approach in which the signal is carried in the
frequency or phase of the carrier signal (frequency and phase modulation).
• Many other forms of modulation including pulse-amplitude modulation (PAM),
pulse-width modulation (PWM), code division multiple access (CDMA) and
spread spectrum. These techniques are typically studied in an introductory
course in communications theory.
The Concept of Modulation
EE 3512: Lecture 12, Slide 3
• Modulation:
Amplitude Modulation Using a Complex Exponential
• Demodulation:
EE 3512: Lecture 12, Slide 4
Amplitude Modulation Using a Sinusoid
EE 3512: Lecture 12, Slide 5
Synchronous Demodulation of Sinusoidal AM
• Assumptions:
  = 0 (for now),
 Local oscillator is
synchronized with the
carrier.
In practice, synchronization
is achieved using a phase-
locked loop (PLL).
EE 3512: Lecture 12, Slide 6
• We can easily derive the properties of the demodulated signal:
• The low-pass filter removes the high-frequency replica of x(t), leaving only the
“baseband” component.
• Suppose there is a phase difference between the transmitter and the receiver:
The mismatch in phase appears as a scale factor that can be ignored.
• If there is a time-varying phase difference (due to drift):
If the phase difference varies slowly in time, the net result is simply a time-
varying amplitude change, which distorts the signal (slightly).
• What happens if the receiver is exactly 90 out of phase?
Synchronous Demodulation in the Time Domain
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EE 3512: Lecture 12, Slide 7
• Consider the spectrum of our modulation signal:
Asynchronous Demodulation
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Problems if the transmitter and receiver are exactly 90 out of phase.
• Alternative: Asynchronous
modulation includes the
carrier in the output and
ensures the envelope
of the modulated carrier
contains the information.
• The carrier must be much
higher in frequency than
the signal: M
c 
 
EE 3512: Lecture 12, Slide 8
Implementation of an Asynchronous Demodulator
• AM modulation was popular because of the ease with which it could be
demodulated:
• However, for this to work, the envelope function must be positive (A+x(t) > 0).
• We pay a price in efficiency: more power must be used to guarantee this
condition is true.
EE 3512: Lecture 12, Slide 9
Double-Sideband Vs. Single-Sideband Modulation
• Since x(t) and y(t) are real, from
conjugate symmetry, both lower
sideband (LSB) and upper sideband
(USB) signals carry exactly the
same information.
• Double-sideband (DSB) occupies
2M bandwidth in  > 0, even though
all the information is contained in M.
• Single-sideband (SSB) occupies M
bandwidth in  > 0.
• Of course, SSB requires slightly
more complicated hardware, so it
was originally only used in
applications where bandwidth was
very limited (e.g., transcontinental
telephone lines).
• Analog television signals, which are
being obsoleted in February 2009,
use a variant of SSB.
EE 3512: Lecture 12, Slide 10
Single-Sideband Modulation
EE 3512: Lecture 12, Slide 11
Frequency Division Multiplexing
• Used in many communications
systems including broadcast radio
and cell phones.
EE 3512: Lecture 12, Slide 12
• Recall to recover one channel (e.g., radio station) from a multiplexed signal,
we must first bandpass filter the multiplexed signal, and then demodulate it:
• However, the channels must not overlap for this to work. Fortunately, this is
an important role played by the FCC (in the U.S.) – management of the
electromagnetic spectrum.
• It is difficult to design a highly selective bandpass filter with a tunable center
frequency.
• A better solution is the superheterodyne receiver: downconvert all channels
to a common intermediate frequency. “The advantage to this method is that
most of the radio's signal path has to be sensitive to only a narrow range of
frequencies. Only the front end (the part before the frequency converter
stage) needs to be sensitive to a wide frequency range.” (Wiki)
Demultiplexing and Demodulation
EE 3512: Lecture 12, Slide 13
• Principle: Down convert the received signal from c to IF using a coarse
tunable bandpass filter. Use a sharp, fixed bandpass filter at IF to demodulate
the remaining signal and remove remnants of the other channels that pass
through the initial coarse filter.
The Superheterodyne Receiver
AM Band: 535 – 1605 kHz
FCC-mandated
IF Frequency: 455 kHz
EE 3512: Lecture 12, Slide 14
Summary
• Introduced the Generalized Fourier transform.
• Demonstrated its use on periodic signals (e.g., Fourier series).
• Introduced the concept of modulation.
• Discussed amplitude and angle modulation.
• Discussed modulation and demodulation of AM signals.
• Introduced both a synchronous and asynchronous approach to demodulation.
• Introduced techniques used in a variety of common communications systems
including single-sideband and double-sideband modulation, and frequency
division multiplexing.

