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Ch 4 Amplitude Modulations and Demodulations

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ENGR 4323/5323 Digital and Analog Communication. Ch 4 Amplitude Modulations and Demodulations. Engineering and Physics University of Central Oklahoma Dr. Mohamed Bingabr. Chapter Outline. Baseband vs. Carrier Communications Double-Sideband Amplitude Modulations (DSB) - PowerPoint PPT Presentation
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Ch 4 Amplitude Modulations and Demodulations ENGR 4323/5323 igital and Analog Communication Engineering and Physics University of Central Oklahoma Dr. Mohamed Bingabr
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Page 1: Ch 4 Amplitude Modulations and Demodulations

Ch 4Amplitude Modulations and Demodulations

ENGR 4323/5323Digital and Analog Communication

Engineering and PhysicsUniversity of Central Oklahoma

Dr. Mohamed Bingabr

Page 2: Ch 4 Amplitude Modulations and Demodulations

Chapter Outline

β€’ Baseband vs. Carrier Communicationsβ€’ Double-Sideband Amplitude Modulations (DSB)β€’ Amplitude Modulation (AM)β€’ Vestigial Sideband Amplitude Modulations (VSB)β€’ Local Carrier Synchronizationβ€’ Frequency Division Multiplexing (FDM)β€’ Phase-Locked Loop and Applicationsβ€’ NTSC Television Broadcasting System

Page 3: Ch 4 Amplitude Modulations and Demodulations

Baseband Vs. Carrier Communicationsβ€’ Baseband signals produced by various information

sources and its original spectrum is not modified.

β€’ Baseband Communications: Baseband signals are transmitted without any modifications of its spectrum. By conversion process (Modulation), such signals are modified to facilitate transmission.

β€’ Carrier Communication: Communication that uses modulation to shift the frequency spectrum of a signal.

β€’ Purpose of Modulation:– Ease of radiation.

– Reduce noise and interference.

– Multiplexing or transmission of several messages over a single channel.

Page 4: Ch 4 Amplitude Modulations and Demodulations

Type of Modulationβ€’ Analog Modulation: The original analog signal modulates

the one of the following parameters of a sinusoidal carrier of high frequency:

β€’ Amplitude Modulation (AM)

β€’ Frequency Modulation (FM)

β€’ Phase Modulation (PM)Angle Modulation

Analog modulation shifts the spectrum of the original signal to be centered around the carrier frequency, Ο‰c.

s(𝑑)=𝐴 (𝑑 ) cos [ πœ”π‘ 𝑑+βˆ… (𝑑 ) ]

Page 5: Ch 4 Amplitude Modulations and Demodulations

Type of Modulationβ€’ Pulse Modulation: The original analog signal modulates

the following parameters of a digital pulse train:β€’ Pulse Amplitude Modulation (PAM)

β€’ Pulse Width Modulation (PWM)

β€’ Pulse Position Modulation (PPM)

β€’ Pulse Code Modulation (PCM)

β€’ Delta Modulation (DM)

In pulse modulation the spectrum of the original signal is not shifted. Pulse modulation is a digital pulse coding schemes used to describe the analog signal.

Page 6: Ch 4 Amplitude Modulations and Demodulations

Double-Sideband Amplitude Modulation

π‘š(𝑑)⇔

𝑀 ( 𝑓 )

Double-sideband, suppressed-carrier (DSB-SC) modulation

π‘š (𝑑 ) cos2 πœ‹ 𝑓 𝑐𝑑⇔

12 [ 𝑀 ( 𝑓 + 𝑓 𝑐)+𝑀 ( 𝑓 βˆ’ 𝑓 𝑐 ) ]

Page 7: Ch 4 Amplitude Modulations and Demodulations

Demodulation

Demodulator: recovering the message signal at the receiver from the modulated signal.

𝑒 (𝑑 )=π‘š (𝑑 )cos2 πœ”π‘π‘‘

𝐸 ( 𝑓 )=12 𝑀 ( 𝑓 )+ 1

4 [ 𝑀 ( 𝑓 +2 𝑓 𝑐 )+𝑀 ( 𝑓 βˆ’ 2 𝑓 𝑐 ) ]

Page 8: Ch 4 Amplitude Modulations and Demodulations

Type of Modulators

Multiplier Modulators: A variable gain amplifier in which the gain parameter (such as the of transistor) is controlled by the message signal m(t) and the input is the carrier signal.

