frequency modulation(fm ) chapter 3. frequency modulation (fm) part 1

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FREQUENCY MODULATION(FM ) CHAPTER 3

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Page 1: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FREQUENCY MODULATION(FM )

CHAPTER 3

Page 2: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FREQUENCY MODULATION(FM)

Part 1

Page 3: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM :Introduction

FM is the process of varying the frequency of a carrier wave in proportion to a modulating signal.

The amplitude of the carrier wave is kept constant while its frequency and a rate of change are varied by the modulating signal.

Page 4: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM :Introduction (cont…) Fig 3.1 :

Frequency Modulated signal

Page 5: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM :Introduction (cont…)

The important features about FM waveforms are :

i. The frequency varies.ii. The rate of change of carrier frequency

changes is the same as the frequency of the information signal.

iii. The amount of carrier frequency changes is proportional to the amplitude of the information signal.

iv. The amplitude is constant.

Page 6: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM :Introduction (cont…) The FM modulator receives two signals,the information

signal from an external source and the carrier signal from a built in oscillator.

The modulator circuit combines the two signals producing a FM signal which passed on to the transmission medium.

The demodulator receives the FM signal and separates it, passing the information signal on and eliminating the carrier signal.

Federal Communication Coporation (FCC) allocation for a standard broadcast FM station is as shown in Fig.3.2

Page 7: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Figure 3.2: FM frequency allocation by FCC

Page 8: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Analysis of FM Mathematical analysis: Let message signal:

(3.1) And carrier signal: (3.2) Where carrier frequency is very much

higher than message frequency.

tVt mmm cos

]cos[ tVt ccc

Page 9: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Analysis of FM (cont’d)

In FM, frequency changes with the change of the amplitude of the information signal. So the instantenous frequency of the FM wave is;

(3.3)

K is constant of proportionality

tKVtKv mmCmci cos

Page 10: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Analysis of FM(cont’d)

Thus, we get the FM wave as:

3.4 Where modulation index for FM is given

by

)sincos(cos)( 1 tKV

tVVctv mm

mCCFM

)sincos()( tmtVtv mfCCFM

m

mf

KVm

Page 11: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Analysis of FM(cont’d)

Frequency deviation: ∆f is the relative placement of carrier frequency (Hz) w.r.t its unmodulated value. Given as:

mC KVmax

mC KVmin

mCCd KV minmax

22md KV

f

Page 12: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM(cont’d) Therefore:

mf

m

f

fm

KVf

;2

;mVf

Page 13: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.1

FM broadcast station is allowed to have a frequency deviation of 75 kHz. If a 4 kHz (highest voice frequency) audio signal causes full deviation (i.e. at maximun amplitude of information signal) , calculate the modulation index.

Page 14: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.2 Determine the peak frequency

deviation, , and the modulation index, mf, for an FM modulator with a deviation Kf = 10 kHz/V. The modulating signal to be transmitted is

Vm(t) = 5 cos ( cos 10kπt).

f

Page 15: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Equations for Phase- and Frequency-Modulated Carriers

TomasiElectronic Communications Systems, 5e

Copyright ©2004 by Pearson Education, Inc.

Upper Saddle River, New Jersey 07458

All rights reserved.

Page 16: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM&PM (Bessel function)

Thus, for general equation:

)coscos()( tmtVtv mfCCFM

)sinsin()( tmtVtv mfCCFM

)sinsin(cos)sincos(sin tmttmtV mfcmfCC

Page 17: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Bessel function

ttmJtmJVtv mCmCfCfCFM )sin()sin()(sin)([ 10

ttmJV mCmCfC )2sin()2sin()([ 2

..])3sin()3sin()([ 3 ttmJV mCmCfC

Page 18: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

B.F. (cont’d) It is seen that each pair of side band is preceded by J

coefficients. The order of the coefficient is denoted by subscript m. The Bessel function can be written as

N=number of the side frequency M=modulation index

....

!2!2

2/

!1!1

2/

!

1

2

42

n

m

n

m

n

mmJ ff

n

ffm

Page 19: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Bessel Functions of the First Kind, Jn(m) for some value of modulation index

Page 20: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

B.F. (cont’d)

Page 21: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Representation of frequency spectrum

Page 22: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Angle ModulationPart 2

FM BandwidthPower distribution of FM

Generation & Detection of FM

Application of FM

Page 23: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM Bandwidth Theoretically, the generation and transmission of FM

requires infinite bandwidth. Practically, FM system have finite bandwidth and they perform well.