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lecture_11.pptx

  • 1. ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete • Objectives: Generalized Fourier Transform Analog Modulation Amplitude Modulation Angle Modulation Demodulation and Demultiplexing • Resources: Wiki: The Fourier Transform Celier: Generalized Fourier Transform MIT 6.003: Lecture 15 Wiki: Amplitude Modulation RE: AM Demodulation Wiki: Electromagnetic Spectrum Wiki: 700 MHz Auction LECTURE 11: SIGNAL MODULATION AND DEMODULATION URL:
  • 2. EE 3512: Lecture 12, Slide 1 • Consider a DC or constant signal: • Compute its Fourier Transform: • Unfortunately, the limit is not finite, and the integral does not converge. • Consider an alternate approach based on an impulse function: • Apply the duality property: • This is known as the Generalized Fourier transform. It allows us to extend the Fourier transform to some additional useful signals such as periodic signals: The Fourier transform of a periodic signal is a train of impulse functions (and is a line spectrum). Generalized Fourier Transform   1 ) ( 0 , 1 ) ( , 0 0 ) (         t d t t         F               k k k t jkω k t jω ) δ(ω-kω c ω X e c t x ) πδ(ω-ω e 0 0 2 ) ( 2 0 0       t - , x(t) 1   2 / 2 / 2 / 2 / 2 / 2 / 1 lim 1 lim lim ) 1 ( ) ( T j T j T T T t j T T -T t j T - t j e e j e j dt e dt e j X                                     2 ) ( 1 ) (         t x t t x F
  • 3. EE 3512: Lecture 12, Slide 2 • The electromagnetic spectrum is the most expensive “real estate” in the world. Hence, we would like to make as efficient use of it as possible (e.g., time and frequency domain multiplexing). • It is more efficient (e.g., less power for a given SNR) to transmit signals at higher frequencies. • Modulation: send multiple signals through the same medium (e.g. air, cables, fibers) by simply shifting them to different places in the spectrum. • Amplitude Modulation: carry the information in the amplitude of the signal; use a sinusoidal carrier, c(t). • Angle Modulation: alternate approach in which the signal is carried in the frequency or phase of the carrier signal (frequency and phase modulation). • Many other forms of modulation including pulse-amplitude modulation (PAM), pulse-width modulation (PWM), code division multiple access (CDMA) and spread spectrum. These techniques are typically studied in an introductory course in communications theory. The Concept of Modulation
  • 4. EE 3512: Lecture 12, Slide 3 • Modulation: Amplitude Modulation Using a Complex Exponential • Demodulation:
  • 5. EE 3512: Lecture 12, Slide 4 Amplitude Modulation Using a Sinusoid
  • 6. EE 3512: Lecture 12, Slide 5 Synchronous Demodulation of Sinusoidal AM • Assumptions:   = 0 (for now),  Local oscillator is synchronized with the carrier. In practice, synchronization is achieved using a phase- locked loop (PLL).
  • 7. EE 3512: Lecture 12, Slide 6 • We can easily derive the properties of the demodulated signal: • The low-pass filter removes the high-frequency replica of x(t), leaving only the “baseband” component. • Suppose there is a phase difference between the transmitter and the receiver: The mismatch in phase appears as a scale factor that can be ignored. • If there is a time-varying phase difference (due to drift): If the phase difference varies slowly in time, the net result is simply a time- varying amplitude change, which distorts the signal (slightly). • What happens if the receiver is exactly 90 out of phase? Synchronous Demodulation in the Time Domain           ) 2 cos( 2 1 2 1 ) ( ) ( cos ) ( ) cos( ) ( ) ( 2 t t x t t x t t y t w c c c                 ) 2 cos( 2 1 ) cos( 2 1 ) ( ) cos( ) cos( ) ( ) cos( ) ( ) (         t t x t t t x t t y t w c c c c          )) ( 2 cos( 2 1 )) ( cos( 2 1 ) ( ) ( t t t t x t w c   
