role of equilibrium distribution in reliability studies

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Probability in the Engineering and Informational Sciences http://journals.cambridge.org/PES Additional services for Probability in the Engineering and Informational Sciences: Email alerts: Click here Subscriptions: Click here Commercial reprints: Click here Terms of use : Click here ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES Ramesh C. Gupta Probability in the Engineering and Informational Sciences / Volume 21 / Issue 02 / April 2007, pp 315 334 DOI: 10.1017/S0269964807070192, Published online: 27 February 2007 Link to this article: http://journals.cambridge.org/abstract_S0269964807070192 How to cite this article: Ramesh C. Gupta (2007). ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES. Probability in the Engineering and Informational Sciences, 21, pp 315334 doi:10.1017/S0269964807070192 Request Permissions : Click here Downloaded from http://journals.cambridge.org/PES, IP address: 137.99.31.134 on 20 Apr 2013

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Page 1: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

Probability in the Engineering and Informational Scienceshttp://journals.cambridge.org/PES

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Email alerts: Click hereSubscriptions: Click hereCommercial reprints: Click hereTerms of use : Click here

ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

Ramesh C. Gupta

Probability in the Engineering and Informational Sciences / Volume 21 / Issue 02 / April 2007, pp 315 ­ 334DOI: 10.1017/S0269964807070192, Published online: 27 February 2007

Link to this article: http://journals.cambridge.org/abstract_S0269964807070192

How to cite this article:Ramesh C. Gupta (2007). ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES. Probability in the Engineering and Informational Sciences, 21, pp 315­334 doi:10.1017/S0269964807070192

Request Permissions : Click here

Downloaded from http://journals.cambridge.org/PES, IP address: 137.99.31.134 on 20 Apr 2013

Page 2: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

ROLE OF EQUILIBRIUMDISTRIBUTION IN

RELIABILITY STUDIES

RAAAMMMEEESSSHHH C. GUUUPPPTTTAAADepartment of Mathematics and Statistics

University of MaineOrono, ME 04469-5752

E-mail: [email protected]

The equilibrium distribution arises as the limiting distribution of the forward recur-rence time in a renewal process+ The purpose of this article is to study the relation-ships between the equilibrium distributions ~including its higher derivates! and theoriginal distributions+ Some stochastic order relations and the relations between theiraging properties are investigated and some applications in the field of insurance andfinancial investments are given+ In addition, the relation between the equilibrium dis-tribution of a series system and the series system of equilibrium distribution is inves-tigated+Bivariate equilibrium distribution whose reliability properties are consistentwith those of the univariate equilibrium distribution is defined+

1. INTRODUCTION

Let X be a continuous random variable with probability density function ~p+d+f+!f ~x!, distribution function F~x!, and survival function OF~x!�1 � F~x!+We definethe p+d+f+ f *~x!as

f *~x! �OF~x!

µ, x � 0, (1.1)

where µ � E~X ! � `+ Then f *~x! is called the p+d+f+ of an equilibrium distributionor induced distribution+

The above distribution arises as the limiting distribution of the forward recur-rence time in a renewal process+ It also arises as the marginal distribution of W1,where the joint p+d+f+ of ~W1,W2! is given by

Probability in the Engineering and Informational Sciences, 21, 2007, 315–334+ Printed in the U+S+A+DOI: 10+10170S0269964807070192

© 2007 Cambridge University Press 0269-9648007 $25+00 315

Page 3: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

g~w1,w2 ! �f ~w2 !

µ, 0 � w1 � w2 � `

� 0, elsewhere;

see Brown @10# +Note that, in this case, the p+d+f+ of W2 is given by the length-biased version of

the original distribution as

fW2~w2 ! �

w2 f ~w2 !

