Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear...

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Probability and Random Processes (Part โ€“ I) 1. The variance of a random variable X is 2 . Then the variance of โ€“kX (where k is a positive constant) is (a) 2 (b) โˆ’ 2 (c) 2 (d) 2 2 [GATE 1987: 2 Marks] Soln. (โˆ’) = [(โˆ’) ] = [ ] = [ ] = Option (d) 2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at the filter output is (a) Uniform (b) Poisson (c) Gaussian (d) Rayleigh [GATE 1987: 2 Marks] Soln. The narrow band representation of noise is () = () + () Its envelope is โˆš () + () () () are two independent zero mean Gaussian processes with same variance. The resulting envelope is Rayleigh variable Option (d) 3. Events A and B are mutually exclusive and have nonzero probability. Which of the following statement(s) are true? (a) ( โˆช ) = () + () (b) ( ) > () (c) ( โˆฉ ) = ()() (d) ( ) < () [GATE 1988: 2 Marks]

Transcript of Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear...

Page 1: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

Probability and Random Processes (Part โ€“ I)

1. The variance of a random variable X is ๐œŽ๐‘ฅ2. Then the variance of โ€“kX

(where k is a positive constant) is

(a) ๐œŽ๐‘ฅ2

(b) โˆ’๐‘˜๐œŽ๐‘ฅ2

(c) ๐‘˜๐œŽ๐‘ฅ2

(d) ๐‘˜2๐œŽ๐‘ฅ2

[GATE 1987: 2 Marks]

Soln. ๐‘ฝ๐’‚๐’“(โˆ’๐’Œ๐‘ฟ) = ๐‘ฌ[(โˆ’๐’Œ๐‘ฟ)๐Ÿ]

๐ˆ๐Ÿ = ๐‘ฌ[๐’Œ๐Ÿ๐‘ฟ๐Ÿ]

= ๐’Œ๐Ÿ๐‘ฌ[๐‘ฟ๐Ÿ]

= ๐’Œ๐Ÿ๐ˆ๐’™๐Ÿ

Option (d)

2. White Gaussian noise is passed through a linear narrow band filter. The

probability density function of the envelope of the noise at the filter

output is

(a) Uniform

(b) Poisson

(c) Gaussian

(d) Rayleigh

[GATE 1987: 2 Marks]

Soln. The narrow band representation of noise is

๐’(๐’•) = ๐’๐’„(๐’•) ๐œ๐จ๐ฌ ๐Ž๐’„๐’• + ๐’๐’”(๐’•) ๐ฌ๐ข๐ง ๐Ž๐’„๐’•

Its envelope is โˆš๐’๐’„๐Ÿ(๐’•) + ๐’๐’”

๐Ÿ(๐’•)

๐’๐’„(๐’•) ๐’‚๐’๐’… ๐’๐’”(๐’•) are two independent zero mean Gaussian processes

with same variance. The resulting envelope is Rayleigh variable

Option (d)

3. Events A and B are mutually exclusive and have nonzero probability.

Which of the following statement(s) are true?

(a) ๐‘ƒ(๐ด โˆช ๐ต) = ๐‘ƒ(๐ด) + ๐‘ƒ(๐ต)

(b) ๐‘ƒ(๐ต๐ถ) > ๐‘ƒ(๐ด)

(c) ๐‘ƒ(๐ด โˆฉ ๐ต) = ๐‘ƒ(๐ด)๐‘ƒ(๐ต)

(d) ๐‘ƒ(๐ต๐ถ) < ๐‘ƒ(๐ด)

[GATE 1988: 2 Marks]

Page 2: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

Soln. For mutually exclusive events A and B

๐‘ท(๐‘จ โˆช ๐‘ฉ) = ๐‘ท(๐‘จ) + ๐‘ท(๐‘ฉ)

Option (a)

4. Two resistors R1 and R2 (in ohms) at temperatures

๐‘‡10 ๐พ ๐‘Ž๐‘›๐‘‘ ๐‘‡2

0 ๐พ respectively, are connected in series. Their equivalent

noise temperature is ________0K.

[GATE 1991: 2 Marks]

Soln.