Nonlinear Modulators: Nonlinear devices such as diode or transistors are used to output modulated signal.

𝑦 (𝑑 )=π‘Žπ‘₯ (𝑑 )+𝑏 x2(𝑑)

]-]

𝑧 (𝑑 )=2π‘Ž .π‘š (𝑑 )+4𝑏 .π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘Single balanced modulator because one of the input does not appear at the output z(t)

Page 9: Ch 4 Amplitude Modulations and Demodulations

Type of Modulators

Switching Modulators: Switching is equivalent to multiplying the message signal m(t) by periodic pulses w(t) with fundamental period Tc.

Page 10: Ch 4 Amplitude Modulations and Demodulations

Type of Modulators

w (𝑑)=βˆ‘π‘›=0

∞

𝐢𝑛 cos (π‘›πœ”π‘ 𝑑+πœƒπ‘› )

w (𝑑 )π‘š (𝑑 )=βˆ‘π‘›=0

∞

πΆπ‘›π‘š (𝑑 )cos (𝑛 πœ”π‘ 𝑑+πœƒπ‘›)

w (𝑑 )π‘š (𝑑 )= 12

π‘š (𝑑 )+ 2πœ‹ [π‘š (𝑑 )π‘π‘œπ‘ πœ”π‘π‘‘ βˆ’ 1

3π‘š (𝑑 ) π‘π‘œπ‘  3πœ”π‘π‘‘+ 1

5π‘š (𝑑 ) π‘π‘œπ‘ 5 πœ”π‘ 𝑑 βˆ’β€¦ ]

Switching Modulators

Page 11: Ch 4 Amplitude Modulations and Demodulations

Circuit of Switching ModulatorsDiode-bridge electronic switch:

Shunt-bridge diode modulator

Diode-bridge electronic switch

Series-bridge diode modulator

When Vc > Vd - all diodes are open and matched- D1 = Vc – Va D2 = Vc – Vb

- D1 = D2

- Va = Vb

Page 12: Ch 4 Amplitude Modulations and Demodulations

Circuit of Switching ModulatorsRing Modulator

During Positive cycle of carrier: - D1 & D3 Conducts - a connected to c & b connected to d - output proportional to m(t)

During Negative cycle of carrier: - D2 & D4 Conducts - a connected to d & b connected to c - output proportional to -m(t)

Double Balanced Modulator

w (𝑑 )π‘š (𝑑 )= 4πœ‹ [π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘ βˆ’ 1

3π‘š (𝑑 ) π‘π‘œπ‘ 3 πœ”π‘π‘‘+ 1

5π‘š (𝑑 )π‘π‘œπ‘  5 πœ”π‘ 𝑑 βˆ’β€¦]

Page 13: Ch 4 Amplitude Modulations and Demodulations

Demodulation of DSB-SC Signals

For demodulation, the receiver must generate a carrier that is synchronous (coherent) in phase and in frequency with incoming carrier.

- The received signal might suffer from some unknown frequency or phase shift.

π‘Ÿ (𝑑 )=π΄π‘π‘š (𝑑 βˆ’ 𝑑0 )π‘π‘œπ‘  [ (πœ”π‘+βˆ†πœ” ) (𝑑 βˆ’ 𝑑0 ) ]

- The receiver must be sophisticated to generate a local oscillator cos[(Ο‰c+Δω)t-ΞΈd)]purely from the received signal r(t).

Challenge of coherent demodulation for DSB-SC signals

- Amplitude modulation (AM) that transmit the carrier with the modulated signal will simplify the job of the receiver.

Page 14: Ch 4 Amplitude Modulations and Demodulations

Amplitude Modulation (AM)Transmit the modulated signal with the carrier signal to simplify the complexity of the receivers.

πœ‘π΄π‘€ (𝑑 )= π΄π‘π‘œπ‘ πœ”π‘π‘‘+π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘ 𝑑

+

[ 𝐴+π‘š (𝑑 ) ]β‰₯ 0 for all t

Condition for demodulation using envelope detection

Modulation index

0β‰€πœ‡β‰€ 1

Page 15: Ch 4 Amplitude Modulations and Demodulations

Example: Tone Modulation

Sketch φAM(t) for modulation indices of ¡= 0.5 and ¡ = 1, when m(t)=b cosωmt.