µ, 0 � w2 � `+

The equilibrium distribution ~1+1! is intimately connected to its parent distri-bution and many of the reliability properties of the original distribution can be eas-ily studied by means of the properties of the equilibrium distribution+

The purpose of this article is to study the relationships between ~1+1! ~includ-ing its higher derivatives! and the original distribution+ Some stochastic order rela-tions and the relations between their aging properties are investigated and someapplications in the field of insurance and financial investments are given+ This isprimarily a review article+ However, the examples in Section 6 are new+

The organization of this article is as follows+ In Section 2 we present somedefinitions and background material encountered in reliability studies, includingsome criteria of aging and their relationships+ Some definitions of stochastic orderrelations and their relationships are also provided+ Section 3 deals with higher-order equilibrium distributions and stop loss moments+ In Section 4 aging proper-ties of equilibrium distributions and their stochastic ordering with the originaldistribution are explored+ In Section 5 the relation between the equilibrium distri-bution of a series system and a series system of equilibrium distributions, consist-ing of two components, is investigated+ Section 6 contains the bivariate equilibriumdistribution along with two examples+ Finally, in Section 7 we provide some con-clusions and comments+

2. DEFINITIONS AND BACKGROUND

Let X be a continuous positive random variable representing a survival time with anabsolutely continuous distribution function F~t !, survival function OF~t !�1 � F~t !,and cumulative hazard rate L~t !� �ln OF~t ! with OF~0!� 1+Wherever necessary, itwill be assumed that rF~t !� L'~t ! is the hazard rate corresponding to F~t !+ A keyrole in this article will be played by the mean residual life function ~MRLF! µF~t !defined as

µF ~t ! � E~X � t 6X � t !�

�t

`

OF~x! dx

OF~t !, t � 0+

316 R. C. Gupta

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It will be assumed that µF~0!� E~X ! � `+ When discussing the variance ofthe residual lifetime X � t 6X � t, it will be assumed that E~X 2!�`+ The varianceresidual life function ~VRLF! is defined as

sF2~t ! � Var~X � t 6X � t !

�2

OF~t !�

t

`�x

`

OF~ y! dy dx � µF2 ~t !, t � 0+

We refer to Gupta and Kirmani @17,18# , Launer @28# , and Gupta, Kirmani, andLauner @19# for details about the MRLF and the VRLF+

The above-defined functions highlight different aspects of survival and re-sidual life distributions+The hazard rate and the mean residual life function arerelated by

rF ~t ! �1 � µF

' ~t !

µF ~t !+ (2.1)

Further, the hazard rate, the MRLF, and the VRLF are tied together by therelation

d

dtsF

2~t ! � rF ~t !$sF2~t !� µF

2 ~t !%; (2.2)

see Gupta @16# +It is well known that rF~t ! determines the distribution function uniquely and,

hence, µF~t ! also characterizes the distribution+ Additionally, OF~t ! and µF~t ! areconnected by

OF~t ! �µF ~0!

µF ~t !exp���

0

t dx

µF ~x!� + (2.3)

Thus, rF~t !, µF~t !, and OF~t ! are equivalent in the sense that given one of them, theother two can be determined+Hence, in the analysis of survival data, one sometimesestimates rF~t ! or µF~t ! instead of OF~t !, according to the convenience of the pro-cedure available+

In addition to the above functions, the residual coefficient of variation is givenby gF~t !�sF~t !0µF~t !+ Further, the MRLF, the VRLF, and the residual coefficientof variation are connected by the relation

d

dtsF

2~t ! � µF ~t !~1 � µF' ~t !!~gF

2~t !� 1!; (2.4)

see Gupta @16# +We now describe briefly some aging classes of life distributions and their

relationships

EQUILIBRIUM DISTRIBUTION IN RELIABILITY 317

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2.1. Some Criteria of Aging for the RLF

In this section we review some of the aging criteria and their relationships+We alsodescribe how the aging properties of the original distribution are transformed intothe aging properties of the residual life+

Let X be a continuous positive random variable representing the life of acomponent+ Let F be the cumulative distribution function of X and OF ~x! �1 � F~x! be the reliability function or the survival function of X+ Then Ft~x! �P~X � x � t 6X � t ! is the survival function of a unit of age t+ Evidently, anystudy of the phenomenon of aging should be based on Ft~x! and functions relatedto this+ Thus, the following hold:

1+ F is said to be PF2 if ln f ~x! is concave, where f ~{! is the density corre-sponding to F~{!+

2+ F is said to have increasing ~decreasing! failure rate @IFR ~DFR!# if Ft~x!�OF~x � t !0 OF~t ! is decreasing ~increasing! in t+ If F is absolutely continuous

with density f, then F is in the IFR ~DFR! class if rF~t !� f ~t !0 OF~t ! is increas-ing ~decreasing! in t+

