Amplitude Modulation.ppt 6qj29

Analogue Modulation – Amplitude Modulation Consider a 'sine wave' carrier.

vc(t) = Vc cos(ct), peak amplitude = Vc, carrier frequency c radians per second. Since c = 2fc, frequency = fc Hz where fc = 1/T. Amplitude Modulation AM In AM, the modulating signal (the message signal) m(t) is 'impressed' on to the amplitude of the carrier.

Message Signal m(t) In general m(t) will be a band of signals, for example speech or video signals. A notation or convention to show baseband signals for m(t) is shown below

Message Signal m(t) In general m(t) will be band limited. Consider for example, speech via a microphone. The envelope of the spectrum would be like:

Contoh

Contoh

Message Signal m(t)

In order to make the analysis and indeed the testing of AM systems easier, it is common to make m(t) a test signal, i.e. a signal with a constant amplitude and frequency given by

m t

V m cos

m

t

Schematic Diagram for Amplitude Modulation

VDC is a variable voltage, which can be set between 0 Volts and +V Volts. This schematic diagram is very useful; from this all the important properties of AM and various forms of AM may be derived.

Equations for AM

From the diagram v s  t  = VDC + m t   cos ωc t  where VDC is the DC voltage that can be varied. The equation is in the form Amp cos ct and we may 'see' that the amplitude is a function of m(t) and VDC. Expanding the equation we get:

v s  t  = VDC cos ωc t  + m t  cos ωc t 

Equations for AM Now let m(t) = Vm cos mt, i.e. a 'test' signal,

cosAcosB =

Using the trig identity we have

v s  t  = VDC cos ωc t  +

v s  t  = VDC cos ωc t  +Vm cos ωm t  cos ωc t 

1  cos A + B  + cos A  B   2

Vm V cos  ωc + ωm  t  + m cos  ωc  ωm  t  2 2

Components:

Carrier upper sideband USB

lower sideband LSB

Amplitude:

VDC

Vm/2

Vm/2

Frequency:

c fc

c + m fc + fm

c – m fc + f m

This equation represents Double Amplitude Modulation – DSBAM

Spectrum and Waveforms

The following diagrams represent the spectrum of the input signals, namely (VDC + m(t)), with m(t) = Vm cos mt, and the carrier cos ct and corresponding waveforms.

Spectrum and Waveforms The above are input signals. The diagram below shows the spectrum and corresponding waveform of the output signal, given by

vs t

V DC cos

c

t

Vm 2

cos

c

m

t

Vm 2

cos

c

m

t

Spektrum 2 sisi

Double Sideband AM, DSBAM The component at the output at the carrier frequency fc is shown as a broken line with amplitude VDC to show that the amplitude depends on VDC. The structure of the waveform will now be considered in a little more detail. Waveforms Consider again the diagram

VDC is a variable DC offset added to the message; m(t) = Vm cos mt

Double Sideband AM, DSBAM

This is multiplied by a carrier, cos ct. We effectively multiply (VDC + m(t)) waveform by +1, -1, +1, -1, ... The product gives the output signal v s t

V DC m t cos

c

t

Double Sideband AM, DSBAM

Modulation Depth Consider again the equation

v s  t  = VDC + Vm cos ωm t   cos ωc t  , which may be written as

  V v s  t  = VDC  1+ m cos ωm t   cos ωc t  VDC  

The ratio is

Vm Vm Modulation Depth m = defined as the modulation depth, m, i.e. VDC VDC

From an oscilloscope display the modulation depth for Double Sideband AM may be determined as follows:

Modulation Depth 2 2Emax = maximum peak-to-peak of waveform 2Emin = minimum peak-to-peak of waveform

2 E max  2 E min Modulation Depth m = 2 E max + 2 E min This may be shown to equal

Vm as follows: VDC

2 E max 2 V DC V m m=

2 E min 2 V DC V m

2VDC + 2Vm  2VDC + 2Vm 4Vm Vm = = VDC 2VDC + 2Vm + 2VDC  2Vm 4VDC

Double Sideband Modulation 'Types' There are 3 main types of DSB •

Double Sideband Amplitude Modulation, DSBAM – with carrier

•

Double Sideband Diminished (Pilot) Carrier, DSB Dim C

•

Double Sideband Suppressed Carrier, DSBSC

•

The type of modulation is determined by the modulation depth, which for a fixed m(t) depends on the DC offset, VDC. Note, when a modulator is set up, VDC is fixed at a particular value. In the following illustrations we will have a fixed message, Vm cos mt and vary VDC to obtain different types of Double Sideband modulation.

