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Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal AM 3. Demodulation of Sinusoidal AM 4. Single-Sideband (SSB) AM 5. Frequency-Division Multiplexing 6. Superheterodyne Receivers

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Page 1: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Signals and SystemsFall 2003

Lecture #1528 October 2003

1. Complex Exponential Amplitude Modulation2. Sinusoidal AM3. Demodulation of Sinusoidal AM4. Single-Sideband (SSB) AM5. Frequency-Division Multiplexing6. Superheterodyne Receivers

Page 2: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

The Concept of Modulation

Why?• More efficient to transmit E&M signals at higher frequencies• Transmitting multiple signals through the same medium using

different carriers• Transmitting through “channels” with limited passbands• Others...

• Many methods• Focus here for the most part on Amplitude Modulation (AM)

How?

Transmitted Signalx(t)

Carrier Signal

Page 3: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Amplitude Modulation (AM) of a Complex Exponential Carrier

Page 4: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Demodulation of Complex Exponential AM

Corresponds to two separate modulation channels (quadratures) with carriers 90o out of phase

Page 5: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Sinusoidal AM

Drawn assuming ωc > ωM

Page 6: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Synchronous Demodulation of Sinusoidal AM

Suppose θ = 0 for now,⇒ Local oscillator is in phase with the carrier.

Page 7: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Synchronous Demodulation in the Time Domain

Two special cases:1) θ = π/2, the local oscillator is 90o out of phase with the carrier,

⇒ r(t) = 0, signal unrecoverable.

Now suppose there is a phase difference, i.e. θ ≠ 0, then

2) θ = θ(t) — slowly varying with time, ⇒ r(t) ≅ cos[θ(t)] • x(t), ⇒ time-varying “gain”.

Page 8: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Synchronous Demodulation (with phase error) in the Frequency Domain

Again, the low-frequency signal (ω < ωM) = 0 when θ = π/2.

Demodulating signal –has phase difference θ w.r.t.

the modulating signal

Page 9: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Alternative: Asynchronous Demodulation

• Assume ωc >> ωM, so signal envelope looks like x(t)• Add same carrier with amplitude A to signal

A = 0 ⇒ DSB/SC (Double Side Band, Suppressed Carrier)A > 0 ⇒ DSB/WC (Double Side Band, With Carrier)

Time Domain

Frequency Domain

Page 10: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Asynchronous Demodulation (continued)Envelope Detector

Disadvantages of asynchronous demodulation:— Requires extra transmitting power [Acosωct]2 to make sure

A + x(t) > 0 ⇒ Maximum power efficiency = 1/3 (P8.27)

In order for it to function properly, the envelope function must be positive for all time, i.e. A + x(t) > 0 for all t.

Demo: Envelope detection for asynchronous demodulation.

Advantages of asynchronous demodulation:— Simpler in design and implementation.

Page 11: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Double-Sideband (DSB) and Single-Sideband (SSB) AM

Since x(t) and y(t) are real, from conjugate symmetry both LSBand USB signals carry exactly the same information.

DSB, occupies 2ωM bandwidth in ω > 0.

Each sideband approach only occupies ωMbandwidth in ω > 0.

USB

LSB

Page 12: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Single Sideband Modulation

Can also get SSB/SCor SSB/WC

Page 13: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Frequency-Division Multiplexing (FDM)(Examples: Radio-station signals and analog cell phones)

air

All the channels can share the same medium.

Page 14: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

FDM in the Frequency-Domain

“Baseband” signals

Channel a

Channel b

Channel c

Multiplexed signals

Page 15: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

Demultiplexing and Demodulation

• Channels must not overlap ⇒ Bandwidth Allocation

• It is difficult (and expensive) to design a highly selective bandpass filter with a tunable center frequency

• Solution – Superheterodyne Receivers

ωa needs to be tunable

Page 16: Signals and Systemsdspace.mit.edu/bitstream/handle/1721.1/60965/6-003...Signals and Systems Fall 2003 Lecture #15 28 October 2003 1. Complex Exponential Amplitude Modulation 2. Sinusoidal

The Superheterodyne Receiver

Operation principle:— Down convert from ωc to ωIF, and use a coarse tunable BPF for the front end.— Use a sharp-cutoff fixed BPF at ωIF to get rid of other signals.

AM, ωc

2π= 535 −1605 kHz — RF

FCC: ω IF

2π= 455 kHz — IF