3+ F is said to have increasing ~decreasing! failure rate average @IFRA ~DFRA!#if *0

t rF ~x! dx0t is increasing ~decreasing!+4+ F is said to have new better ~worse! than used @NBU ~NWU!# if OFt~x!� ~�!OF~x! for x � 0 and t � 0+

5+ F is said to have decreasing ~increasing!mean residual life @DMRL ~IMRL!#if the mean residual life µF~t !� *t

` OF~x! dx0 OF~t ! is decreasing ~increasing!assuming that the mean µF~0! exists+

6+ F is said to have new better ~worse! than used in expectation @NBUE~NWUE!# if µF~t ! � ~�! µF~0! for all t � 0+

7+ F is said to have decreasing variance residual life ~increasing variance resid-ual life! @DVRL ~IVRL!# if sF

2~t ! is decreasing ~increasing!+

The chain of implications among these classes of distributions is

PF2 n IFR n IFRA n NBU

⇓ ⇓

DMRL n NBUE+

DVRL

The reverse implications are not true; for counterexamples, see Bryson andSiddiqui @11# + Some extensions of these classes of distributions are containedin Klefsjo @26,27# , Shaked @32# , Singh and Deshpande @35# , Deshpande, Kochar,and Singh @12#, Basu and Ebrahimi @5,6#,Abouammoh @1#,Abouammoh and Ahmad@2# , and Loh @30# +

318 R. C. Gupta

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2.2. Stochastic Order Relations

Let X and Y be nonnegative absolutely continuous random variables with densityfunctions f ~x! and g~x! and survival functions OF~x! and OG~x!, respectively+ Then,we have the following:

1+ X is said to be smaller than Y in the likelihood ratio ordering, written asX �LR Y, if f ~x!0g~x! is nonincreasing in x+

2+ X is said to be smaller than Y in the failure ~hazard! rate ordering, written asX �FR Y, if rF~x! � rG~x! for all x+

3+ X is said to be smaller than Y in the stochastic ordering, written as X �st Y,if OF~x! � OG~x! for all x+

4+ X is said to be smaller than Y in the mean residual life ordering, written asX �MRL Y, if µF~x! � µG~x! for all x+ Deshpande, Singh, Bagai, and Jain@13# show that X �MRL Y if and only if *x

` OF~u! du0*x` OG~u! du is decreas-

ing in x+5+ X is said to be smaller than Y in the increasing convex order, written as

X �icx Y, if *x` OF~u! du � *x

` OG~u! du for all x+ Note that in the literature theincreasing convex order has also been called stop loss ordering ~Hesselager@22# ! and ST2 ordering; see Belzunce, Candel, and Ruiz @7# and Shaked andShanthikumar @33# + For some generalized variability ordering, see Zarek@39# , Li and Zhu @29# , and Bhattacharjee and Sethuraman @8# +

6+ X is said to be smaller than Y in the variance residual life ordering, writtenas X �VRL Y, if sF

2~x! � sG2~x! for all x+

7+ X is said to be smaller than Y in the Laplace transform ordering, written asX �LT Y, if E~e�sX!� E~e�sY!+ Shaked and Shanthikumar @33# showed thatthis is equivalent to *0

` e�sx OF~x! dx � *0` e�sx OG~x! dx+

8+ X is said to be smaller than Y in the moment generating function ordering,written as X �MGF Y, if E~esX! � E~esY!+

It is well known that

X �LR Yn X �FR Yn X �MRL Y n X �VRL Y

⇓ ⇓

X �st Y X �icx Y;

see Shaked and Shanthikumar @33# +

3. HIGHER-ORDER EQUILIBRIUM DISTRIBUTIONS AND STOPLOSS MOMENTS

We define the sequence of induced distributions as follows+ Let OF~x! be the sur-vival function of a nonnegative random variable X with MRLF given by µF~t !+Wenow define a sequence $ OF1, OF2, + + +% of survival functions induced by OF as