πœ‡=π‘šπ‘

𝐴

Page 16: Ch 4 Amplitude Modulations and Demodulations

Sideband and Carrier Power

carrierπœ‘π΄π‘€ (𝑑 )= π΄π‘π‘œπ‘ πœ”π‘π‘‘+π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘ 𝑑

sidebands

𝑃𝑐=𝐴2

2Power of the carrier (wasted):

Power of the sidebands: 𝑃𝑠=12~π‘š2(𝑑 )

Power efficiency:

πœ‚=useful   powertotal   power

=𝑃𝑠

𝑃𝑐+ 𝑃𝑠=

~π‘š2(𝑑)

𝐴2+~π‘š2(𝑑 )

100 %

Page 17: Ch 4 Amplitude Modulations and Demodulations

Example

Determine Ξ· and the percentage of the total power carried by the sidebands of the AM wave for tone modulation when (a) Β΅ =1 (b) Β΅ = 0.5 (c) Β΅ = 0.3

πœ‚=~π‘š2(𝑑)

𝐴2+~π‘š2(𝑑)

100 % πœ‡=π‘šπ‘

𝐴

Page 18: Ch 4 Amplitude Modulations and Demodulations

Demodulation of AM Signals

Rectifier

π‘£π‘Ÿ (𝑑 )= {[ 𝐴+π‘š(𝑑) ]π‘π‘œπ‘ πœ”π‘π‘‘ }𝑀 (𝑑 )

ΒΏ [ 𝐴+π‘š (𝑑)] π‘π‘œπ‘ πœ”π‘ 𝑑 [ 12+ 2

πœ‹ (π‘π‘œπ‘ πœ”π‘π‘‘ βˆ’ 13

π‘π‘œπ‘  3πœ”π‘π‘‘+ 15

π‘π‘œπ‘ 5 πœ”π‘π‘‘ βˆ’ …) ]ΒΏ

1πœ‹ [ 𝐴+π‘š(𝑑) ]+other   terms   of   higher   frequencies

Page 19: Ch 4 Amplitude Modulations and Demodulations

Demodulation of AM Signals

Envelope Detector

1/πœ”π‘ β‰ͺ𝑅𝐢<1 /(2 πœ‹ 𝐡) 2 πœ‹ 𝐡<1/𝑅𝐢<πœ”π‘

or

Page 20: Ch 4 Amplitude Modulations and Demodulations

Bandwidth-Efficient Amplitude Modulations

Single-Sideband (SSB) modulation, which remove either the LSB or the USB so that for one message signal m(t), there is only a bandwidth of B Hz.

Quadrature Amplitude (QAM) modulation, which utilize spectral redundancy by sending two messages over the same of 2B Hz.

The bandwidth of Amplitude Modulation is 2B Hz.

Page 21: Ch 4 Amplitude Modulations and Demodulations

Amplitude Modulation: Single Sideband (SSB)

Single-Sideband (SSB) modulation, which remove either the LSB or the USB. Hilbert transform is used to remove the LSB or USB.

Page 22: Ch 4 Amplitude Modulations and Demodulations

Hilbert Transform

Hilbert Transformh(t)H(f)

m(t) mh(t)

M(f) Mh(f)

𝐻 ( 𝑓 )=βˆ’ 𝑗 𝑠𝑔𝑛( 𝑓 ) h (𝑑 )= 1πœ‹ 𝑑

π‘šh (𝑑 )=π‘š (𝑑 ) βˆ—h (𝑑)

𝑀 h ( 𝑓 )=βˆ’ 𝑗 𝑠𝑔𝑛 ( 𝑓 ) 𝑀 ( 𝑓 )

𝐻 ( 𝑓 )={1.π‘’βˆ’ 𝑗 πœ‹

2 =βˆ’ 𝑗 𝑓 >0

1.𝑒𝑗 πœ‹2 = 𝑗 𝑓 <0

Hilbert transform is an ideal phase shifter that shifts the phase of every positive spectral component by -Ο€/2.

