Memoryless Sysrtems Part 3-Probability and Statistics-Assignment Solution, Exercises of Probability and Statistics

Sir Tanika Mukopadhyay taught us Probability at Homi Bhabha National Institute. He gave us assignments so that we can practice what we learned in form of problems. Here is solution to those problems. Its main emphasis is on following points: Analysis, Stochastic, Systems, Guassian, Power, Easily, Shown, leads, Consequently, Gaussian, Variables

Typology: Exercises

2011/2012

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1
ECE 863 – Analysis of Stochastic Systems
Fall 2001
Solutions for Homework Set #3
Problem 1
3.51 P Y 3.5d P Y 3.5d edx
3d x
===-=
-•
-zaa
2
α
=1-3 d
2e
P Y 2.5d P Y 2.5d e
2dx
3d
2d x
===-=
-
-zaa
=-
--
1
2ee
2d 3daa
ot
Similarly,
{}
αα
=== =


-d -2d
1
PY 1.5d PY -1.5d e e
2
P Y 0.5d P Y 0.5d 1
21e
d
===-=-
-a
ot
PY 4d 2 e
2dx e
4d
x4d
>= =
-
-
zaa
a
docsity.com
pf3
pf4
pf5
pf8
pf9

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1

ECE 863 – Analysis of Stochastic Systems

Fall 2001

Solutions for Homework Set

Problem 1

3.51 P Y 3.5d P Y 3.5d e^ dx

3d x = = = - =

z

a a 2

= 1 -3^ α^ d 2 e

P Y 2.5d P Y 2.5d e 2

dx 3d

2d x = = = - =

z

a a

= 1 -^ - -

oe 2 ad^ e^3 adt

Similarly,

 =  =  =  = { - α^ d^ − -2α^ d}

P Y 1.5d P Y -1.5d 1 e e 2

P Y 0.5d P Y 0.5d 1 2

= = = - = o 1 - e -adt

P Y 4 d 2 e 2

dx e 4 d

x (^4) d > = =

  • -^ -

z

a a^ a

2

Problem 2

3.53 When X is Gaussian

fi Y = a X + b is also Gaussian where:

m' = E Y = a E X + b = a m +b

b g^ s '^2 =^ a^2 s^2 fi^ a^ =^ s s

b = m' - ms s

Problem 3

3.56 Power = P =R X^2

F y P R X y

F y / R F y / R y 0

p^2

X X

b g

e (^) j e (^) j

fi = +

f y

f y / R 2R y / R

f y / R 2R y / R

f y / R f y / R 2 R y

p

x x

x x

b g

e j e j

e j e j

fi f y 1 2 R y

p 2 e

y 2^2 R b g =^

  • FH IK p s

/ s

4

Problem 5

3.59 (a) For y £ 0 P Y £ y = 0

y > 0

( )

( ) ( )

X

X

Y X

P Y y P e y P X ln (y)

F ln (y)

0 y 0 F y F ln (y) y 0

 ≤^  =^ ^ ≤^  =^  ≤ 

fi " y > 0

f y d d y

F y

d d y

F ln y d d y

ln y

f ln y 1 y

f ln y y

Y Y

X

X

x

b g b g

d c b ghi c b gh

c b gh

c b gh

(b) For a Gaussian RV X,

f y

0 y 1 2 y

Y (^) e ln y^ m y 0 b g = c b g h^2 2

R S

|

T|^

p s

/ s

Problem 6

E X kP x k

k n

n n 1 2n

n 1 2

k 1

n

k 1

n

= = +^ = +

=

=

Â

Â

b g

5

sx^2 = E X^2 - (^) cE X h^2

E X k n

n 1 2n 1 6

2 k 1

n 2 = = +^ + =

Â

b gb g

fi sx^2 = - n^2 12

Problem 7

3.67 (a) E X k k!

e k 1!

e k 0

k k 1

k 1 = = = -

  • (^) -

  • -^ -

 Â

l (^) l (^) l l l b g

= l el e-l = l

E X k k!

e k k 1!

e

j 1 j!

e where j k 1

1

2 2 k k 1

k 1

j 0

j

2

 Â

Â

  • =
  • -^ -

=

  • (^) -

l (^) l l

l l

l l l l

l l

l

b g

b g

l q

fi s (^) x^2 = l^2 + l - l^2 = l

(b) E X = (^) barrival rate g b∑ time (^) g = lt

Problem 8

3.71 For non-negative random variables one can use the following formula for E X :

[ ] ( (^) X(^ )) 0

E X 1 F x dx

∞ = (^) ∫ −

7

c^ E Y h^2 =^ cE A h^2 Cos^2 b gwt^ +^ 2C Cos^ b gwt E A^ +C^2

fi s (^) Y^2 = Cos^2 b gwt E A^2 - cE A h^2

s (^) Y^2 = s (^) A^2 Cos^2 b gwt

Problem 11

3.76 g X b g =ba X

E g X ba k!

e b a k!

e

be e be

k 0

k k k 0

k

a a 1

b g

b g

b g

=

  • (^) -

  • (^) -

 Â

l (^) l l l

l l l

Problem 12

3.78 E Y[ ] g x f( ) (^) X (^) ( x (^) )dx

− ∞

= (^) ∫

( ) (^ )^ (^ )^ ( ) (^ )

a (^) a X X X a a

x a f x dx 0 f x dx x a f x dx

− (^) ∞

− ∞ −

= (^) ∫ + + (^) ∫ + (^) ∫ −

[ ] ( ) ( ) (^) ( ) ( ( ))

a X X X X a

E Y x f a dx x f x dx aF a a 1 F a

− (^) ∞

− ∞

= (^) ∫ + (^) ∫ + − − −

For Laplacian RV, f x 2 X^ b g^ =^ a^ e-ax

Since fX (^) b gx is symmetric around zero,

a X X a

x f x dx x f x dx

− (^) ∞

− ∞

⇒ (^) ∫ = −∫

8

fi = - - -

= -^ - - =

E Y aF a a 1 F a a 2

e a 2

e 0

X X a a

b g c b gh

a a

( ) (^ )^ ( ) (^ )

a 2 2 2 2 X X a

E Y x a f x dx x a f x dx

− (^) ∞

− ∞

σ = ^  = ∫ + + ∫ −

a a 2 2 X X X X a a

x f x dx x f x dx 2 a x f x dx x f x dx

− (^) ∞ − ∞

− ∞ − ∞

+ a 2 FX b- a g + c 1 - F Xb gah

For Laplacian, this leads to:

a 2 2 2 x 2 x a

E Y x e dx x e dx 2 2

− (^) ∞

  • α − α − ∞

σ =   = α^ + α

using x 2 e x^ dx e^ x 2 x 2

x 3

a a 2 2 a

z =^ da^ -^ a + i

− ∞ ∞

⇒ =  ^ − + ^ − ^ + +  

x -a x 2 2 2 2 2 (^3) - 3 a

σ e^ x 2 x 2 e x 2 x 2 2

= 1 -^ + + + - + +

2 e^ a^2 a^2 2a^2 e^ a^2 a^2 2a^2 a

{ a^ a^ a^ a a^ a }

s a^ a a

2 2 2 a 2 = a^ +^ 2a^ +^2 e-a