EQUILIBRIUM DISTRIBUTION IN RELIABILITY 319

Page 7: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

Fn~t ! �

�t

`

OFn�1~u! du

µn�1

, (3.1)

where µn is the mean of the distribution Fn+ Assume that E~Xn!� ` for the largestn used above so that µ1, µ2, + + + , µn will all be finite+ In what follows, we will denoteby X @0# � X, corresponding to the survival function OF0 � OF, the original randomvariable and X @1#, X @2#, + + + corresponding to OF1, OF2, + + + +

We now present the following result+

Theorem 3.1: Let f be a convex function. Then

EF @f~X � t !6X � t #� f~0!� EF @~X � t !6X � t #EF1@f '~X � t !6X � t # + (3.2)

Proof:

EF @f~X � t !6X � t #

��t

`

f~x � t ! d OF~x!

OF~t !

� f~0!��

t

`

f '~x � t ! OF~x! dx

OF~t !

� f~0!��t

`

f '~x � t ! �OF~x!0µ

�t

`

~ OF~x!0µ! dx ��

t

`

OF~x! dx

OF~t !dx

� f~0!� EF @~X � t !6X � t #�t

`

f '~x � t !f1~x!

F1~x!dx,

where f1~x!� OF~x!0µ is the p+d+f+ of the first induced distribution and F1~x! is itssurvival function+ Thus,

EF @f~X � t !6X � t #� f~0!� EF @~X � t !6X � t #EF1@f '~X � t !6X � t # + �

Particular Cases:

EF @~X � t !2 6X � t #� 2µF ~t !µF1~t ! (3.3)

and, in general,

EF @~X � t !k 6X � t #� k!)j�0

k�1

µj ~t !, (3.4)

320 R. C. Gupta

Page 8: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

where µ0~t !� µ~t !� MRLF of F and µj~t ! is the MRLF of the j th induced distri-bution; see also Stein and Dattero @36# + From this, it is clear that

EF ~Xk 6X � t !� k!)

j�0

k�1

µj , (3.5)

where µj is the mean of the j th induced distribution+

3.1. Stop Loss Transform

Definition 3.1: The function pX~t ! � E @~X � t !�# is called the stop loss trans-form of X, where ~X � t !� � Max~X � t,0! represents the amount by which Xexceeds the threshold t.

The kth stop loss moment is given by

Rk~t ! � E @~X � t !�k #��

t

`

~x � t !k dF~x!; (3.6)

see Willmot, Drekic, and Cai @38# and Hesselager, Wang, and Willmot @23# + Notethat Rk~t ! has also been called the kth partial moment in the literature; see Guptaand Gupta @15# +We now present the following result+

Theorem 3.2: The survival function of the kth equilibrium distribution is given by

OFk~t ! � E @~X � t !�k #0E~X k !+ (3.7)

Proof:

E @~X � t !�k #0E~X k !

��t

`

~x � t !k dF~x!0E~X k !

��t

`

k~x � t !k�1 OF~x! dx0E~X k !

� kµ�t

`

~x � t !k�1 f1~x! dx0E~X k !

�kµ

E~X k !�

t

`

~k � 1!~x � t !k�2 OF1~x! dx

�k~k � 1!µµ1

E~X k !�

t

`

~x � t !k�2 f2~x! dx+

EQUILIBRIUM DISTRIBUTION IN RELIABILITY 321

Page 9: ROLE OF EQUILIBRIUM DISTRIBUTION IN RELIABILITY STUDIES

Proceeding in this way, we get

E @~X � t !�k #0E~X k ! �

k!Pj�0k�1 µj

E~X k !OFk~t !

� OFk~t !+ �

We now show that Rk~t ! determines the distribution function uniquely+

Theorem 3.3: Under the above-stated conditions,

OF~t ! �~�1!k

k!Rk~k!~t !, (3.8)

where Rk~k!~t ! denotes the kth derivative of Rk~t ! .

Proof: Applying Taylor’s theorem to F~x!, we get

F~x! � 1 �~�1!k

k!�

t

`

~x � t !kF ~k! ~x! dF~x!

� 1 �~�1!k

k!� d

dt�k�

0

`

uk f ~t � u! du

� 1 �~�1!k

k!� d

dt�k�

t

`

~x � t !k dF~x!