Page 23: Ch 4 Amplitude Modulations and Demodulations

Time Domain Representation of SSB Signals

𝑀+ΒΏ ( 𝑓 )=𝑀 ( 𝑓 ). 𝑒 ( 𝑓 )=𝑀 ( 𝑓 ) 1

2 [1+𝑠𝑔𝑛(𝑓 ) ] ΒΏ

𝑀+ΒΏ ( 𝑓 )=1

2 [ 𝑀 (𝑓 )+ 𝑗 𝑀 h ( 𝑓 )] ΒΏ

π‘€βˆ’ ( 𝑓 )=𝑀 ( 𝑓 ) .𝑒 (βˆ’ 𝑓 )=𝑀 ( 𝑓 ) 12 [1βˆ’π‘ π‘”π‘›( 𝑓 ) ]

Ξ¦π‘ˆπ‘†π΅ ( 𝑓 )=𝑀+ΒΏ ( 𝑓 βˆ’ 𝑓 𝑐 )+𝑀 βˆ’ ( 𝑓 + 𝑓 𝑐 )ΒΏ

Ξ¦π‘ˆπ‘†π΅ ( 𝑓 )=12 [ 𝑀 ( 𝑓 βˆ’ 𝑓 𝑐 )+ 𝑀 ( 𝑓 + 𝑓 𝑐) ]

βˆ’ 𝑗2 [ 𝑀 h ( 𝑓 + 𝑓 𝑐 ) βˆ’π‘€ h ( 𝑓 βˆ’ 𝑓 𝑐 ) ]

πœ‘π‘ˆπ‘†π΅ (𝑑 )=π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘ 𝑑 βˆ’π‘šh (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘πœ‘πΏπ‘†π΅ (𝑑 )=π‘š (𝑑 )π‘π‘œπ‘  πœ”π‘ 𝑑+π‘šh (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘

Page 24: Ch 4 Amplitude Modulations and Demodulations

Demodulation of SSB-SC

πœ‘π‘†π‘†π΅ (𝑑 ) 2cos πœ”π‘π‘‘=[π‘š (𝑑 ) π‘π‘œπ‘ πœ”ΒΏΒΏ 𝑐𝑑 βˆ“π‘šh (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘ ]2cos πœ”π‘π‘‘ ΒΏ

ΒΏπ‘š (𝑑 ) [1+π‘π‘œπ‘ 2πœ”ΒΏΒΏπ‘ 𝑑 ]βˆ“π‘šh (𝑑 ) 𝑠𝑖𝑛 2πœ”π‘ 𝑑 ΒΏ

ΒΏπ‘š (𝑑 )+[π‘š (𝑑 ) π‘π‘œπ‘ 2 πœ”ΒΏΒΏ 𝑐𝑑 βˆ“π‘šh (𝑑 ) 𝑠𝑖𝑛 2πœ”π‘ 𝑑 ]ΒΏ

These terms can be filtered out by using low-pass filter

Page 25: Ch 4 Amplitude Modulations and Demodulations

Tone Modulation Example: SSBFind for the simple case of a tone modulation, that is, a modulating signal that is sinusoid m(t) = cosωmt. Also demonstrate the coherent demodulation of the SSB signal.

Page 26: Ch 4 Amplitude Modulations and Demodulations

SSB Modulation Systems

Common Methods to Generate SSB 1- Phase Shift 2- Selective-filtering 3- Weaver’s

These modulation methods require that the baseband signal spectrum have little power near the origin, because ideal filters and Hilbert transformer are not realizable.

Speech signal has no DC and little power near the origin. For speech recognition we can eliminate all frequency components below 300 Hz.

Page 27: Ch 4 Amplitude Modulations and Demodulations

SSB Phase Shift Modulation System

πœ‘π‘ˆπ‘†π΅ (𝑑 )=π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘ 𝑑 βˆ’π‘šh (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘

Page 28: Ch 4 Amplitude Modulations and Demodulations

SSB Selective-Filtering Modulation SystemThe signal is passed through a sharp cutoff filter to eliminate the undesired sideband. Low-pass filter to eliminate the USB spectrum, and high-pass filter to eliminate the LSB spectrum.

Weaver’s method modulates the signal to a low carrier frequency first and filter out the undesired SSB, after that it modulate it again to the desired high carrier frequency.

