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108

Volume-4, Issue-1, February-2014,ISSN No.: 2250-0758

International Journal of Engineering and Management Research

Available at:

Page Number: 108-116

Reliability Evaluation for Power Distribution System

Dr. Reena Garg

Assistant Professor, YMCA University, Faridabad, Haryana, INDIA

ABSTRACT

In this model, the authors have evaluated availability and profit function for a power distribution system. Since the system is of non-Markovian nature, the supplementary variables have introduced to make the system Markovian. All the failures follow exponential time distribution whereas all the repairs follow general time distribution. System configuration has shown in

fig.1. Laplace-transform and supplementary

variables technique have used to solve and formulated the mathematical model, respectively. Steady-state behavior of the system and a particular case has also been obtained to improve the practical utility of the model.

Keywords: Markovian process,

supplementary variables, steady state behavior, Laplace-transform.

I. INTRODUCTION

The authors have considered a power distribution system, in this model, to evaluate some reliability parameters. The whole system is divided in to two subsystems, namely A and B, connected in series. The whole system can fail due to failure of its either subsystems, due to environmental reasons and due to human error. The subsystem A is power generation system and it has M non-identical power plants connected in parallel redundancy. The subsystem A is of 2- out of M: F nature. The subsystem B is power

distribution system and it contains N- non-identical units (as shown in fig. 1) connected in series. The subsystem A is of 1-out of N:F nature. The state-transition diagram has shown in fig.2. Some important reliability parameters together with a numerical example and graphical illustrations have appended at the end to show the practical utility of the model.

II. ASSUMPTIONS

The following assumptions are associated with this model:

(1) Initially, all the components are in operable condition of full efficiency.

(2) Failures are statistically independent.

(3) The subsystem B is of nature 1-out-of –M: D.

(4) All the failures follow exponential time distribution where as all the repairs follow general time distribution.

(5) System may be fail due to environmental reasons and human error.

(6) Repair facilities are always available.

(7) After repair system works like a new one and

never damages anything.

(8)

III. NOTATIONS

The following notations have been used throughout this model:

(2)

109 Fig.1 (System Configuration)

1

2

3

4

Transmission Substations

Transmission Lines

Power Substations

Transformer Power Poles

(3)

110 Fig. 2. State-transition Diagram

P0,j(x,t)∆/Pi,F(y,t)∆ :The probability that at time ‘t’ the system is in failed state due to failure

of (jth-B)/(ith-A and jth-B) component and elapsed repair time lies in the interval (x, x+∆) / (y, y+∆) .

Pi,0(y,t)∆/PF,0(z,t)∆ :The probability that at time ‘t’ , the system is in degraded/failed state due

to failure of ith

–A/2-A components and elapsed repair time lies in the interval (y, y+∆) /(z, z+∆) .

j

P0,

Operable

) (reducedefficiencystates Degraded

= = 1

1 2

M

i i

α α

= = M

i i

1

1 α

α µi(y)

1 e

2 h

λ

) (y

i

µ λ

) (x

j

µ

) (k

γ

Failed φ

Pi, 0 (0, t)

Pi, 0 (y, t)

P0, 0 (t)

PE (0, t)

PE (r, t)

PH (0, t)

PE (k, t)

1 h

PH (0, t)

PE (k, t)

PF, 0 (0, t)

PF, 0 (z, t)

Pi, F (0,t)

Pi, F (y,t)

) (z

µ 2 e

(4)

111 PE(r,t)∆/PH(k,t)∆ :The probability that at time ‘t’, the system is in failed state due to

environmental reasons/human error and elapsed repair time lies in the interval (r, r+∆)/(k, k+∆).

αi/λj : Failure rate of ith-A/jth-B component.

e1/e2

h

: Failure rate due to environmental reasons.

1/h2

β(r)∆/γ(k)∆ : Probability that system will be repaired from environmental failure/human error in time interval (r, r+∆)/(k, k+∆) conditioned that it was not repaired up to time r/k.

: Failure rate due to human error.