� 1 �~�1!k

k!Rk~k!~t !+ (3.9)

This gives the desired result+ �

Remark 3.1: For other proofs, see Gupta and Gupta @15# and Navarro, Franco, andRuiz @31# +

4. AGING PROPERTIES OF EQUILIBRIUM DISTRIBUTIONS ANDSOME ORDER RELATIONS

It is well known that the failure rate of F1 is the reciprocal of the MRLF of F and,in general, the failure rate of Fi ~i � 1,2, + + +! is the reciprocal of the MRLF of Fi�1

~i � 1,2, + + +!+ This means that Fi is IFR is equivalent to Fi�1 is DMRL+ In the fol-lowing, we show that Fi�1 is DMRL is equivalent to Fi�2 is DVRL+

Theorem 4.1: Fi�1 is DMRL is equivalent to Fi�2 is DVRL ~i � 2,3, + + +! .

Proof: It is enough to prove the result for i � 2+ We have

E~~X � t !2 6X � t !

E~~X � t !6X � t !� 2µF1

~t !+ (4.1)

322 R. C. Gupta

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Also,

µF1~t ! �

sF2~t !� µF

2 ~t !

µF ~t !

�1

2µF ~t !~gF

2~t !� 1!+

This gives

d

dt@E~~X � t !2 6X � t !#0E~X � t 6X � t !

� 2µF1

' ~t !

� 2~rF1~t !µF1

~t !� 1!

� 2�µF1~t !

µF ~t !� 1�

� 2� 1

2~gF

2~t !� 1 � 1!� gF

2~t !� 1+

This proves the result; see also Gupta et al+ @19# , Singh @34# , Fagiuoli and Pellerey@14# , and Willmot @37# + �

Corollary 4.1: Suppose F is a strictly increasing life distribution. Then F is DVRL(IVRL) if and only if the induced distribution corresponding to F is DMRL.

Remark 4.1: The restriction to strictly increasing F in Theorem 4+1 and Corollary4+1 cannot be relaxed+ This can be seen from Example 1 of Gupta et al+ @19# , whereF is IVRL but the function E~~X � t !2 6X � t !0E~~X � t !6X � t ! is not increasingin the neighborhood of t � 1

2_ +

Remark 4.2: It is also clear from the above derivation that

µF1~t !

µF ~t !�

1

2~1 � gF

2~t !!+

From the above, we can state the following+

Theorem 4.2: Suppose F is a strictly increasing life distribution. Then F is DVRL(IVRL) if and only if µF1

~t ! � ~�! µF~t ! .

Remark 4.3: The above result was also noticed by Deshpande et al+ @13# and Abou-ammoh, Kanjo, and Khalique @3# +

EQUILIBRIUM DISTRIBUTION IN RELIABILITY 323

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It is also clear from the above that µF1~t !� µF~t ! if and only if F has an expo-

nential distribution+The following theorem addresses the stochastic comparisons of X @1# and X+

Theorem 4.3: Suppose X is a nonnegative random variable with E~X !�`. ThenX is NBUE (NWUE) if X @1# �st ~�st ! X.

Proof: The survival function of X @1# is given by

OFX @1# ~t ! ��t

`

OF~x! dx0µ

� OFX ~t ! OFX ~t !0µ+

This gives

OFX @1# ~t !

OFX ~t !�

µF ~t !

µ+

Thus,

OFX @1# ~t ! � OFX ~t ! if and only if X is NBUE+

Similarly, OFX @1# ~t ! � OFX~t ! if and only if X is NWUE+ �

We now present the following result dealing with the hazard rate comparisonof X @1# and X+

Theorem 4.4: Suppose X is a nonnegative random variable with E~X !�`. ThenX is IMRL (DMRL) if and only if X �FR ~�FR! X @1#.

Proof:

X � X @1# m OFX @1# ~t !0 OFX ~t ! is increasing

mOFX @1# ~v!

OFX ~v!�OFX @1# ~u!

OFX ~u!if u � v

m OFX @1# ~v! OFX ~u!� OFX @1# ~u! OFX ~v!

m �v

` OF~t !

µdt OFX ~u!� �

u

` OF~t !