Page 29: Ch 4 Amplitude Modulations and Demodulations

Demodulation of SSB Signal with a Carrier

Where E(t) the envelope of

πœ‘π‘†π‘†π΅+𝐢 (𝑑 )=π΄π‘π‘œπ‘  πœ”π‘ 𝑑+[π‘š (𝑑 )π‘π‘œπ‘ πœ”π‘π‘‘+π‘šh (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘ ]

πœ‘π‘†π‘†π΅+𝐢 (𝑑 )=[𝐴+π‘š (𝑑 ) ]π‘π‘œπ‘ πœ”π‘π‘‘+π‘šh (𝑑 ) 𝑠𝑖𝑛 πœ”π‘π‘‘

πœ‘π‘†π‘†π΅+𝐢 (𝑑 )=𝐸 (𝑑 ) cos (πœ”ΒΏΒΏπ‘π‘‘+πœƒ)ΒΏ

𝐸 (𝑑 )= {[ 𝐴+π‘š (𝑑 )]2+π‘šh2(𝑑)}1/2

𝐸 (𝑑 )=A [1+ 2π‘š(𝑑)𝐴 +

π‘š2(𝑑)𝐴2 +

π‘šh2(𝑑)𝐴2 ]

1 /2

𝐸 (𝑑 )β‰ˆ 𝐴 [1+2π‘š (𝑑)

𝐴 ]1/2

If A>> |m(t)|

𝐸 (𝑑 )β‰ˆ 𝐴 [1+π‘š(𝑑 )

𝐴 ] 𝐸 (𝑑 )β‰ˆ 𝐴+π‘š(𝑑 )

Use Taylor expansion and discard higher order

Page 30: Ch 4 Amplitude Modulations and Demodulations

Quadrature Amplitude Modulation (QAM)It is difficult to generate accurately SSB-SC and requires large power A >>|m(t)|, so QAM offers an attractive alternative.

QAM operates by transmitting two DSB signals via carrier of the same frequency but in phase quadrature.

Page 31: Ch 4 Amplitude Modulations and Demodulations

Quadrature Amplitude Modulation (QAM)

πœ‘π‘„π΄π‘€ (𝑑 )=π‘š1 (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘+π‘š2 (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘π‘₯1 (𝑑 )=2πœ‘π‘„π΄π‘€ (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘

ΒΏ2 [π‘š1 (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘+π‘š2 (𝑑 ) π‘ π‘–π‘›πœ”π‘ 𝑑  ]π‘π‘œπ‘  πœ”π‘π‘‘ΒΏπ‘š1 (𝑑 )+π‘š1 (𝑑 ) π‘π‘œπ‘  2πœ”π‘π‘‘+π‘š2 (𝑑 ) 𝑠𝑖𝑛2πœ”π‘π‘‘

π‘₯2 (𝑑 )=π‘š2 (𝑑 ) βˆ’π‘š2 (𝑑 ) π‘π‘œπ‘  2πœ”π‘ 𝑑+π‘š1 (𝑑 ) 𝑠𝑖𝑛2πœ”π‘π‘‘

In-phase channel

Quadrature channel

Page 32: Ch 4 Amplitude Modulations and Demodulations

Quadrature Amplitude Modulation (QAM)

π‘₯1 (𝑑 )=2[π‘š1 (𝑑 ) π‘π‘œπ‘ πœ”π‘ 𝑑+π‘š2 (𝑑 ) π‘ π‘–π‘›πœ”π‘π‘‘  ]cos (πœ”ΒΏΒΏ 𝑐𝑑+πœƒ)ΒΏ

Drawback of QAM An error in the phase or the frequency of the carrier at the demodulator will result in loss and Cochannel interference.

The output of the low-pass filter:

If ΞΈ is small then the distortion is tolerable for some applications.

Page 33: Ch 4 Amplitude Modulations and Demodulations

Amplitude Modulations: Vestigial Sideband (VSB)

VSB signals are relatively easy to generate, and their bandwidth is typically 25% greater than that of SSB signals.

Φ𝑉 𝑆𝐡 ( 𝑓 )= [𝑀 ( 𝑓 + 𝑓 𝑐 )+𝑀 ( 𝑓 βˆ’ 𝑓 𝑐 ) ] 𝐻 𝑖( 𝑓 )

Page 34: Ch 4 Amplitude Modulations and Demodulations

Demodulation of Vestigial Sideband (VSB)

-----------> 1Φ𝑉 𝑆𝐡 ( 𝑓 )= [𝑀 ( 𝑓 + 𝑓 𝑐 )+𝑀 ( 𝑓 βˆ’ 𝑓 𝑐 ) ] 𝐻 𝑖( 𝑓 )