๏ฟฝฬ…๏ฟฝ๐’๐Ÿ = ๏ฟฝฬ…๏ฟฝ๐’๐Ÿ

๐Ÿ + ๏ฟฝฬ…๏ฟฝ๐’๐Ÿ

๐Ÿ

๐Ÿ’๐‘ฒ๐‘ป๐’†๐‘ฉ(๐‘น๐Ÿ + ๐‘น๐Ÿ) = ๐Ÿ’๐‘ฒ๐‘ป๐Ÿ๐‘ฉ๐‘น๐Ÿ + ๐Ÿ’๐‘ฒ๐‘ป๐Ÿ๐‘ฉ๐‘น๐Ÿ

๐‘ป๐’†(๐‘น๐Ÿ + ๐‘น๐Ÿ) = ๐‘น๐Ÿ๐‘ป๐Ÿ + ๐‘น๐Ÿ๐‘ป๐Ÿ

๐’๐’“ ๐‘ป๐’† = (๐‘น๐Ÿ๐‘ป๐Ÿ + ๐‘น๐Ÿ๐‘ป๐Ÿ)/(๐‘น๐Ÿ + ๐‘น๐Ÿ) Equivalent noise temperature

5. For a random variable โ€˜Xโ€™ following the probability density function,

p(x), shown in figure, the mean and the variance are, respectively

p(x)

x-1 0 3

1/4

(a) 1/2 and 2/3

(b) 1 and 4/3

(c) 1 and 2/3

(d) 2 and 4/3

[GATE 1992: 2 Marks]

Page 3: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

Soln. Mean or average of any random variable is known as expected value

of random variable X

๐‘ด๐’†๐’‚๐’ = ๐๐‘ฟ = ๐‘ฌ[๐‘ฟ] = โˆซ ๐’™๐‘ท๐‘ฟ(๐’™)๐’…๐’™

โˆž

โˆ’โˆž

= โˆซ ๐’™๐Ÿ

๐Ÿ’๐’…๐’™ =

๐Ÿ

๐Ÿ’[๐’™๐Ÿ

๐Ÿ]

๐Ÿ

๐Ÿ‘๐Ÿ‘

โˆ’๐Ÿ

=๐Ÿ

๐Ÿ’[๐Ÿ–

๐Ÿ] = ๐Ÿ

๐‘ฝ๐’‚๐’“๐’Š๐’‚๐’๐’„๐’† = ๐ˆ๐’™๐Ÿ = ๐‘ฌ[(๐‘ฟ โˆ’ ๐๐‘ฟ)] = โˆซ(๐’™ โˆ’ ๐๐‘ฟ)๐Ÿ๐‘ท๐‘ฟ(๐’™)๐’…๐’™

โˆž

โˆ’โˆž

= โˆซ(๐’™ โˆ’ ๐Ÿ)๐Ÿ

๐Ÿ‘

โˆ’๐Ÿ

๐’…๐’™

๐Ÿ’

=๐Ÿ

๐Ÿ’โˆซ(๐’™๐Ÿ + ๐Ÿ โˆ’ ๐Ÿ๐’™)๐’…๐’™

๐Ÿ‘

โˆ’๐Ÿ

=๐Ÿ

๐Ÿ’[๐’™๐Ÿ‘

๐Ÿ‘+ ๐’™ โˆ’

๐Ÿ๐’™๐Ÿ

๐Ÿ]

โˆ’๐Ÿ

๐Ÿ‘

=๐Ÿ’

๐Ÿ‘

Option (b)

Page 4: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

6. The auto-correlation function of an energy signal has

(a) no symmetry

(b) conjugate symmetry

(c) odd symmetry

(d) even symmetry

[GATE 1996: 2 Marks]

Soln. The auto correlation is the correlation of a function with itself. If the

function is real, the auto correlation function has even symmetry.

๐‘น๐‘ฟ(๐‰) = ๐‘น๐‘ฟ(โˆ’๐‰)

The autocorrelation function has conjugate symmetry

๐‘น๐‘ฟ(๐‰) = ๐‘น๐‘ฟโˆ— (๐‰)

Option (b) and (d)

7. The power spectral density of a deterministic signal is given by

[sin(๐‘“)/๐‘“]2, where โ€˜fโ€™ is frequency the autocorrelation function of this

signal in the time domain is

(a) a rectangular pulse

(b) a delta function

(c) a sine pulse

(d) a triangular pulse

[GATE 1997: 2 Marks]

Soln. The Fourier transform of autocorrelation function ๐‘น๐‘ฟ(๐‰)

=๐Ÿ

๐Ÿ๐…โˆซ ๐‘ญ(๐Ž)

โˆž

โˆ’โˆž

๐‘ญโˆ—(๐Ž)๐’†๐’‹๐Ž๐‰๐’…๐Ž

๐‘น๐‘ฟ(๐‰) =๐Ÿ

๐Ÿ๐…โˆซ |๐‘ญ(๐Ž)|๐Ÿ

โˆž

โˆ’โˆž

๐’†๐’‹๐Ž๐‰๐’…๐Ž

๐‘น๐‘ฟ(๐‰) = ๐‘ญโˆ’๐Ÿ[|๐‘ญ(๐Ž)|๐Ÿ]

= Fourier inverse of power spectral density.