  • 8. EE 3512: Lecture 12, Slide 7 • Consider the spectrum of our modulation signal: Asynchronous Demodulation     c j c j t j j t j j c e e e e e e t c c                           2 1 2 1 ) cos( Problems if the transmitter and receiver are exactly 90 out of phase. • Alternative: Asynchronous modulation includes the carrier in the output and ensures the envelope of the modulated carrier contains the information. • The carrier must be much higher in frequency than the signal: M c   
  • 9. EE 3512: Lecture 12, Slide 8 Implementation of an Asynchronous Demodulator • AM modulation was popular because of the ease with which it could be demodulated: • However, for this to work, the envelope function must be positive (A+x(t) > 0). • We pay a price in efficiency: more power must be used to guarantee this condition is true.
  • 10. EE 3512: Lecture 12, Slide 9 Double-Sideband Vs. Single-Sideband Modulation • Since x(t) and y(t) are real, from conjugate symmetry, both lower sideband (LSB) and upper sideband (USB) signals carry exactly the same information. • Double-sideband (DSB) occupies 2M bandwidth in  > 0, even though all the information is contained in M. • Single-sideband (SSB) occupies M bandwidth in  > 0. • Of course, SSB requires slightly more complicated hardware, so it was originally only used in applications where bandwidth was very limited (e.g., transcontinental telephone lines). • Analog television signals, which are being obsoleted in February 2009, use a variant of SSB.
  • 11. EE 3512: Lecture 12, Slide 10 Single-Sideband Modulation
  • 12. EE 3512: Lecture 12, Slide 11 Frequency Division Multiplexing • Used in many communications systems including broadcast radio and cell phones.
  • 13. EE 3512: Lecture 12, Slide 12 • Recall to recover one channel (e.g., radio station) from a multiplexed signal, we must first bandpass filter the multiplexed signal, and then demodulate it: • However, the channels must not overlap for this to work. Fortunately, this is an important role played by the FCC (in the U.S.) – management of the electromagnetic spectrum. • It is difficult to design a highly selective bandpass filter with a tunable center frequency. • A better solution is the superheterodyne receiver: downconvert all channels to a common intermediate frequency. “The advantage to this method is that most of the radio's signal path has to be sensitive to only a narrow range of frequencies. Only the front end (the part before the frequency converter stage) needs to be sensitive to a wide frequency range.” (Wiki) Demultiplexing and Demodulation
  • 14. EE 3512: Lecture 12, Slide 13 • Principle: Down convert the received signal from c to IF using a coarse tunable bandpass filter. Use a sharp, fixed bandpass filter at IF to demodulate the remaining signal and remove remnants of the other channels that pass through the initial coarse filter. The Superheterodyne Receiver AM Band: 535 – 1605 kHz FCC-mandated IF Frequency: 455 kHz
  • 15. EE 3512: Lecture 12, Slide 14 Summary • Introduced the Generalized Fourier transform. • Demonstrated its use on periodic signals (e.g., Fourier series). • Introduced the concept of modulation. • Discussed amplitude and angle modulation. • Discussed modulation and demodulation of AM signals. • Introduced both a synchronous and asynchronous approach to demodulation. • Introduced techniques used in a variety of common communications systems including single-sideband and double-sideband modulation, and frequency division multiplexing.

Editor's Notes

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