𝑀 ( 𝑓 )=[ Φ𝑉 𝑆𝐡 ( 𝑓 + 𝑓 𝑐 )+Φ𝑉 𝑆𝐡 ( 𝑓 βˆ’ 𝑓 𝑐) ] π»π‘œ( 𝑓 )

Substitute equation 1 and filter out spectra at Β± 2fc

M

π»π‘œ ( 𝑓 )= 1𝐻 𝑖 ( 𝑓 + 𝑓 𝑐 )+𝐻 𝑖 ( 𝑓 βˆ’ 𝑓 𝑐) |f|B

Page 35: Ch 4 Amplitude Modulations and Demodulations

Demodulation of Vestigial Sideband (VSB)

π»π‘œ ( 𝑓 )= 1𝐻 𝑖 ( 𝑓 + 𝑓 𝑐 )+𝐻 𝑖 ( 𝑓 βˆ’ 𝑓 𝑐)

For envelope demodulation, VSB+C require larger carrier than DSB+C but less than SSB+C.

The carrier frequency of a certain VSB signals is fc= 20 kHz, and the baseband signal bandwidth is 6 kHz. The VSB shaping filter Hi(f)at the transmitter is shown below, find the filter H0(f)at the receiver for distortionless reception.

Page 36: Ch 4 Amplitude Modulations and Demodulations

Use of VSB in Broadcast Television

TV Broadcasting- Bandwidth 4.5 MHz- Has sizable power in the low-frequency region- Envelope detector is used instead of synchronous to reduce

the cost of the receiver.

BW for SSB = 4.5 MHzBW for DSB = 9 MHzBW for VSB = 6 MHz

Page 37: Ch 4 Amplitude Modulations and Demodulations

Frequency Division Multiplexing (FDM)

Signal multiplexing allows the transmission of several signals on the same channel.

Time Division Multiplexing (TDM): several signals time-share the same channel.

Frequency Division Multiplexing (FDM): several signals share the band of a channel.

Telephone Analog L-carrier hierarchyUsing SSB+C

48 kHz

240 kHz

2400 kHz600 voice channel

Page 38: Ch 4 Amplitude Modulations and Demodulations

Frequency Division Multiplexing (FDM)

Page 39: Ch 4 Amplitude Modulations and Demodulations

Local Carrier Synchronization

It is difficult for the receiver to generate the carrier in synchronization with the received carrier because of frequency shift due to Doppler effect and phase shift due to traveling.

π‘Ÿ (𝑑)=π‘š (𝑑 ) π‘π‘œπ‘  [ (πœ”π‘+βˆ†πœ” ) 𝑑+𝛿 ] βˆ’π‘šh (𝑑 ) 𝑠𝑖𝑛 [ (πœ”π‘+βˆ†πœ” )𝑑+𝛿 ]

Doppler Effect βˆ† πœ”π‘šπ‘Žπ‘₯=𝑣𝑒

𝑐 πœ”π‘ ve is the speed of receiver

Time Delay 𝛿=βˆ’ (πœ”π‘+βˆ† πœ” ) 𝑑/𝑐

Two ways to recover the incoming carrier at the receiver: - The transmitter transmits a pilot (sinusoid) signal - The receiver uses nonlinear device to generate a separate carrier component to be extracted by narrow bandpass filters.

dTraveled distance by radio wave

Page 40: Ch 4 Amplitude Modulations and Demodulations

Phase-Locked Loop and Applications (PLL)

Typically used to track the phase and the frequency of the carrier component of an incoming signal.

Application of PLL1) Synchronous demodulation2) Timing recovery in digital receiver

sin [ (πœ”π‘+βˆ†πœ” ) 𝑑+(πœƒπ‘–+βˆ†πœƒ ) ]sin [πœ”π‘π‘‘+ ( βˆ†πœ”π‘‘+πœƒπ‘–+βˆ† πœƒ ) ]sin [ πœ”π‘π‘‘+πœƒπ‘– (𝑑 )]

Remember frequency or phase shift can be represented as phase shift:

Page 41: Ch 4 Amplitude Modulations and Demodulations

Phase-Locked Loop and Applications (PLL)

A sin [ πœ”π‘ 𝑑+πœƒπ‘– (𝑑 ) ]βˆ—2B cos [πœ”π‘π‘‘+πœƒ0 (𝑑 ) ]𝐴𝐡¿ ΒΏ

Output of the multiplier

eo(t)depends on the difference between the received phase ΞΈi and the generated ΞΈoat the receiver. eo(t) will control the oscillation of the voltage controlled oscillator to phase locked with ΞΈi.