The auto correlation function and power spectral density make the

Fourier transfer pair

๐‘น๐‘ฟ(๐‰) โ†” ๐‘ฎ๐‘ฟ(๐Ž)

Page 5: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

๐‘น๐‘ฟ(๐‰) = ๐‘ญโˆ’๐Ÿ [๐’”๐’Š๐’ ๐’‡

๐’‡]

๐Ÿ

Inverse Fourier transform of square of sinc function is always a

triangular signal in time domain

Option (d)

8. A probability density function is given by ๐‘ƒ(๐‘ฅ) = ๐พ ๐‘’๐‘ฅ๐‘(โˆ’๐‘ฅ2/2), โˆ’โˆž <

๐‘ฅ < โˆž. The value of K should be

(a) 1

โˆš2๐œ‹

(b) โˆš2

๐œ‹

(c) 1

2โˆš๐œ‹

(d) 1

๐œ‹โˆš2

[GATE 1998: 1 Mark]

Soln. Gaussian Probability density of a random variable X is given by

๐‘ท๐‘ฟ(๐’™) =๐Ÿ

โˆš๐Ÿ๐…๐ˆ๐Ÿ๐’†

โˆ’[(๐’™โˆ’๐)๐Ÿ

๐Ÿ๐ˆ๐Ÿ ]

When ๐ˆ = ๐Ÿ ๐’‚๐’๐’… ๐ = ๐ŸŽ (zero mean)

๐‘ท๐‘ฟ(๐’™) =๐Ÿ

โˆš๐Ÿ๐…๐’†

โˆ’๐’™๐Ÿ

๐Ÿ

๐‘ฎ๐’Š๐’—๐’†๐’ ๐‘ท(๐’™) = ๐’Œ๐’†โˆ’๐’™๐Ÿ

๐Ÿ

๐‘บ๐’, ๐’Œ =๐Ÿ

โˆš๐Ÿ๐…

Option (a)

9. The amplitude spectrum of a Gaussian pulse is

(a) uniform

(b) a sine function

(c) Gaussian

(d) an impulse function

Page 6: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

[GATE 1998: 1 Mark]

Soln. The Fourier transform of a Gaussian signal in time domain is also

Gaussian signal in the frequency domain

๐’†โˆ’๐…๐’•๐Ÿโ†” ๐’†โˆ’๐…๐’•๐Ÿ

Option (c)

10. The ACF of a rectangular pulse of duration T is

(a) a rectangular pulse of duration T

(b) a rectangular pulse of duration 2T

(c) a triangular pulse of duration T

(d) a triangular pulse of duration 2T

[GATE 1998: 1 Mark]

Soln. Autocorrelation function of a rectangular pulse of duration T is a

triangular pulse of duration 2T

The autocorrelation function is an even function of ๐‰

Option (d)

11. The probability density function of the envelope of narrow band

Gaussian noise is

(a) Poisson

(b) Gaussian

(c) Rayleigh

(d) Rician

[GATE 1998: 1 Mark]

Soln. The Probability density function of the envelope of narrowband

Gaussian noise is Rayleigh.

Option (c)

Page 7: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

12. The PDF of a Gaussian random variable X is given by

๐‘ƒ๐‘‹(๐‘ฅ) =1

3โˆš2๐œ‹๐‘’

โˆ’(๐‘ฅโˆ’4)2

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The probability of the event {X=4} is

(a) 1

2

(b) 1

3โˆš2๐œ‹

(c) 0

(d) 1

4

[GATE 2001: 1 Mark]

Soln. The probability distribution function of a Gaussian random variable

X is

๐‘ท๐‘ฟ(๐’™) =๐Ÿ

๐Ÿ‘โˆš๐Ÿ๐…๐’†

โˆ’(๐‘ฟโˆ’๐Ÿ’)๐Ÿ

๐Ÿ๐Ÿ–

The probability of a Gaussian random variable is defined for the

interval and not at a point. So at X = 4, it is zero

Option (c)

