AM Modulators: ReviewEE 179, Lecture 9, Handout #14

Multiplier modulator (perhaps using variable gain amplifier)

Nonlinear modulator, using square-law device

Switching modulator effectively multiplies signal by square wave

Multiplying a signal by a sinusoid shifts the frequency band.

Super-heterodyning: mix = c + I .

Sub-heterodyning: mix = c I .

EE 179, April 18, 2014 Lecture 9, Page 1

Demodulation of DSB-SC Signals

Both modulator and demodulator use a multiplier by carrier signal.

Modulator uses bandpass filter

Demodulator uses lowpass filter

The carrier used by the demodulator must be in phase with the transmittercarrier (taking into account transmission delay).

Such a receiver is called synchronous, coherent, homodyne.

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50.5

0

0.5e2(t) = x(t) * sin(2*pi*fc*t)

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 50.1

0.05

0

0.05

0.1e2(t) lowpass filtered

homo = same, dyne = power (irregular suffix)

EE 179, April 18, 2014 Lecture 9, Page 2

Demodulation of DSB-SC Signals (cont.)

The phase of the carrier in the received signal must be extracted.

Suppose that the signal is not ideal (frequency is shifted):

r(t) = Acm(t t0) cos(

(c +)(t t0))

= Acm(t t0) cos(

(c +)t d)

where d = (c +)t0.

The receiver has a local oscillator that must be adjusted to stay in phasewith the received signal.

A voltage-controlled oscillator (VCO) that is controlled by a phase-lockedloop (PLL) is commonly used.

If the goal is cheap receivers, then we can eliminate the PLL bytransmitting the carrier signal along with the modulated message.

AM(t) = A cosct+m(t) cos ct = (A+m(t)) cos ct

The tone A cosct contains the desired carrier in correct phase.

EE 179, April 18, 2014 Lecture 9, Page 3

AM Modulation

AM modulation is a form of amplitude modulation. For ka > 0,

s(t) = (Ac +m(t)) cos(ct) = Ac(1 + kam(t)) cos(2fct)

We need bandwidth of m(t) fc and modulation index ka < 1.

Spectrum of modulated signal:

S(f) = 12Ac

(

(f + fc) + (f fc))

+

1

2kaAc

(

M(f + fc) +M(f fc))

EE 179, April 18, 2014 Lecture 9, Page 4

DSB-SC vs. AM

DSB-SC modulated signals undergo phase reversal when m(t) changes sign.It is difficult to extract carrier from received signal.

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

1

0.5

0

0.5

1

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

1

0.5

0

0.5

1

EE 179, April 18, 2014 Lecture 9, Page 5

DSB-SC vs. AM (cont.)

In AM, the carrier signal is modulated by Ac +m(t) = Ac(1 + kam(t)).Examples: ka = 1 and ka = 0.5.

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 22

1

0

1

2

ka = 1

0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 21.5

1

0.5

0

0.5

1

1.5

ka = 0.5

EE 179, April 18, 2014 Lecture 9, Page 6

AM Signal and Its Envelope

EE 179, April 18, 2014 Lecture 9, Page 7

Envelope Detection of AM Signals

The term detection means extracting signal from received data. In somecases it means demodulation.

Suppose that a signal x(t) can be written as

x(t) = E(t) cos ct ,

where E(t) varies slowly compared to the carrier cosct.

Then |E(t)| is called the envelope of x(t).

For envelope detection to work, we need

fc bandwidth of m(t)

Otherwise positive and negative spectral components overlap.

A+m(t) 0

Otherwise phase reversals occur when A+m(t) < 0.

EE 179, April 18, 2014 Lecture 9, Page 8

Message Signal Peak and Offset

The requirement for envelope detection,

A m(t)

is equivalent toA mmin = minm(t)

Typically m(t) has zero offset, i.e., minm(t) = maxm(t) = mp.

The modulation index of the modulated signal is defined by

=mpA

Larger modulation index reduces power but makes demodulation harder.

Broadcast AM stations use modulation index close to 1. Input signals arecontrolled using automatic gain control (AGC).

Zero offset is not the same as zero DC value.

EE 179, April 18, 2014 Lecture 9, Page 9

Modulation Index Example

For tone modulation,m(t) = b cosmt

the message peak is b and = b/A.

AM(t) = (A+ b cosmt) cos ct = A(1 + cosmt) cosct

EE 179, April 18, 2014 Lecture 9, Page 10

Modulation and Demodulation of AM Signals

Modulation: use DSB-SC modulator with A cosct added to signal.

Demodulation: we could use coherent DSB-SC demodulator.

But this approach fails to use the carrier component.

EE 179, April 18, 2014 Lecture 9, Page 11

Envelope Detector for AM

EE 179, April 18, 2014 Lecture 9, Page 12

AM Demodulation: Rectifier + Lowpass Filter

Diodes were the first semiconductor electronic devices. The discovery of crystals rectifying abilities was made by German physicist

Ferdinand Braun in 1874. The first semiconductor diodes, called cats whisker diodes, developed around 1906, were made of

mineral crystals such as galena. Today most diodes are made of silicon, but other semiconductors such as germanium are

sometimes used.

EE 179, April 18, 2014 Lecture 9, Page 13

AM Demodulation Experiment

m(t) = cos 2t , fc = 10 , h(t) =1

RCet/RCu(t)

0 0.5 1 1.5 22

1

0

1

2

0 0.5 1 1.5 20

0.5

1

1.5

2

0 0.5 1 1.5 20

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0 0.5 1 1.5 20.4

0.3

0.2

0.1

0

0.1

0.2

0.3

EE 179, April 18, 2014 Lecture 9, Page 14

Cats Whiskers (Crystal) Radio

This radio was powered only by received radio energy.

The point-contact semiconductor detector was subsequently resurrected around WorldWar II because of the military requirement for microwave radar detectors.

EE 179, April 18, 2014 Lecture 9, Page 15

Corncob Pipe Radio

EE 179, April 18, 2014 Lecture 9, Page 16

Single Sideband (SSB)

DSB-SC is spectrally inefficient. It uses twice the bandwidth of themessage.

The signal can be reconstructed from either the upper sideband (USB) orlower sideband.

SSB transmits a bandpass filtered version of the modulated signal.

EE 179, April 18, 2014 Lecture 9, Page 17

Single Sideband (cont.)

EE 179, April 18, 2014 Lecture 9, Page 18

Single Sideband (cont.)

EE 179, April 18, 2014 Lecture 9, Page 19

Single Sideband Modulation and Demodulation

SSB can be transmitted using a DSB-SC modulator with a narrowerbandpass filter. For USB, center frequency is

fc = fc +1

2B

and cutoff frequency is B/2.

The bandfilter must roll off quickly to eliminate unwanted contributionsfrom the other sideband.

Message frequencies near 0 will be affected by the nonideal filter.

SSB demodulation can use a DSB-SC demodulator with no change.

The input to the lowpass filter is different from that of DSB-SC.

EE 179, April 18, 2014 Lecture 9, Page 20