µdt OFX ~v!

m

�v

`

OF~t ! dt

OFX ~v!�

�u

`

OF~t ! dt

OFX ~u!

m µX ~v!� µX ~u!

m X is IMRL+ �

324 R. C. Gupta

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The following result deals with the Laplace ordering of two random variablesand their corresponding equilibrium distributions+

Theorem 4.5: Let X and Y be two nonnegative random variables with E~X ! �E~Y ! . Then

X �LT Ym X @1# �LT Y @1#+

Proof: We have

LX @1# ~t ! � t�0

`

e�tx��0

x OFX ~ y!

µdy� dx

�t

E~X !�

0

`��y

`

e�tx dx� OFX ~ y! dy

�1

E~X !�

0

`

e�ty OFX ~ y! dy+

Now

X �LT Ym �0

`

e�tx OFX ~x! dx � �0

`

e�ty OFY ~ y! dy

m LX @1# ~t !� LY @1# ~t ! since E~X !� E~Y !+ �

The following two results deal with the stop loss ordering of two random vari-ables and their corresponding equilibrium variables+

Theorem 4.6: Let X and Y be two nonnegative random variables with E~X ! �E~Y ! . Then

X �SL Ym X @1# �st Y @1#+

Proof:

X @1# �st Y @1# mpX ~t !

E~X !�pY ~t !

E~Y !for all t � 0

m pX ~t !� pY ~t ! since E~X !� E~Y !

m X �SL Y+ �

EQUILIBRIUM DISTRIBUTION IN RELIABILITY 325

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Theorem 4.7: Let X and Y be two nonnegative random variables with finite means.Then

X �HR Ym X @1# �LR Y @1#+

Proof:

X @1# �LR Y @1#

mfX @1% ~t !

fY @1% ~t !is decreasing

mfX @1% ~u!

fY @1% ~u!�

fX @1% ~v!

fY @1% ~v!if u � v

mOFX ~u!

OFY ~u!�OFX ~v!

OFY ~v!

mOFX ~t !

OFY ~t !is decreasing

m X �HR Y+ �

We now define the convex ordering as follows+

Definition 4.1: X �icx Y if E~ f ~X !! � E~ f ~Y !! for all increasing convex func-tions. This is equivalent to

X �icx Y if OFX ~t ! � OFY ~t ! for all t � 0.

Following the above concept, we define a similar ordering between the sthequilibrium as follows+

Definition 4.2: X �s�icx Y if OFX~s!~t ! � OFY

~s!~t ! for all t � 0, where OFX~s!~t ! and

OFY~s!~t ! are the survival functions of their sth equilibrium distributions; see Klar

and Muller [25].

Comparing the original variable and its equilibrium variable in the above order-ing, we have

X �s�icx X @s# for s � 1 if E~X � t !�s�1 � E~X @s# � t !�

s�1 +

This is equivalent to

E~X � t !�s

E~X � t !�s�1

� µs+

326 R. C. Gupta

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Denoting

Mn~t ! �E~X � t !�

n

nE~X � t !�n�1,

the above inequality can be written as

Ms~t ! � µ;

see Stein and Dattero @36# +

5. EQUILIBRIUM DISTRIBUTION OF A SERIES SYSTEM

Let X1, X2, + + + , Xn be independent random variables with survival functions OFX1,

OFX2, + + + , OFXn

, respectively+ When the components are arranged in a series system,we observe X1 ∧ X2 ∧ {{{ ∧ Xn � Min~X1, X2, + + + , Xn!+ In this section, we will com-pare two systems whose components are the nth equilibrium distributions of X andY and the nth equilibrium distribution of a system having components X and Y+More precisely, we have the following result due to Bon and Illayk @9# +

Theorem 5.1: Let X and Y be independent nonnegative random variables. LetX @k# and Y @k# be respectively the independent equilibrium variables of X and Y oforder k. If X and Y have the DMRL property and if the nth moments of X and Y exist,then

X @n# ∧ Y @n# �LR ~X ∧ y!@n#,

where ~X ∧ y!@n# is the equilibrium variable of X ∧ Y of order n.

Proof: For n � 1, X @1# and Y @1# are independent and the p+d+f+ of X @1# ∧ Y @1# isgiven by

fX @1#∧Y @1# ~t ! � fX @1# ~t ! OFY @1# ~t !� fY @1# ~t ! OFX @1# ~t !+

Also, the p+d+f+ of ~X ∧ Y !@1# is

f~X∧Y !@1# ~t ! �OFX ~t ! OFY ~t !