13. A 1 mW video signal having a bandwidth of 100 MHz is transmitted to a

receiver through a cable that has 40 dB loss. If the effective one-sided

noise spectral density at the receiver is 10-20 Watt/Hz, then the signal-to-

noise ratio at the receiver is

(a) 50 dB

(b) 30 dB

(c) 40 dB

(d) 60 dB

[GATE 2004: 2 Marks]

Soln. Signal power = ๐‘ท๐‘บ = ๐Ÿ๐’Ž๐’˜

Noise power = ๐‘ท๐‘ต = ๐‘ต๐ŸŽ๐‘ฉ

๐‘ต๐ŸŽ = Noise spectral density = ๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ

B = bandwidth = 100 MHz

๐‘บ๐‘ต๐‘น =๐‘ท๐‘บ

๐‘ท๐‘ต=

๐Ÿ๐ŸŽโˆ’๐Ÿ‘

๐Ÿ๐ŸŽโˆ’๐Ÿ๐ŸŽ ร— ๐Ÿ๐ŸŽ๐ŸŽ ร— ๐Ÿ๐ŸŽ๐Ÿ”

= ๐Ÿ๐ŸŽ๐Ÿ— = ๐Ÿ—๐ŸŽ๐’…๐‘ฉ

Page 8: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

Cable loss = 40 dB

SNR at receiver = 90 โ€“ 40

= 50 dB

Option (a)

14. A random variable X with uniform density in the interval 0 to 1 is

quantized as follows:

If 0 โ‰ค ๐‘‹ โ‰ค 0.3 ๐‘ฅ๐‘ž = 0

If 0.3 < ๐‘‹ โ‰ค 1, ๐‘ฅ๐‘ž = 0.7

Where ๐‘ฅ๐‘žis the quantized value of X

The root-mean square value of the quantization noise is

(a) 0.573

(b) 0.198

(c) 2.205

(d) 0.266

[GATE 2004: 2 Marks]

Soln.

0

1

1x

๐ŸŽ โ‰ค ๐‘ฟ โ‰ค ๐ŸŽ. ๐Ÿ‘ ๐’™๐’’ = ๐ŸŽ

๐ŸŽ. ๐Ÿ‘ โ‰ค ๐‘ฟ โ‰ค ๐Ÿ ๐’™๐’’ = ๐ŸŽ. ๐Ÿ•

๐’™๐’’ is the quantized value of random variable X.

Mean square value of the quantization noise

= ๐‘ฌ [(๐‘ฟ โˆ’ ๐’™๐’’)๐Ÿ

]

= โˆซ(๐’™ โˆ’ ๐’™๐’’)๐Ÿ

๐Ÿ

๐ŸŽ

๐’‡๐‘ฟ(๐’™)๐’…๐’™

Page 9: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

= โˆซ (๐’™ โˆ’ ๐ŸŽ)๐Ÿ๐’…๐’™

๐ŸŽ.๐Ÿ‘

๐ŸŽ

+ โˆซ(๐’™ โˆ’ ๐ŸŽ. ๐Ÿ•)๐Ÿ๐’…๐’™

๐Ÿ

๐ŸŽ.๐Ÿ‘

= [๐’™๐Ÿ‘

๐Ÿ‘]

๐ŸŽ

๐ŸŽ.๐Ÿ‘

+ โˆซ (๐’™๐Ÿ + ๐ŸŽ. ๐Ÿ’๐Ÿ— โˆ’๐Ÿ. ๐Ÿ’

๐Ÿ๐’™) ๐’…๐’™

๐Ÿ

๐ŸŽ.๐Ÿ‘

๐ˆ๐Ÿ = ๐ŸŽ. ๐ŸŽ๐Ÿ‘๐Ÿ—

Root mean square value of the quantization noise

๐ˆ = โˆš๐ŸŽ. ๐ŸŽ๐Ÿ‘๐Ÿ— = ๐ŸŽ. ๐Ÿ๐Ÿ—๐Ÿ–

Option (b)

15. Noise with uniform power spectral density of ๐‘0(๐‘Š/๐ป๐‘ง) is passed

through a filter ๐ป(๐œ”) = 2๐‘’๐‘ฅ๐‘(โˆ’๐‘—๐œ”๐‘ก๐‘‘) followed by an ideal low pass

filter of bandwidth B Hz. The output noise power in Watts is

(a) 2 N0B

(b) 4 N0B

(c) 8 N0B

(d) 16 N0B

[GATE 2005: 2 Marks]

Soln.