Graphical Representation of Modulation Depth and Modulation Types.

Graphical Representation of Modulation Depth and Modulation Types 2.

Graphical Representation of Modulation Depth and Modulation Types 3 Note then that VDC may be set to give the modulation depth and modulation type. DSBAM VDC >> Vm, m  1 DSB Dim C 0 < VDC < Vm, m > 1 (1 < m < ) DSBSC VDC = 0, m =  The spectrum for the 3 main types of amplitude modulation are summarised

Bandwidth Requirement for DSBAM In general, the message signal m(t) will not be a single 'sine' wave, but a band of frequencies  extending up to B Hz as shown

– the 'shape' is used for convenience to distinguish low frequencies from high frequencies in the baseband signal.

Bandwidth Requirement for DSBAM Amplitude Modulation is a linear process, hence the principle of superposition applies. The output spectrum may be found by considering each component cosine wave in m(t) separately and summing at the output. Note: • • • • • • •

Frequency inversion of the LSB the modulation process has effectively shifted or frequency translated the baseband m(t) message signal to USB and LSB signals centred on the carrier frequency fc the USB is a frequency shifted replica of m(t) the LSB is a frequency inverted/shifted replica of m(t) both sidebands each contain the same message information, hence either the LSB or USB could be removed (because they both contain the same information) the bandwidth of the DSB signal is 2B Hz, i.e. twice the highest frequency in the baseband signal, m(t) The process of multiplying (or mixing) to give frequency translation (or up-conversion) forms the basis of radio transmitters and frequency division multiplexing which will be discussed later.

Power Considerations in DSBAM 2

 V pk 

ing that Normalised Average Power = (VRMS)2 =  



2

we may tabulate for AM components as follows: V V v s  t  = VDC cos ωc t  + m cos  ωc + ωm  t  + m cos  ωc  ωm  t  2 2 Component

Carrier

USB

Amplitude pk

VDC

Vm 2

Power

Power

VDC 2

VDC 2

2

2

2

 Vm  



 2 2 2

LSB

Vm 2 V = m 8

m VDC 8

2

2

2



 Vm  

 2 2

V = m 8

m 2VDC 8

2

2

Total Power PT = Carrier Power Pc + PUSB + PLSB

Power Considerations in DSBAM From this we may write two equivalent equations for the total power PT, in a DSBAM signal 2

2

2

2

V V V V V PT = DC + m + m = DC + m 2 8 8 2 4 The carrier power

V Pc = DC 2

2

i.e.

2

2

2

and

VDC m 2VDC m 2VDC PT = + + 2 8 8

m2 m2 PT = Pc + Pc + Pc 4 4

or

2



m2 PT = Pc  1 + 2 

  

Either of these forms may be useful. Since both USB and LSB contain the same information a useful ratio which shows the proportion of 'useful' power to total power is

m2 Pc PUSB 4 = PT  m2 Pc  1 + 2  



m2 = 4 + 2m 2 

Power Considerations in DSBAM For DSBAM (m  1), allowing for m(t) with a dynamic range, the average value of m may be assumed to be m = 0.3 m2  0.3 = 0.0215 = 4 + 2m 2 4 + 2 0.3 2 2

Hence,

Hence, on average only about 2.15% of the total power transmitted may be regarded as 'useful' power. ( 95.7% of the total power is in the carrier!)

m2 1 = Even for a maximum modulation depth of m = 1 for DSBAM the ratio 4 + 2m 2 6 i.e. only 1/6th of the total power is 'useful' power (with 2/3 of the total power in the carrier).

Grafik

Example Suppose you have a portable (for example you carry it in your ' back pack') DSBAM transmitter which needs to transmit an average power of 10 Watts in each sideband when modulation depth m = 0.3. Assume that the transmitter is powered by a 12 Volt battery. The total power will be

m2 m2 PT = Pc + Pc + Pc 4 4 m2 410 40 where Pc = 444.44 Watts = 10 Watts, i.e. Pc = = 2 2 4 m  0.3 Hence, total power PT = 444.44 + 10 + 10 = 464.44 Watts. Hence, battery current (assuming ideal transmitter) = Power / Volts = i.e. a large and heavy 12 Volt battery.