The value of modulation index determine the number of sidebands that have the significant relative amplitudes

If n is the number of sideband pairs, and line of frequency spectrum are spaced by fm, thus,, the bandwidth is:

For n=>1

mfm nfB 2

Page 24: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM Bandwidth (cont’d) Estimation of transmission b/w; Assume mf is large and n is approximate mf +2; thus Bfm=2(mf +2)fm

=

(1) is called Carson’s rule

mm

ff

f)2(2

)1)........(2(2 mfm ffB

Page 25: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Deviation Ratio (DR)

The worse case modulation index which produces the widest output frequency spectrum.

Where ∆f(max) = max. peak frequency deviation fm(max) = max. modulating signal frequency

(max)

(max)

mf

fDR

Page 26: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.3 An FM modulator is operating with a

peak frequency deviation =20 kHz.The modulating signal frequency, fm is 10 kHz, and the 100 kHz carrier signal has an amplitude of 10 V. Determine :

a) The minimum bandwidth using Bessel Function table.

b)The minimum bandwidth using Carson’s Rule.

Sketch the frequency spectrum for (a), with actual amplitudes.

f

Page 27: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.4 For an FM modulator with a modulation

index m=1, a modulating signal Vm(t)=Vm sin(2π1000t), and an unmodulated carrier Vc(t) = 10sin(2π500kt), determine :

a) Number of sets of significant side frequencies

b) Their amplitudes c) Draw the frequency spectrum

showing their relative amplitudes.

Page 28: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.4 (solution)

a) From table of Bessel function, a modulation index of 1 yields a reduced carrier component

and three sets of significant side frequencies. b) The relative amplitude of the carrier and

side frequencies are Jo = 0.77 (10) = 7.7 V J1 = 0.44 (10) = 4.4 V J2 = 0.11 (10) = 1.1 V J3 = 0.02 (10) = 0.2 V

Page 29: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.4 (solution) : FREQUENCY SPECTRUM

497 498 499 500 501 502 503 J3 J2 J1 JO J1 J2 J3

7.7 V

4.4V4.4V

1.1V1.1V

0..2 0..2

Page 30: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM Power Distribution

As seen in Bessel function table, it shows that as the sideband relative amplitude increases, the carrier amplitude,J0 decreases.

This is because, in FM, the total transmitted power is always constant and the total average power is equal to the unmodulated carrier power, that is the amplitude of the FM remains constant whether or not it is modulated.

Page 31: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM Power Distribution (cont’d) In effect, in FM, the total power that is

originally in the carrier is redistributed between all components of the spectrum, in an amount determined by the modulation index, mf, and the corresponding Bessel functions.

At certain value of modulation index, the carrier component goes to zero, where in this condition, the power is carried by the sidebands only.

Page 32: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Average Power

The average power in unmodulated carrier

The total instantaneous power in the angle modulated carrier.

The total modulated power

R

VP cc

2

R

Vtt

R

VP

ttR

V

R

tmP

cc

ct

cc

t

2)](22cos[

2

1

2

1

)]([cos)(

22

222

R

V

R

V

R

V

R

VPPPPP ncnt 2

)(2..

2

)(2

2

)(2

2..

222

21

2

210 R

V

R

V

R

V

R

VPPPPP ncnt 2

)(2..

2

)(2

2

)(2

2..

222

21

2

210

Page 33: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.5

a) Determine the unmodulated carrier power for the FM modulator and condition given in example 3.4, (assume a load resistance RL = 50 Ώ)

b) Determine the total power in the angle modulated wave.

Page 34: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Example 3.5 : solution a) Pc = (10)(10)/(2)(50) =1 W

b)

)50(2

)2.0(2

)50(2

)1.1(2

)50(2

)4.4(2

)50(2

7.7 2222

tP

WPt 0051.10008.00242.03872.05929.0

Page 35: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Generation of FM

Two major FM generation:i) Direct method:

i) straight forward, requires a VCO whose oscillation frequency has linear dependence on applied voltage.

ii) Advantage: large frequency deviationiii) Disadvantage: the carrier frequency tends to drift

and must be stabilized.iv) example circuit:

i) Reactance modulatorii) Varactor diode

Page 36: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Generation of FM (cont’d)

ii) Indirect method: i. Frequency-up conversion.ii. Two ways:

a. Heterodyne methodb. Multiplication method

iii. One most popular indirect method is the Armstrong modulator

Page 37: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Armstrong modulator

IntegratorBalanced modulator

Down converter

Frequency multiplier (x n)

Crystal oscillatorPhase shifter

Vc(t)fc

Vm(t)fm

Page 38: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Armstrong modulator For example:

Let fm =15Hz and fc= 200kHzAt frequency deviation= 75kHz,it need a frequency multiplication by a factor, n,n=75000/15=5000;

So it need a chain of four triplers (34) and six doublers (26), ie:n= (34) x (26)=5184,

But, n x fc=5000 x 200kHz=1000MHz

So, down converter with oscillating frequency=900MHz is needed to put fc in the

FM band of 88MHz-108MHz

Page 39: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM Detection/Demodulation

FM demodulation

is a process of getting back or regenerate the original modulating signal from the modulated FM signal.