The output power spectral density of noise

๐‘ต๐’๐’–๐’• = |๐‘ฏ(๐Ž)|๐Ÿ๐‘ต๐’Š

= 4 N0

The output noise power ๐‘ท๐‘ต = ๐Ÿ’๐‘ต๐ŸŽ๐‘ฉ

The output power ๐‘ท๐‘ต = ๐Ÿ’๐‘ต๐ŸŽ๐‘ฉ

Option (b)

Page 10: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

16. An output of a communication channel is a random variable v with the

probability density function as shown in the figure. The mean square

value of v is

p(v)

v0 4

k

(a) 4

(b) 6

(c) 8

(d) 9

[GATE 2005: 2 Marks]

Soln. Area under the probability density function = 1

So, ๐Ÿ

๐Ÿร— ๐Ÿ’ ร— ๐’Œ = ๐Ÿ

๐’Œ =๐Ÿ

๐Ÿ

The mean square value of the random variable X

๐‘ฌ[๐‘ฟ๐Ÿ] = โˆซ ๐’™๐Ÿ๐’‡๐‘ฟ(๐’™)๐’…๐’™

๐Ÿ’

๐ŸŽ

๐’€ = ๐’Ž๐’™ + ๐‘ช =๐’Œ

๐Ÿ’๐’™

= โˆซ ๐’™๐Ÿ.๐’™

๐Ÿ–๐’…๐’™

๐Ÿ’

๐ŸŽ

=๐’™๐Ÿ’

๐Ÿ– ร— ๐Ÿ’|

๐ŸŽ

๐Ÿ’

=๐Ÿ’๐Ÿ’

๐Ÿ–ร—๐Ÿ’= ๐Ÿ–

Option (c)

Page 11: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

Common Data for Questions 20 and 21

Asymmetric three-level midtread quantizer is to be designed assuming

equiprobable occurrence of all quantization levels.

17. If the probability density function is divided into three regions as shown

in the figure, the value of a in the figure is

Region 2 Region 3

1/4

1/8

X

+3+1+a-a

-1-3

Region 1

(a) 1/3

(b) 2/3

(c) 1/2

(d) 1/4

[GATE 2005: 2 Marks]

Soln. The area under the Pdf curve must be unity. All three regions are

equi -probable, thus area under each region must be ๐Ÿ

๐Ÿ‘.

Area of region ๐Ÿ = ๐Ÿ๐’‚ ร—๐Ÿ

๐Ÿ’

๐Ÿ๐’‚

๐Ÿ’=

๐Ÿ

๐Ÿ‘ ๐’๐’“ ๐’‚ =

๐Ÿ

๐Ÿ‘

Option (c)

18. The quantization noise power for the quantization region between โ€“a and

+a in the figure is

(a) 4

81

(b) 1

9

(c) 5

81

(d) 2

81

[GATE 2005: 2 Marks]

Soln. The quantization noise power for the region between โ€“a and +a in the

above figure is

Page 12: Probability and Random Processes (Part I)...2. White Gaussian noise is passed through a linear narrow band filter. The probability density function of the envelope of the noise at

๐‘ต๐’’ = โˆซ ๐’™๐Ÿ๐‘ท(๐‘ฟ)๐’…๐’™

๐’‚

โˆ’๐’‚

= ๐Ÿ โˆซ ๐’™๐Ÿ๐Ÿ

๐Ÿ’๐’…๐’™

๐’‚

๐ŸŽ

=๐Ÿ

๐Ÿ’[๐’™๐Ÿ‘

๐Ÿ‘]

๐ŸŽ

๐’‚

=๐Ÿ

๐Ÿ’ร—

๐’‚๐Ÿ‘

๐Ÿ‘=

๐’‚๐Ÿ‘

๐Ÿ”

๐’‚ =๐Ÿ

๐Ÿ‘

๐‘บ๐’, ๐‘ต๐’’ =๐Ÿ๐Ÿ‘

๐Ÿ๐Ÿ• ร— ๐Ÿ”=

๐Ÿ’

๐Ÿ–๐Ÿ

Option (a)

19. A zero-mean white Gaussian noise is passed through an ideal lowpass

filter of bandwidth 10 KHz. The output is then uniformly sampled with

sampling period ๐‘ก๐‘† = 0.03 msec. The samples so obtained would be

(a) correlated

(b) statistically independent

(c) uncorrelated

(d) orthogonal

[GATE 2006: 2 Marks]

Soln. White noise contains all frequency components, but the phase

relationship of the components is random. When white noise is

sampled, the samples are uncorrelated. If white noise is Gaussian, the

samples are statistically independent

Option (b)