464.44 amps! 12

Suppose we could remove one sideband and the carrier, power transmitted would be 10 Watts, i.e. 0.833 amps from a 12 Volt battery, which is more reasonable for a portable radio transmitter.

Single Sideband Amplitude Modulation One method to produce signal sideband (SSB) amplitude modulation is to produce DSBAM, and the DSBAM signal through a band filter, usually called a single sideband filter, which es one of the sidebands as illustrated in the diagram below.

The type of SSB may be SSBAM (with a 'large' carrier component), SSBDimC or SSBSC depending on VDC at the input. A sequence of spectral diagrams are shown on the next page.

Single Sideband Amplitude Modulation

Single Sideband Amplitude Modulation Note that the bandwidth of the SSB signal B Hz is half of the DSB signal bandwidth. Note also that an ideal SSB filter response is shown. In practice the filter will not be ideal as illustrated.

As shown, with practical filters some part of the rejected sideband (the LSB in this case) will be present in the SSB signal. A method which eases the problem is to produce SSBSC from DSBSC and then add the carrier to the SSB signal.

Single Sideband Amplitude Modulation

Single Sideband Amplitude Modulation

with m(t) = Vm cos mt, we may write:

v s  t  = VDC cos ωc t  +

Vm V cos  ωc + ωm  t  + m cos  ωc  ωm  t  2 2

The SSB filter removes the LSB (say) and the output is

v s  t  = VDC cos ωc t  + Again, note that the output may be SSBAM, VDC large SSBDimC, VDC small SSBSC, VDC = 0

Vm cos  ωc + ωm  t  2 For SSBSC, output signal = V v s  t  = m cos  ωc + ωm  t  2

Power in SSB 

m2   From previous discussion, the total power in the DSB signal is PT = Pc  1 + 2   2 2 m m = PT = Pc + Pc + Pc for DSBAM. 4 4 Hence, if Pc and m are known, the carrier power and power in one sideband may be determined. Alternatively, since SSB signal =

v s  t  = VDC cos ωc t  +

Vm cos  ωc + ωm  t  2

then the power in SSB signal (Normalised Average Power) is 2

PSSB

V  V  = DC +  m  2  2 2

2

2

V V = DC + m 2 8 2

2

VDC Vm + Power in SSB signal = 2 8

2

Demodulation of Amplitude Modulated Signals

There are 2 main methods of AM Demodulation: • Envelope or non-coherent Detection/Demodulation. • Synchronised or coherent Demodulation.

Envelope or Non-Coherent Detection An envelope detector for AM is shown below:

This is obviously simple, low cost. But the AM input must be DSBAM with m << 1, i.e. it does not demodulate DSBDimC, DSBSC or SSBxx.

Large Signal Operation For large signal inputs, ( Volts) the diode is switched i.e. forward biased  ON, reverse biased  OFF, and acts as a half wave rectifier. The 'RC' combination acts as a 'smoothing circuit' and the output is m(t) plus 'distortion'.

If the modulation depth is > 1, the distortion below occurs

Small Signal Operation – Square Law Detector For small AM signals (~ millivolts) demodulation depends on the diode square law characteristic.

The diode characteristic is of the form i(t) = av + bv2 + cv3 + ..., where

v = VDC + m t   cos ωc t 

i.e. DSBAM signal.

Small Signal Operation – Square Law Detector i.e.

a VDC + m t   cos ωc t  + b VDC + m t   cos ωc t   + ... 2





2 = aVDC + am t  cos ωc t  + b VDC + 2VDC m t  + m t  cos  ωc t  + ... 2



2



1 1  + cos 2ωc t    2 2 

= aVDC + am t  cos ωc t  + bVDC + 2bVDC m t  + bm t   2

2

bVDC 2bVDC m t  bm t  2 VDC     aV + am t cos ω t + + + + b cos 2ωc t  + ... = DC c 2 2 2 2 2

2

'LPF' removes components. 2

bVDC aV + + bVDC m t  i.e. the output contains m(t) Signal out = DC 2

Synchronous or Coherent Demodulation A synchronous demodulator is shown below

This is relatively more complex and more expensive. The Local Oscillator (LO) must be synchronised or coherent, i.e. at the same frequency and in phase with the carrier in the AM input signal. This additional requirement adds to the complexity and the cost. However, the AM input may be any form of AM, i.e. DSBAM, DSBDimC, DSBSC or SSBAM, SSBDimC, SSBSC. (Note – this is a 'universal' AM demodulator and the process is similar to correlation – the LPF is similar to an integrator).

