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An in-depth exploration of the exponential and erlang distributions, including their probability density functions (pdfs), mean and variance calculations, and problem-solving examples. The exponential distribution is discussed as a memoryless distribution, and its relationship to the erlang distribution is explained. The document also includes examples of how these distributions can be applied to real-world scenarios, such as waiting times for customers.
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Exponential and Erlang
Delta
Problem Solving Examples
Reading:
G. R. Cooper & C. D. McGillem 2.6 - 2.
EE/STAT 322, #
The PDF is given by
f X
(^) ( x ) =
τ 1 (^) e −
τ^1 (^) x
x
otherwise
τ (^) , and
σ x 2
=
τ (^2) .
∞ 0
f (^) ( x ) xdx
∞ 0
τ 1 (^) e
−
τ^1 (^) x
xdx
By integrating by parts (
xdy
xy
ydx
), we get
∞
0
xde
−
τ^1 (^) x
xe
−
τ^1 (^) x | 0 ∞
∞
0
e −
τ^1 (^) x
dx
τ
EE/STAT 322, #
Example:
The waiting time of a customer has an exponential distribution
with a mean of 5 minutes.
Then what is the probability that he will wait
Solution:more than 10 minutes?
τ
Pr(
e −
10
/ τ = e − 2
another 10 minutes is given byIf he already spent five minutes there, the chance that he needs to wait
Pr(
e −
15
/ τ /e^
−
5 / τ
= Pr(
EE/STAT 322, #
Exponential distribution:
arrival interval between the first and second
Erlang: arrival interval between the first and the fourth customers (fig. b).customers (fig. a);
t
-- events
t
(a)
(b)
EE/STAT 322, #
f (^) ( x ) =
p 1 δ ( x − x 1
p 2 δ ( x − x 2 ) ,
where
p 1
p 2
= 1
, and
δ ()
is the Kronecker delta function.
x Example: Two possible outcomes of a coin experiment. 1
= 0
for H, and
x 2
= 1
for T, and
p 1
=
p 2
= 0
∞ −∞
x [ p 1 δ ( x − x 1
p 2 δ ( x − x 2
dx
= p 1 x 1 + p 2 x 2.
2 ) =
∞ −∞
x 2 [ p 1 δ ( x − x 1
p 2 δ ( x − x 2
dx
p 1 x 12
p 2 x 22 .
σ X 2
= E ( X 2 ) − X 2 = p 1 p 2 ( x 1 − x 2 ) 2.
EE/STAT 322, #
f Extension: Multiple outcomes. (^) ( x ) =
p i δ ( x − x i )
, where
(^) p
i = 1
p i x i , X 2 = ∑
p i x i 2 (^) ,
σ X 2
2 1
∑
(^) p
i p j ( x i − x j ) 2.
Example:
(Ex 2-7.3)
Three coins are tossed. Let
number of heads
Find
E ( H ) , σ
H 2
(^).
EE/STAT 322, #
Example:
(Problem 2-4.5, textbook) RV
has a pdf of the form
f X
(^) ( x )
ax
2
< x
ax
< x
Find (a) the value of
a , (b)
, (c)
Pr(
(a) We need Solution:
3 0
f X
(^) ( x ) dx
, so that
2 0
ax
2 dx
3 2
ax
ax
3 / 3 | 02
ax
2 / 2 | 23
=
a [
/ 3 + 9
a
(b)
2 0
xax
2 dx
3 2
xaxdx
6 31
(c)
Pr(
3 2
f X
(^) ( x ) dx
3 2
6 31
xdx
EE/STAT 322, #
Example:
(2-5.3) Gaussian RV
has a probability of 0.5 of having value
less than or equal to 1. Further,
Pr(
Find (a)
; (b)
σ x 2 ; (c)
Pr(
(a) Solution:
Pr(
. So
(b)
Pr(
/σ
x ) =
/σ
x ) = 0
Using the inverse of
-function, we get
/σ
x
= 2
, so
σ x 2
= 4
(c)
Pr(
/σ
x ) = Φ(1) = 0
. Alternatively,
Pr(
Pr(
/σ
x ) = 1
EE/STAT 322, #
11
Example:
(2-6.3) A current
with a Rayleigh PDF passes through a
resistor with
π )Ω
A. Power dissipation:
2 .
(a) Find the mean of power dissipated
. (b) Find
Pr(
. (c)
Pr(
(a) Solution:
π/
σ
σ
/π
2 ) =
σ
2 ) = 2
π 2 · 4 · 2
/π
(b)
Pr(
2
≤
2
<
I (^) (
exp(
1 . 382
2
2 σ 2
(c)
Pr(
I (^) (
EE/STAT 322, #
Example:
θ
is uniformly distributed in
π ) .
Another RV
is given by
= cos(
θ ) .
(a) Find PDF of
; (b) Find
; (c) Find
σ x 2 ; (d) Find
Pr(
(a) Solution:
dx/dθ
(^) sin
(^) θ
cos
2 θ = − √ 1 − x 2.
EE/STAT 322, #
At both
θ 1
and
θ 2 , | dx/dθ
| = √ 1 − x 2.
f X
(^) ( x ) =
f (^) ( θ )
√ 1 − x 2 = 1
π √ 1 − x 2 − 1 ≤ x ≤ 1
elsewhere
(b)
[cos(
θ )] =
2 π
0
cos(
θ )
1
2 π (^) dθ
(c)
2 ) =
2
=
[cos
2 θ ] =
2 π
0
cos
2 ( θ )
1
2 π (^) dθ
2 1 .
σ x 2
= X 2 − X 2 = X 2 =
2 1 .
EE/STAT 322, #
(d)
Pr(
1 0 . 5 f X
(^) ( x ) dx
1 0 . 5
1
π √ 1 − x 2
(^) dx
Procedure: Let
x
= cos(
θ ) , for
θ
∈
, π/
So
dx
sin
θdθ
1
√ 1 − x 2 = 1
sin
(^) θ (^).
x
θ
= cos
−
1 (1) = 0
x
θ
= cos
− 1 (
π/
1
0 . 5
π √ 1 − x 2
(^) dx
0
π/
3
π
sin
(^) θ
( −
(^) sin
(^) θ
) dθ
π/
3
0
π 1
dθ
EE/STAT 322, #