E~X ∧ Y !+

These give

fX @1#∧Y @1# ~t !

f~X∧Y !@1# ~t !�

E~X ∧ Y !@µX ~t !� µY ~t !#

E~X !E~Y !+

Since X and Y have the DMRL property, the right-hand side of the above equa-tion is decreasing and, hence, X @1# ∧ Y @1# �LR ~X ∧ Y !@1#+

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For the general case, we proceed by induction and assume that the result is trueof k � n+ It can be verified that

fX @n#∧Y @n# ~t !

f~X∧Y !@n# ~t !

� E~X ∧ Y !@n�1#� OFX @n�1# ~t ! OFY @n# ~t !

E~X @n�1# ! OF~X∧Y !@n�1# ~t !�

OFY @n�1# ~t ! OFX @n# ~t !

E~Y @n�1# ! OF~X∧Y !@n�1# ~t ! ,� A~t !� B~t !,

where

A~t ! �OFX @n�1# ~t ! OFY @n# ~t !

E~X @n�1# ! OF~X∧Y !@n�1# ~t !,

and likewise for B~t !+ We now show that A~t ! and B~t ! are decreasing functionsof t+

Since Y has the DMRL property, all of its equilibrium variables have the IFRproperty and also the DMRL property+ This means that Y @n# �HR Y @n�1#+ Thus,

X @n�1# ∧ Y @n# �HR X @n�1# ∧ Y @n�1#+

Also, the induction hypothesis implies that

X @n�1# ∧ Y @n�1# �HR ~X ∧ Y !@n�1#+

Therefore, X @n�1# ∧ Y @n# �HR ~X ∧ Y !@n�1#+ This implies that A~t ! is decreasing+Similary, B~t ! is decreasing and the proof is complete+ �

Remark 5.1: For the lower bound on the nth moment of a series system, see theabove remark+

6. BIVARIATE EQUILIBRIUM DISTRIBUTION

In order to define bivariate equilibrium distribution, we first review the bivariatehazard rates and bivariate MRLF as follows+ Let ~X1, X2! be a nonnegative bivar-iate random variable with survival function OF~x1, x2!+The hazard components of~X1, X2! are given by h1~x1, x2! and h2~x1, x2!, where

hi ~x1, x2 ! �]

]xi

@�ln OF~x1, x2 !# , i � 1,2,

328 R. C. Gupta

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and the MRLF of ~X1, X2! is given by ~µ1~x1, x2!, µ2~x1, x2!!, where

µ1~x1, x2 ! � E~X1 � x16X1 � x1, X2 � x2 !

�1

OF~x1, x2 !�

x1

`

OF~x1, x2 ! dx1,

and likewise for µ2~x1, x2!+ The hazard components and the MRLF components arerelated by

hi ~x1, x2 ! �

1 �]

]xi

µi ~x1, x2 !

µi ~x1, x2 !, i � 1,2+

Keeping these properties in mind, Gupta and Sankaran @21# defined the bivar-iate equilibrium random variable ~Y1,Y2! by means of the conditional distributionas follows+

The p+d+f+ of Y1 given Y2 � y2 is

g~ y16Y2 � y2 !�P~X1 � y16X2 � y2 !

E~X16X2 � y2 !+ (6.1)

Likewise, the p+d+f+ of Y2 given Y1 � y1 is

g~ y2 6Y1 � y1!�P~X2 � y2 6X1 � y1!

E~X2 6X1 � y1!+ (6.2)

It can be easily seen that the marginal distributions of Y1 and Y2 coincide with theequilibrium distributions of X1 and X2, respectively+ Following the above scheme,one can easily define equilibrium distributions in higher dimensions+

We now present two examples+

Example 6.1: Gumbel’s bivariate exponential distribution with survival function

OF~x1, x2 ! � exp~�ax1 � bx2 � cx1 x2 !, x1, x2 � 0,a,b, c � 0+

It is well known that for this distribution, the conditional distribution of X1

given X2 � x2 and the conditional distribution of X2 given X1 � x1 are exponential+Also, the marginal distributions of X1 and X2 are exponentials+ However, the con-ditional distribution of X1 given X2 � x2 and that of X2 given X1 � x1 are not expo-nential+ For other properties of this model, see Arnold @4# +