µi(y)∆/ µj(x)∆/ µ(z)∆: Probability that ith-A/jth

) (s F

-B/2A components will be repaired in the time interval (y, y+∆)/(x, x+∆)/(z, z+∆) , conditioned that it was not repaired up to the time y/x/z.

: Laplace transform of the function F(t).

Pup(t)/ Pdown(t) : Probability that at time t , the system is in up/down state.

IV. FORMULATION OF MATHEMATICAL MODEL

By the elementary probability consideration and continuity argument, we may obtain the following set of difference-differential equations for the stochastic process, which is continuous in time and discrete in space:

+ +

+ =

  

+ + + +

∞ ∞

dk k t k P dy y t y P dx x t x P t P h e dt

d

H i

i j

j( , ) ( ) ( , ) ( ) ( , ) ( )

) (

0 0

0 , 0

, 0 0

, 0 1 1

1 µ µ γ

α λ

dz z t z P dr r t r

PE( , ) ( ) F ( , ) ( )

0 0 , 0

µ

β

+ (1)

0 ) , ( )

( 0, =



+

∂ ∂ + ∂

t x P x t

x µj j (2) 0

) , ( )

( ,0

2 2

2  =

  

 

+ + + + + ∂

∂ + ∂

t y P y e

h t

y α λ µi i (3) 0

) , ( )

( ,0 =

  

+

∂ ∂ + ∂

t z P z t

z µ F (4) )

, ( )

, ( )

(y P, y t P,0 y t t

y µi iFi

 

 

+ ∂

∂ + ∂

(5) 0

) , ( )

( =

  

+

∂ ∂ + ∂

t r P r t

r β E (6) 0

) , ( )

(  =



+

∂ ∂ + ∂

t k P k t

(5)

112 Boundary Conditions are

dy y t y P t P t

P j(0, ) ( ) iF( , ) i( )

0 , 0 , 0 ,

0 λ

µ

∞ +

= (8)

) ( )

, 0

( 1 0,0

0

, t P t

Pi =α (9) )

( )

, 0

( 2 ,0

0

, t P t

PFi (10)

0 ) , 0 (

, t =

PiF (11) ) ( ) ( ) , 0

( t e1 P0,0 t e2 P,0 t

PE = + i (12)

) ( ) ( ) , 0

( t h1 P0,0 t h2 P,0 t

PH = + i (13) Initial conditions are

1 ) 0 ( 0 , 0 =

P ; Otherwise all state probabilities are zero. (14) V. SOLUTION OF MATHEMATICAL MODEL

Taking Laplace Transforms of equations (1) through (13), subjected to (14) and then on solving them one by one , we may obtained the following Laplace transforms of different state

probabilities: ) ( 0 , 0 s P = ) ( 1 s

A (15)

) ( )}] ( ) ( { 1 [ ) ( )

( 2 2 2

2 2 2

1 ,

0 S s S s h e Dj s

e h s

A s

P j ii + + + +

+ + + +

= λ α

α λ α λ (16)

[

( )

]

) ( )

( 1 2 2 2

0

, D s h e

s A s

Pi = α i +λ+α + + (17)

[

( )

]

( )

) ( )

( 2 2 2

2 1 0

, D s h e D s

s A s

PF = i +λ+α + +

α α (18)

[

( ) ( )

]

) )( ( )

( 2 2 2

2 2 2

1

, D s D s h e

e h s

A s

PiF ii + + + +

+ + +

= λ α

α λ λα (19) ) ( )] ( [ ) ( 1 )

( e1 e2 1D s 2 h2 e2 D s

s A s

PE = + α i +λ+α + + β (20)

) ( )] ( )[ ( )

(s P0,0 s h1 h2 1D s 2 h2 e2 D s

PH = + α i +λ+α + + γ (21)

where, B B S B D A A ) ( 1 )

( = − , for all A and B.

and A(s)= s+λ+α1+h1+e11 Si (s+λ+α2+h2+e2)

) ( )}] ( ) ( { 1

[ 2 2 2

2 2 2

1 S s S s h e S s

e

h + ii + + + + j

+ + +

− λ α

α λ

α

λ

-α1α2Di(s+λ+α2 +h2+e2)S(s)