It can be achieved by converting the frequency deviation of FM signal to the variation of equivalent voltage.

The demodulator will produce an output where its instantaneous amplitude is proportional to the instantaneous frequency of the input FM signal.

Page 40: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

FM detection (cont’d) To detect an FM signal, it is necessary

to have a circuit whose output voltage varies linearly with the frequency of the input signal.

The most commonly used demodulator is the PLL demodulator. Can be use to detect either NBFM or WBFM.

Page 41: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

PLL Demodulator

Phase detector

VCO

Low pass filter

Amplifier

FM input

Vc(t)

fVc0

V0(t)

Page 42: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

PLL Demodulator The phase detector produces an average output voltage

that is linear function of the phase difference between the two input signals. This low frequency component is selected by LPF.

After amplification, part of the signal is fed back through VCO where it results in frequency modulation of the VCO frequency. When the loop is in lock, the VCO frequency follows or tracks the incoming frequency.

Page 43: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

PLL Demodulator Let instantaneous freq of FM Input, fi(t)=fc +k1vm(t), and the VCO output frequency, f VCO(t)=f0 + k2Vc(t);

f0 is the free running frequency. For the VCO frequency to track the

instantaneous incoming frequency, fvco = fi; or

Page 44: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

PLL Demodulator f0 + k2Vc(t)= fc +k1vm(t), so,

If VCO can be tuned so that fc=f0, then

Where Vc(t) is also taken as the output voltage, which therefore is the demodulated output

)()( 10 tvkfftV mcc

)()( 1 tvktV mc

Page 45: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Comparison AM and FM Its the SNR can be increased without increasing transmitted

power about 25dB higher than in AM

Certain forms of interference at the receiver are more easily to suppressed, as FM receiver has a limiter which eliminates the amplitude variations and fluctuations.

The modulation process can take place at a low level power stage in the transmitter, thus a low modulating power is needed.

Power content is constant and fixed, and there is no waste of power transmitted

There are guard bands in FM systems allocated by the standardization body, which can reduce interference between the adjacent channels.

Page 46: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Application of FM

used by most of the field VHF portable, mobile and base radios in exploration use today. It is preferred because of its immunity to noise or interference and at the frequencies used the antennas are of a reasonable size.

Page 47: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary of angle modulation-what you need to be familiar with

Page 48: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary (cont’d)

Page 49: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary (cont’d) Bandwidth:a) Actual minimum bandwidth from

Bessel table:

b) Approximate minimum bandwidth using Carson’s rule:

)(2 mfnB

)(2 mffB

Page 50: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary (cont’d)

Multitone modulation (equation in general): 21 mmci KvKv

....cos2cos2 2211 tftfci

......sinsin 22

21

1

1 tf

ft

f

ftCi

Page 51: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary (cont’d)

..].........sinsinsin[

]sinsinsin[

sin

2211

22

21

1

1

tmtmtV

tf

ft

f

ftVtv

Vtv

ffCC

CCfm

iCfm

Page 52: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Summary (cont’d)-Comparison NBFM&WBFM

Page 53: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

ANGLE MODULATION

Part 3Advantages

Disadvantages

Page 54: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Advantages

Wideband FM gives significant improvement in the SNR at the output of the RX which proportional to the square of modulation index.

Angle modulation is resistant to propagation-induced selective fading since amplitude variations are unimportant and are removed at the receiver using a limiting circuit.

Angle modulation is very effective in rejecting interference. (minimizes the effect of noise).

Angle modulation allows the use of more efficient transmitter power in information.

Angle modulation is capable of handing a greater dynamic range of modulating signal without distortion than AM.

Page 55: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

Disadvantages Angle modulation requires a

transmission bandwidth much larger than the message signal bandwidth.

The capture effect where the wanted signal may be captured by an unwanted signal or noise voltage.

Angle modulation requires more complex and inexpensive circuits than AM.

Page 56: FREQUENCY MODULATION(FM ) CHAPTER 3. FREQUENCY MODULATION (FM) Part 1

END OF ANGLE MODULATION