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Communications II Lecture 5: Effects of on FM

Professor Kin K. Leung EEE and Computing Departments Imperial College London © Copyright reserved Outline

• Recap of FM

• FM system model in noise

• Derivation of output SNR

• Pre/de-emphasis

• Comparison with AM

• Reference: Lathi, Chap. 12.

© KKL 2 Modulation

Fundamental difference between AM and FM:

AM: message information contained in the amplitude ⇒ Additive noise: corrupts directly the modulated signal.

FM: message information contained in the signal frequency ⇒ the effect of noise on an FM signal is determined by the extent to which it changes the frequency of the modulated signal.

Consequently, FM is less affected by noise than AM signals

© KKL 3 REVISION:

A carrier waveform

s(t) = A cos[θi(t)]

where

θi(t): the instantaneous phase angle.

© KKL 4 When

s(t) = A cos(2f t) ⇒ θi(t) = 2f t

We may say that  d 1 d  2 f  f  dt 2 dt Generalisation: instantaneous frequency:

1 d (t) f (t)  i i 2 dt

© KKL 5 In FM: the instantaneous frequency of the carrier varies linearly with the message: f (t)=f +k m(t) i c f  where k is the frequency sensitivity of the modulator. Hence (assuming f   θi(0)=0):  t i (t)  2 fi ( )d 0  t   2 fct  2 k f m( )d  0 Modulated signal:   t   s(t)  Acos 2 fct  2 k f m( )d  0  Note:   (a) The envelope is constant (b) Signal s(t) is a non-linear function of the message signal m(t).

© KKL 6 Bandwidth of FM

mp ≡ max |m(t)|: peak message amplitude

fc − kf mp < instantaneous frequency < fc + kf mp

Define: frequency deviation= the deviation of the instantaneous frequency from the carrier frequency:

∆f ≡ kf mp Define: deviation ratio: f   W where W: the message bandwidth.

© KKL 7 Small β: FM bandwidth  2x message bandwidth (narrow-band FM)

Large β: FM bandwidth >> 2x message bandwidth (wide-band FM)

Carson’s rule of thumb:

BT = 2W(β+1) = 2(∆f + W)

β <<1 ⇒ BT ≈ 2W (as in AM)

β >>1 ⇒ BT ≈ 2∆f, independent of W

© KKL 8 Noise in FM

Model of an FM receiver

© KKL 9 Bandpass filter: removes any signals outside the bandwidth of

fc ± BT/2 ⇒ the predetection noise at the receiver is bandpass with a bandwidth of

BT.

FM signal has a constant envelope ⇒ use a limiter to remove any amplitude variations

Discriminator: a device with output proportional to the deviation in the instantaneous frequency ⇒ it recovers the message signal

Final baseband low-pass filter: has a bandwidth of W ⇒ it passes the message signal and removes out-of-band noise.

© KKL 10 Linear argument at high SNR

FM is nonlinear modulation, meaning superposition doesn’t hold.

Nonetheless, it can be shown (see Chap. 9, Lathi) that for high SNR, noise output and message signal are approximately independent of each other: Output ≈ Message + Noise.

Any (smooth) nonlinear systems are locally linear!

Noise does not affect of the message signal at the output

⇒ We can compute the signal power for the case without noise, and accept that the result holds for the case with noise too.

© KKL 11 Power of signal at the output without noise:

Instantaneous frequency of the input signal:

fi  fc  k f m(t)

Output of discriminator:

k f m(t)

So, output signal power:

2 PS  k f P

where: P : the average power of the message signal

© KKL 12  In the presence of additive noise, the real predetection signal is    t   x(t)  Acos 2 fct  2 k f m( )d  0 

 nc (t)cos(2 fct)  ns (t)sin(2fct)

It can be shown (by linear argument): For high SNR, noise output: approximately independent of the message signal

⇒ We only have the carrier and noise signals present ⇒ In order to calculate the power of output noise, we may use: ~ x(t)  Acos(2fct)  nc (t)cos(2fct)  ns (t)sin(2fct)

© KKL 13 Phasor diagram of the FM carrier and noise signals

© KKL 14 Instantaneous phase:

1 ns (t) i (t)  tan A  nc (t) For large carrier power (large A): n (t)  (t)  tan1 s i A n (t)  s A Discriminator output = instantaneous frequency: 1 d (t) f (t)  i i 2 dt 1 dn (t)  s 2A dt