- [e1+e2α1Di(s+λ+α2+h2 +e2)]Sβ(s)

(6)

113 Also, it is interesting to note that

) ( 0 ,

0 s

P +P0,j(s)+

s s P s P s P s P s

Pi F iF E H

1 ) ( ) ( ) ( ) ( )

( ,0 ,

0

, + + + + = (23)

VI. STEADY-STATE BEHAVIOR OF THE SYSTEM

By using Abel’s lemma, viz; sP s P t P

t

s→ ( )=lim→∞ ( )=

lim

0 (say) ;Provided the limit on R.H.S. exist,

we have the following time independent state probabilities from equations (15) through (21): ) 0 ( 1 0 , 0 A P

= (24)

Tj e h S e h A

P j [1 {1 i( )}]

) 0

( 2 2 2 2 2 2

1 ,

0 = ′ +λ+α + + − λ+α + +

α λ (25)

[

( )

]

) 0

( 2 2 2

1 0

, D h e

A

Pi = i λ+α + +

α

(26)

[

D h e

]

T

A

PF i( )

) 0

( 2 2 2

2 1 0

, = ′ λ+α + +

α α (27)

[

( )

]

) )( 0

( 2 2 2 2 2 2

1

, T D h e

e h A

PiF ii + + +

+ + + ′

= λ α

α λ λα (28) β α λ

α D h e T

e e A

PE [ i( )]

) 0 ( 1 2 2 2 1 2

1+ + + +

= (29)

γ α

λ

α D h e T

h h A

PH [ i( )]

) 0 ( 1 2 2 2 1 2

1+ + + +

= (30)

where, 0 ) ( ) 0 ( =     = ′ s s A ds d

A and Tj =−Si'(0)etc.

VII. PARTICULAR CASE

When all the repairs follow exponential time distribution

Setting Si(s)= i i

s µ µ

+ etc. in equations (15) through (21), we obtain the following Laplace

transforms of various state probabilities:

) ( 0 , 0 s P = ) ( 1 s

B (31)

i i i i i j s e h s s e h s B s P µ µ α λ µ µ µ α λ α λ + + + + + + − + + + + +

= [1 { }] 1

) ( ) ( 2 2 2 2 2 2 1 ,

0 (32)

i i

e

h

s

s

B

s

P

µ

α

λ

α

+

+

+

+

+

=

2 2 2 1 0 ,

1

)

(

)

(7)

114 ) )( ( 1 ) ( ) ( 2 2 2 2 1 0

, λ α µ µ

α α + + + + + + = s e h s s B s P i

F (34)

      + + + + + − + + + + = i i F i e h s s e h s B s P µ α λ µ α λ λα 2 2 2 2 2 2 1 , 1 1 ) )( ( )

( (35)

1 2 1 [ ) ( 1 )

( e eα

s B s

PE = +

i

e h

s+λ+α2+ 2 + 2+µ 1 ] β + s 1 (36) 1 2 1 [ ) ( 1 )

( h hα

s B s

PH = +

i

e h

s+λ+α2+ 2+ 2+µ 1 ] γ + s 1 (37) where,

B(s)= s+λ+α1+h1+e1

-i i

e h

s λ α µ

µ α + + + +

+ 2 1 2 2 − [1+λ+α2 +1h2+e2 α λ       + + + + + −

+i i s ih e i

s λ α µ

µ µ µ 2 2 2 ] j j s µ µ + µ µ µ α λ α α + + + + + + − s e h

s 2 2 2 i

2 1 β β µ α λ α +       + + + + + + − s e h s e e i 2 2 2 1 2 1 1 γ γ µ α λ λ +       + + + + + + − s e h s h h i 2 2 2 1 2

1 (38)

VIII. UP AND DOWN STATE PROBABILITIES

We have } ) ( exp{ } ) ( exp{ ) 1 ( )

(t c 1 e1 h1 t c 2 h2 e2 t

PUp = + − λ+α + + − − λ+α + + (39) where, C=

1 1 1 2 2 2 1 e h e

h + − − −

+ α

α

α

(40) Also, Pdown(t)=1−PUp(t) (41)

