lecture 18-19: linear modulations aliazam abbasfar

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Lecture 18-19: Linear Modulations Aliazam Abbasfar

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Page 1: Lecture 18-19: Linear Modulations Aliazam Abbasfar

Lecture 18-19: Linear Modulations

Aliazam Abbasfar

Page 2: Lecture 18-19: Linear Modulations Aliazam Abbasfar

OutlineAmplitude Modulation

DSB/AM/SSB/VSB

Page 3: Lecture 18-19: Linear Modulations Aliazam Abbasfar

DSB modulation Double sideband modulation

xo(t) = Ac x(t) cos(ct)

Lowpass signal xI(t) = x(t), xQ(t) = 0 A(t), (t)= ?

Xo(t) = ½ Ac [ X(f-fc) + X(f+fc) ] Symmetric spectrum around fc Bandwidth : 2W Upper and lower sidebands

Transmitted power GXo(t) = ¼ Ac

2 [ GX(f-fc) + GX(f+fc) ] PXo = ½ Ac

2 PX = Pc PX

Pc = Unmodulated carrier power

Page 4: Lecture 18-19: Linear Modulations Aliazam Abbasfar

DSB demodulation Coherent demodulation

y(t) = 2A cos(ct) xo(t) = A Ac x(t) + A Ac x(t) cos(2ct) Filter out x(t) cos(2ct) by a LPF

z(t) = A Ac x(t) = K x(t)

Coherent demodulation Phase and frequency of the carrier is known

Phase offset z(t) = K cos() x(t) Lower gain

Frequency offset (f) z(t) = K cos(f t) x(t) Distortion

Page 5: Lecture 18-19: Linear Modulations Aliazam Abbasfar

AM modulation Amplitude modulation

xo(t) = Ac (1+x(t)) cos(ct) : modulation index (1+x(t)) > 0 (<= 1 if |x(t)|<1) Signal DC value = 0

Lowpass signal xI(t) = 1+x(t), xQ(t) = 0 A(t) = 1+x(t), (t)= 0

Xo(t) = ½Ac [(f-fc) + (f+fc) ] + ½ Ac [ X(f-fc) + X(f+fc) ]

Symmetric spectrum around fc Additional tone at fc

Transmitted power PXo = ½ Ac

2 (1+) PX = Pc (1+ PX)

Efficiency: AM = PX / (1+ PX) <= 50%

Page 6: Lecture 18-19: Linear Modulations Aliazam Abbasfar

AM demodulationEnvelope detection

Very simple circuits

Using non-linear circuitsHalf-wave/full-wave rectifier

Good for radio broadcastExpensive TX (only 1)Cheap RXs (many)

Page 7: Lecture 18-19: Linear Modulations Aliazam Abbasfar

SSB modulation Single sideband modulation

Send only one of the sidebands LSSB or USSB Filter out other sideband Signal usually has a DC hole

Xo(f) = X(f-fc)u(f-fc) ; f>0 Bandwidth : W Spectrally efficient Not symmetric

Transmitted power PXo = ½ PDSB = ½ Pc

PX

Good for FDM Low bandwidth Low power

Page 8: Lecture 18-19: Linear Modulations Aliazam Abbasfar

SSB modulation - 2Lowpass signal

xI(t) = ½ x(t), xQ(t) = ½ x(t)

IQ modulator

Weaver modulator

Page 9: Lecture 18-19: Linear Modulations Aliazam Abbasfar

SSB demodulation Coherent demodulation

y(t) = 2A cos(ct) xo(t) = ½ A Ac x(t) [1+cos(2ct)] - ½ A Ac x(t) sin(2ct) Filter out high freq. terms by a LPF

z(t) = ½ A Ac x(t) = K x(t)

Phase offset z(t) = K cos() x(t) + K sin() x(t) Lower gain + distortion

Frequency offset (f) z(t) = K cos(f t) x(t) + K sin(f t) x(t) Distortion

IQ demodulator Multiply with both cos(ct) and sin(ct) Complex demodulator No distortion

Page 10: Lecture 18-19: Linear Modulations Aliazam Abbasfar

VSB modulation Vestigial sideband modulation

Send one of the sidebands and and part of other Filter out part of other sideband Keeps signal DC components

Xo(f) = X(f-fc) H(f) ; f>0 Bandwidth > W Not symmetric

Transmitted power PSSB < PXo < PDSB

Used in video broadcast Low bandwidth Keeps low frequencies Low power

Page 11: Lecture 18-19: Linear Modulations Aliazam Abbasfar

VSB modulationH(f) has odd symmetry around fc

H(f) = (1 +j HVSB )/2

HVSB is a realizable filter

Lowpass signalxI(t)= ½ x(t), xQ(t) = ½ x(t)*hVSB(t)

IQ modulator

Page 12: Lecture 18-19: Linear Modulations Aliazam Abbasfar

VSB demodulation Coherent demodulation

y(t) = ½ A Ac x(t) [1+cos(2ct)] - ½ A Ac x’(t) sin(2ct) Filter out high frequency terms by a LPF

z(t) = ½ A Ac x(t) = K x(t)

Phase offset z(t) = K cos() x(t) + K sin() x’(t) Lower gain + distortion

Frequency offset (f) z(t) = K cos(f t) x(t) + K sin(f t) x(t) Distortion

Use IQ demodulator

Page 13: Lecture 18-19: Linear Modulations Aliazam Abbasfar

ReadingCarlson Ch. 4.2, 4.3 and 4.4

Proakis 2.5, 3.1, 3.2