Synchronous or Coherent Demodulation If the AM input contains a small or large component at the carrier frequency, the LO may be derived from the AM input as shown below.

Synchronous (Coherent) Local Oscillator If we assume zero path delay between the modulator and demodulator, then the ideal LO signal is cos(ct). Note – in general the will be a path delay, say , and the LO would then be cos(c(t – ), i.e. the LO is synchronous with the carrier implicit in the received signal. Hence for an ideal system with zero path delay

Analysing this for a DSBAM input = 

VDC + m t   cos ωc t 

Synchronous (Coherent) Local Oscillator VX = AM input x LO =

VDC + m t   cos 2  ωc t 

=

VDC + m t   cos ωc t   cos ωc t 

=

VDC + m t   

1 1  + cos 2ωc t    2 2 

Vx =

VDC VDC m t  m  t  + cos 2ωc t  + + cos 2ωc t  2 2 2 2

We will now examine the signal spectra from 'modulator to Vx'

Synchronous (Coherent) Local Oscillator

(continued on next page)

Synchronous (Coherent) Local Oscillator

and

Note – the AM input has been 'split into two' – 'half' has moved or shifted up to

m t  V  m t   cos 2ωc t  + VDC cos 2ωc t   and half shifted down to baseband, DC and 2 2  2 

2 fc 

Synchronous (Coherent) Local Oscillator The LPF with a cut-off frequency  fc will only the baseband signal i.e.

Vout =

VDC m t  + 2 2

In general the LO may have a frequency offset, , and/or a phase offset, , i.e.

The AM input is essentially either: • DSB • SSB

(DSBAM, DSBDimC, DSBSC) (SSBAM, SSBDimC, SSBSC)

1. Double Sideband (DSB) AM Inputs The equation for DSB is

VDC + m t   cos ωc t 

where VDC allows full carrier (DSBAM),

diminished carrier or suppressed carrier to be set. Hence, Vx = AM Input x LO Since cosAcosB =

Vx = VDC + m t   cos ωc t  .cos  ωc + Δω  t + Δφ 

1  cos A + B  + cos A  B   2

VDC + m t    cos  ω

Vx =

2

c

+ ωc + Δω  t + Δφ  + cos  ωc + Δω  t + Δφ  ωc t  

 VDC m t   +   cos  2ωc + Δω  t + Δφ  + cos Δωt + Δφ   2 2  

Vx = 

VDC V cos  2ωc + Δω  t + Δφ + DC cos Δωt + Δφ  2 2 m t  m t  + cos  2ωc + Δω  t + Δφ  + cos Δωt + Δφ 2 2

Vx =

1. Double Sideband (DSB) AM Inputs The LPF with a cut-off frequency  fc Hz will remove the components at 2c (i.e. components above c) and hence Vout =

VDC m t  cos Δt  + Δφ + cos Δωt + Δφ  2 2

VDC m t  + 2 2 Consider now if  is equivalent to a few Hz offset from the ideal LO. We may then say V m t  Vout = DC cos Δωt  + cos Δωt  2 2

Obviously, if Δω = 0 and Δφ we have, as previously Vout =

The output, if speech and processed by the human brain may be intelligible, but would include a low frequency 'buzz' at , and the message amplitude would fluctuate. The requirement  = 0 is necessary for DSBAM.

1. Double Sideband (DSB) AM Inputs Consider now if  is equivalent to a few Hz offset from the ideal LO. We may then say V m t  Vout = DC cos Δωt  + cos Δωt  2 2 The output, if speech and processed by the human brain may be intelligible, but would include a low frequency 'buzz' at , and the message amplitude would fluctuate. The requirement  = 0 is necessary for DSBAM. Consider now that  = 0 but   0, i.e. the frequency is correct at c but there is a phase offset. Now we have

Vout =

VDC m t  cos Δφ  + cos Δφ 2 2

'cos()' causes fading (i.e. amplitude reduction) of the output.