IX. PROFIT FUNCTION

The profit function for the considered system is given by 3

0

2

1 ( )

)

(t C P t dt C t C

G

t

Up − −

=

where, C1 and C2 are revenue and repair costs per unit time and C3

{

}

{

}

2 3

) ( 2 2 2 ) ( 1 1 1 1 2 2 2 1 1 1 1 1 1 )

( e Ct C

e h C e h e C C t

G e h t h e t − −

     − + + + − − + + + +

= −λ+α + + −λ+α + +

α λ α

λ

is system establishment cost per set up. So, have

(8)

115 X. NUMERICAL COMPUTATION

For a numerical comput ation, let us consider the values:

time unit per Rs

C h

h e

e 0.01, 0.02, 0.03, 0.035, .7.00 ,

07 . 0 , 06 . 0 , 001 .

0 1= 2 = 1 = 2 = 1= 2 = 1 =

= α α

λ

C2 = Rs. 2.00 per unit time , C3

By using these values in equations (39),(41) and (42), we may observe the changes in values of corresponding reliability parameters.

= Rs. 10.00 per set up and t = 0,1,2 .. .. .. .. .. ..

where C= 2.4

025 .

06 . 1 . 125 .

06

. = =

PUp(t)=3.4 e-0.101t -2.4 e-0.126t

{

}

{

1

}

2 10

126 .

4 . 2 1

101 .

4 . 3 7 )

(t = e−.101 − −e−0.126 t

G t

and

XI. RESULTS & DISCUSSION

In this model, the authors have evaluated availability and profit function for a power distribution system. Since the system is of non-Markovian nature, the supplementary variables have been introduced to make the system Markovian. These supplementary variables disappear at the solution stage.

We compute the table-1 and 2 for the considered numerical example. The corresponding graphs have shown in the fig-3 and 4. Table-1 shows that how the availability of the power plant decreases as we make increase in the value of time. Availability decreases approximately in a constant manner.

From table-2 we observe that from t= 0 to 2 the profit function is negative. This shows that there is no profit up to t=2 because initially we only have to spend money to establish the system and initial repairs. After t=2 , we recover the system establishment cost and so it becomes positive. Thus after t=2 profit function increases in uniform way.

0 0.2 0.4 0.6 0.8 1 1.2

0 1 2 3 4 5 6 7 8 9 10 11 12

Pup(t)

Table-1

t

Fig 3 t PUp(t)

0 1.0 1 0.9568 2 0.91286 3 0.86644 4 0.80536 5 0.74786 6 0.7279 7 0.68318 8 0.63962 9 0.59778 10 0.5574 11 0.51904 12 0.48264

(9)

116

-15 -10 -5 0 5 10 15 20 25 30

0 1 2 3 4 5 6 7 8 9 10 11 12

G(t)

t Fig 4

Table-2

REFERENCES

[1] Cassady, C.R.; Lyoob, I.M.; Schneider, K.; Pohi, E.A. : “A generic model of equipment availability under imperfect maintenance”, IEEE TR. On reliability, vol.54, issue-4, PP. 564-571, 2005.

[2] Fang-Ming, S.; Xuemin, S.; Pin-Han, H.: “Reliability optimization of distributed access networks with constrained total cost’’, IEEE TR. on reliability, vol.54, Issue-3, PP 421-430, 2005.

[3] Sim, S.H.; Endrenyi, J.: “A failure-repair model with minimal and major maintenance”, IEEE TR. on reliability, vol.55, issue-1, P.P. 134-140, 2006.

[4] Wang, F.K.: “Quality evaluation of a manufactured product with multiple characteristics” , Quality and Reliability engineering , vol. 22, issue-2, P.P.225-236,2006.

t G(t) 0 -10 1 -5.112112 2 -0.6085219 3 3.6223846 4 8.3526956 5 12.543772 6 14.364086 7 17.298193 8 19.934112 9 22.259432 10 24.311971 11 26.079316 12 27.578826

G(t)

Figure

Fig. 2. State-transition Diagram
Table-2

References

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