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It can be easily verified that in this case

g~ y16Y2 � y2 !� ~a � cy2 !e�ay1�cy1 y2, y1 � 0, y2 � 0+

This shows that the distribution of Y1 given Y2 � y2 is exponential with parametera � cy2+ Similarly, the distribution of Y2 given Y1 � y1 is exponential with param-eter b � cy1+

We will now obtain the equilibrium distributions in the case of series and par-allel systems+

Series System: In this case, we observe T1 � Min~X1, X2! and the survivalfunction is given by

OF~t ! � exp~�at � bt � ct 2 !, t � 0,

and

E~T1! �1

2c�102e ~~a�b!204c!G�1

2,~a � b!2

4c�,

where

G~m, x! ��x

`

t m�1e�t dt;

see Gupta, Tajdari, and Bresinsky @20# + The above two expressions yield thep+d+f+ of the equilibrium distribution in the case of a series system+

Parallel System: In this case, we observe T2 � Max~X1, X2! and the survivalfunction is given by

OF~t ! � e�at � e�bt � e�at�bt�ct 2

, t � 0,

and

E~T2 ! �a � b

ab� E~T1!+

The above two expressions yield the equilibrium distribution in the case of aparallel system+

Example 6.2: Generalized bivariate Pareto distribution with survival function

OF~x1, x2 ! �1

@1 � a~x1 � x2 !� a2bx1 x2 #c,

x1, x2 � 0, a, c � 0, 0 � b � 1 � c+

330 R. C. Gupta

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The above survival function was obtained as a mixture of independent exponentialrandom variables; see Hutchinson and Lee @24, p+ 118# +

It can be verified that, in this case,

g~ y16Y2 � y2 ! �OF~ y1, y2 !

P~X2 � y2 !E~X16X2 � y2 !

� � 1 � ay2

1 � a~ y1 � y2 !� a2by1 y2c 1

E~X16X2 � y2 !,

where

E~X16X2 � y2 ! ��0

`� 1 � ay2

1 � a~ y1 � y2 !� a2by1 y2c

dy1

� ~c � 1!~a � a2by2 !~1 � ay2 !

c�1

@1 � a~ y1 � y2 !� a2by1 y2 #c+

We will now obtain the equilibrium distributions in the case of series and par-ralel systems+

Series System: In this case, we observe T1 � Min~X1, X2! and the survivalfunction is given by

OF~t ! �1

~1 � 2at � a2bt 2 !c, t � 0,

and

E~T1! �2c�102

aMb�1

b� 1�~1�2c!04

G�c �1

2�b~2c � 1,1!Pc�302102�c� 1

Mb�,

c �1

2,

where

Pnµ~z! �

1

G~1 � µ!� z � 1

z � 1�µ02

2 F1��n,n� 1,1 � µ,1 � z

2�

is the associated Legendre function of the first kind; see Gupta et al+ @20# +The above two expressions yield the p+d+f+ of the equilibrium distribution in

the case of a series system+

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Parallel System: In this case, we observe T2 � Max~X1, X2! with survivalfunction

OF~t ! �2

~1 � ab!c�

1

~1 � 2at � a2bt 2 !c

and

E~T2 ! �2

a~c � 1!� E~T1!+

The above two expressions yield the distribution of the equilibrium distribu-tion in the case of a parallel system+

7. SOME CONCLUSIONS AND COMMENTS

In this article we have presented the equilibrium distribution including its higherderivates from a reliability point of view+ Since the equilibrium distribution is inti-mately connected with the original distribution, it provides a useful tool in studyingseveral important properties of the original distribution+ Aging properties of equi-librium distributions and their stochastic orderings with the original distributionsare explored+ The relation between the equilibrium distribution of a series systemand a series system of equilibrium distributions, consisting of two components, isinvestigated+ Extension to bivariate equilibrium distributions is provided along withsome examples+ It is hoped that this article will be useful to theoreticians and prac-titioners in studying the applications of equilibrium distribution in reliability+

AcknowledgmentThe author is thankful to the Editor Sheldon Ross for some useful comments that enhanced thepresentation+

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