1. Double Sideband (DSB) AM Inputs The 'VDC' component is not important, but consider for m(t), • if Δφ =

m t   π π π cos  = 0 (900), cos  = 0 i.e. Vout = 2 2  2  2

• if Δφ =

m t  π (1800), cos π  = 1 i.e. Vout = cos π  = m t  2 2

The phase inversion if  =  may not be a problem for speech or music, but it may be a problem if this type of modulator is used to demodulate PRK

π the signal strength However, the major problem is that as  increases towards 2 π output gets weaker (fades) and at the output is zero 2

1. Double Sideband (DSB) AM Inputs If the phase offset varies with time, then the signal fades in and out. The variation of amplitude of the output, with phase offset  is illustrated below

Thus the requirement for  = 0 and  = 0 is a 'strong' requirement for DSB amplitude modulation.

2. Single Sideband (SSB) AM Input The equation for SSB with a carrier depending on VDC is

VDC cos ωc t  +

Vm cos ωc + ωm t  2

i.e. assuming m t  = Vm cos ωm t 

V   Hence V x =  VDC cos ωc t  + m cos ωc + ωm t   cos  ωc + ωm  + Δφ  2   VDC V cos  2ωc + Δω  t + Δφ  + DC cos Δωt + Δφ  2 2 V V + m cos  2ωc + ωm + Δω  t + Δφ  + m cos  ωm  Δω  t  Δφ  4 4

=

2. Single Sideband (SSB) AM Input The LPF removes the 2c components and hence

VDC Vm cos Δωt + Δφ  + cos  ωm  Δω  t  Δφ  2 4 Note, if  = 0 and  = 0,

VDC Vm + cos ωm t  ,i.e. m t  = Vm cos ωmt  has been 2 4

recovered. Consider first that   0, e.g. an offset of say 50Hz. Then

Vout =

VDC V cos Δωt  + m cos  ωm  Δω  t  2 4

If m(t) is a signal at say 1kHz, the output contains a signal a 50Hz, depending on VDC and the 1kHz signal is shifted to 1000Hz - 50Hz = 950Hz.

2. Single Sideband (SSB) AM Input The spectrum for Vout with  offset is shown

Hence, the effect of the offset  is to shift the baseband output, up or down, by . For speech, this shift is not serious (for example if we receive a 'whistle' at 1kHz and the offset is 50Hz, you hear the whistle at 950Hz ( = +ve) which is not very noticeable. Hence, small frequency offsets in SSB for speech may be tolerated. Consider now that  = 0,  = 0, then

Vout =

VDC V cos Δφ  + m cos ωm t  Δφ  2 4

2. Single Sideband (SSB) AM Input • This indicates a fading VDC and a phase shift in the output. If the variation in  with time is relatively slow, thus phase shift variation of the output is not serious for speech. • Hence, for SSB small frequency and phase variations in the LO are tolerable. The requirement for a coherent LO is not as a stringent as for DSB. For this reason, SSBSC (suppressed carrier) is widely used since the receiver is relatively more simple than for DSB and power and bandwidth requirements are reduced.

Comments •

In of 'evolution', early radio schemes and radio on long wave (LW) and medium wave (MW) to this day use DSBAM with m < 1. The reason for this was the reduced complexity and cost of 'millions' of receivers compared to the extra cost and power requirements of a few large LW/MW transmitters for broadcast radio, i.e. simple envelope detectors only are required.

•

Nowadays, with modern integrated circuits, the cost and complexity of synchronous demodulators is much reduced especially compared to the additional features such as synthesised LO, display, FM etc. available in modern receivers. Amplitude Modulation forms the basis for:

• • • • •

Digital Modulation – Amplitude Shift Keying ASK Digital Modulation – Phase Reversal Keying PRK Multiplexing – Frequency Division Multiplexing FDM Up conversion – Radio transmitters Down conversion – Radio receivers

Phase Shift Method for SSB Generation The diagram below shows the Phase Shift Method for generating SSBSC

fm and fc denote phase shifts at the message frequency (fm) and the carrier frequency (fc).

Phase Shift Method for SSB Generation Solving for Vout in general i.e.