Output of the loop filter 𝑒0 (𝑑 )= 𝐴𝐡sin (πœƒπ‘– βˆ’πœƒπ‘œ )

Instantaneous frequency of VCO = Ο‰ c  +  ceo ( t )  =  Ο‰ c+ οΏ½Μ‡οΏ½π‘œ(𝑑)

Page 42: Ch 4 Amplitude Modulations and Demodulations

Carrier Acquisition in DSB-SC

π‘₯ (𝑑 )=[π‘š (𝑑 ) π‘π‘œπ‘ πœ”π‘π‘‘ ]2

Signal-Squaring Method

12 π‘š2 (𝑑 )=π‘˜+βˆ… (𝑑)

π‘₯ (𝑑 )=12 π‘š2 (𝑑 )+ 1

2 π‘š2 (𝑑 ) π‘π‘œπ‘  2πœ”π‘π‘‘

Page 43: Ch 4 Amplitude Modulations and Demodulations

Carrier Acquisition in DSB-SC

Costas Method

π‘š (𝑑 ) π‘π‘œπ‘  (πœƒπ‘– βˆ’πœƒπ‘œ )+π‘š (𝑑 ) cos (2πœ”π‘+πœƒπ‘–+πœƒπ‘œ)

Page 44: Ch 4 Amplitude Modulations and Demodulations

NTSC Television Broadcasting System

NTSC: National Television System CommitteeThe information of the entire picture is transmitted by transmitting an electrical signal proportion to the brightness level of the pixels taken in a certain sequence.

The optical system of the television camera tube generates a focused image on a photo cathode, which eventually produces electrically charged image on another surface (target mosaic).

Charge Coupled Device

Electron gun scans the target mosaic.

Page 45: Ch 4 Amplitude Modulations and Demodulations

NTSC Television Broadcasting System

NTSC: National Television System Committee

Few pixelsLow ResolutionLess data

More pixelsHigh ResolutionMore data

Page 46: Ch 4 Amplitude Modulations and Demodulations

NTSC Television Broadcasting System

Scanning Pattern

Line scanning

Frame scanning

Time to scan one horizontal line: 53.5 Β΅sTime to fly back to scan next line (blank no data): 10 Β΅sNumber of lines per frame 525 line/frameTime to scan one frame: 15.71 msTime to fly back to scan next frame (blank): 0.95 msTotal number of frames per second: 60 frame/sec

Page 47: Ch 4 Amplitude Modulations and Demodulations

NTSC Television Broadcasting System

Scanning Pattern

DSBVSB+C

white: more positive charge

Page 48: Ch 4 Amplitude Modulations and Demodulations

NTSC Television Standard and Bandwidth

525 lines per frame495 lines per frame are active scanning40 frames per second needed to avoid flicker and jerky motion. 30 frames per second to conserve bandwidth in NTSC standardFrame scanned twice and in each scan only 247.5 line is used.First scan is the solid lines and the second scan is dashed lines.

BandwidthIf frame consist of 525 by 525 pixels and 30 frames per second, thenBW = 525 X 525 X 30 = 8.27 X 106 pixels (pulse) per second. = 4.135 MHz

Page 49: Ch 4 Amplitude Modulations and Demodulations

Television Transmitter

Page 50: Ch 4 Amplitude Modulations and Demodulations

Television Receiver

Page 51: Ch 4 Amplitude Modulations and Demodulations

Compatible Color Television (CCTV)

π‘šπΏ (𝑑 )=0.30π‘šπ‘Ÿ (𝑑 )+0.59π‘šπ‘” (𝑑 )+0.11π‘šπ‘ (𝑑 )π‘šπΌ (𝑑 )=0.60π‘šπ‘Ÿ (𝑑 )+0.28π‘šπ‘” (𝑑 )βˆ’ 0.32π‘šπ‘ (𝑑 )π‘šπ‘„ (𝑑 )=0.21π‘šπ‘Ÿ (𝑑 )βˆ’ 0.52π‘šπ‘” (𝑑 )+0.31π‘šπ‘ (𝑑 )

Luminance

Chrominance

Page 52: Ch 4 Amplitude Modulations and Demodulations

Color Television Receiver (CCTV)


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