© KKL 15 The discriminator output in the presence of signal and noise:

1 dn (t) k m(t)  s f 2A dt dn (t) What is the PSD of s dt

Fourier theory: if x(t)  X ( f ) dx(t) then  j2fX ( f ) dt Differentiation with respect to time = passing the signal through a system with transfer function of H(f ) = j2 f

© KKL 16 It can be shown:

2 So ( f ) | H ( f ) | Si ( f )

where:

Si(f ): PSD of input signal

So(f ): PSD of output signal

H(f ): transfer function of the system

© KKL 17  dns (t) 2 PSD of  | j2f | PSD of ns (t)  dt 

 BT  PSD of ns (t)  N0 within band    2 

Then: 

 dns (t) 2 PSD of  | j2 f | N0  dt   2  1 dns (t)  1  2 PSD of fi (t)      | j2f | N0  SD ( f )  2 A dt   2 A After the baseband LPF, this is restricted in the band ±W

© KKL 18 Power spectral densities for FM noise analysis

© KKL 19 Average at the receiver output:

W PN  SD ( f )df W Thus,

2 3 W  1  2 2N0W PN    | j2f | N0df  W  2 A 3A2

1 Average noise power at the output of a FM receiver  carrier power A2

A ↑⇒Noise↓, called the quieting effect

© KKL 20 2 2 3A k f P SNRO  3  SNRFM 2N0W Transmitted power of an FM waveform: A2 P  T 2 PT From SNRbaseband  : N0W 2 3k f P 2 P SNRFM  2 SNRbaseband  3 2 SNRbaseband W mp Valid when the carrier power is large compared with the noise power

© KKL 21 The FM detector exhibits a (more pronounced) threshold effect like the AM envelope detector.

The threshold point occurs around when signal power is 10 time noise power: A2  10 2N0BT

where

BT = 2W (β + 1) (Carson’s rule of thumb)

© KKL 22 Qualitative discussion of threshold effect

Phase noise

(c) phase shift 2  is caused by rotation around the origin

© KKL 23 Pre-emphasis and De-emphasis: An alternative way to

increase SNRFM

PSD of the noise at the detector output ∝ square of frequency.

PSD of a typical message typically rolls off at around 6 dB per decade

© KKL 24 To increase SNRFM : • Use a LPF to cut-off high at the output

Message is attenuated too Not very satisfactory

• Use pre-emphasis and de-emphasis

Message is unchanged High frequency components of noise are suppressed

© KKL 25 Pre-emphasis and de-emphasis in an FM system

© KKL 26 Hpe(f ): used to artificially emphasize the high frequency components of the message prior to modulation, and hence, before noise is introduced.

Hde(f ): used to de-emphasize the high frequency components at the receiver, and restore the original PSD of the message signal.

In theory, Hpe(f ) ∝ f , Hde(f ) ∝ 1/f .

This can improve the output SNR by around 13 dB.

Dolby uses an analogous pre-emphasis technique to reduce the effects of noise (hissing noise in audiotape recording is also concentrated on high frequency).

© KKL 27 Simple linear pre-emphasis and de-emphasis circuits

© KKL 28 Comparison of Analogue Communication Systems

Assumptions:

① single-tone modulation, ie: m(t) = Am cos(2 fmt)

② the message bandwidth W = fm;

③ for the AM system, µ = 1;

④ for the FM system, β = 5 (which is what is used in commercial FM transmission, with ∆f = 75 kHz, and W = 15 kHz).

© KKL 29 With these assumptions, we find that the SNR expressions for the various modulation schemes become:

SNRDSBSC = SNRbaseband

1 SNR  SNR AM 3 baseband 3 75 SNR   2SNR  SNR FM 2 baseband 2 baseband

where we used  = 5

© KKL 30 Noise performance of analog communication systems

© KKL 31 Conclusions

AM: The SNR performance is 4.8 dB worse than a baseband system, and

the transmission bandwidth is BT = 2W .

DSB: The SNR performance is identical to a baseband system, and the

transmission bandwidth is BT = 2W (for SSB, the SNR performance is again identical, but the transmission bandwidth is only BT = W ).

FM: The SNR performance is 15.7 dB better than a baseband system, and

the transmission bandwidth is BT = 2(β + 1)W = 12W (with pre- and de- emphasis the SNR performance is increased by about 13 dB with the same transmission bandwidth).

© KKL 32