Vout = Va + Vb

Vout = Vm cos ωm t  cos ωc t  + Vm cos ωm t + φm  cos ωc t + φc 

Since cosAcosB =

Vout =

1  cos A + B  + cos A  B   2

Vm V V cos  ωc + ωm  t  + m cos  ωc  ωm  t  + m cos  ωc + ωm  t + φc + φm  2 2 2 Vm + cos  ωc  ωm  t +  φc  φm   2

The actual form of the modulation at the output will depend on the phase shifts fm and fc.

Phase Shift Method for SSB Generation

Consider Vout when φm =

Vout =

Since

π 2

φc =

π (i.e.900) 2

Vm V V cos  ωc + ωm  t  + m cos  ωc  ωm  t  + m cos  ωc + ωm  t + π  2 2 2 Vm + cos  ωc  ωm  t + 0  2

Vcos θ + π  = Vcosθ

then Vout

= Vm cos  ωc  ωm  t  , i.e. SSBSC/LSB.

When fm = 900 and fc = 900 the output is Single Sideband Suppressed Carrier – Lower Sideband.

Phase Shift Method for SSB Generation π π φ =  Consider Vout when φm = , c 2 2  

Vout

Vm Vm Vm = cos  ωc + ωm  t  + cos  ωc  ωm  t  + cos  ωc + ωm  t + 0  2 2 2 V + m cos  ωc  ωm  t  π  2

and since

Vcos θ  π  = Vcosθ

then 

Vout = Vm cos  ωc + ωm  t 

i.e. SSBSC/USB. When fm = 900 and fc = -900 the output is Single Sideband Suppressed Carrier – Upper Sideband. Note – for m(t) as a band of signals, the phase shift fm must be the same e.g. /2 or 900 at all frequencies.

Exercise 1) When fm = 0 and fc = 0 show that

Vout = Vm cos  ωc + ωm  t  + Vm cos  ωc  ωm  t 

2) When fm = 0 and fc =  show that Vout = 0

Quadrature Modulation A variation on the Phase Shift Method is shown below

In this form of the method, 2 different message signals m1(t) and m2(t) are input.

Quadrature Modulation The carrier cos ωc t  is phase shifted by 900 to give

sin  ωc t 

The two carriers, cos ωc t  and  sin  ωc t  are in phase quadrature (orthogonal). The process is described as

. 

Quadrature Modulation or Quadrature Multiplexing and as Independent Sideband ISB.

Clearly,

Vout = m1  t  cos ωc t  + m2  t  cos ωc t 

Quadrature Modulation Each 'term' in the output is a DSBSC signal occupying the same bandwidth, but phase shifted by 900 relative to each other

Quadrature Modulation Demodulation will require synchronous demodulators as shown below.

Vin = m1  t  cos ωc t  + m2  t  cos ωc t 

Quadrature Modulation 2 Clearly  Vx1 = m1  t  cos  ωc t  + m2  t  cos ωc t  sin  ωc t 

1  sin  A + B  + sin  A  B   2 m t m t t m t Vx1 = m1 + 1 cos 2ωc t  + 2 sin  2ωc t  + 2 sin0 2 2 2 2

Since  sinAcosB =

Since the LPF with cut-off frequency = fc, the output V1 out = Similarly,

Vx2 = m1  t  cos ωc t  sin  ωc t  + m2  t  sin 2  ωc t 

2 Since sin A =

Vx2 =

m1  t  2

1 1  cos2 A 2

m1  t  m t m t m t sin  2ωc t  + 2 sin0 + 2  2 cos 2ωc t  2 2 2 2

Again, LPF removes the '2wc components, i.e. V2 out =

m2  t  2

Quadrature Modulation This type of modulation/multiplexing is used in radio systems, television and as a form of stereo multiplexing for AM radio.

Vestigial Sideband Modulation Some signals, such as TV signals contain low frequencies, or even extend down to DC.

When DSB modulated we have

Vestigial Sideband Modulation It is now impossible to produce SSB, because the SSB filter would need to be ideal, as shown above. In practice the filter is as below

The signal produced is called vestigial sideband, it contains the USB and a 'vestige' of the lower sideband. The BPF design is therefore less stringent. When demodulated the baseband signal is the sum of the USB and the vestige of the LSB

Vestigial Sideband Modulation

Hence the original baseband signal. VSB is used in TV systems.