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Research Inventy: International Journal Of Engineering And Science
Issn: 2278-4721, Vol.2, Issue 6 (March 2013), Pp 11-14
Www.Researchinventy.Com
11
A Study Of Convolution Closure Of Idmrl Class Of Life
Distribution
Fuxiang Liu
Science College and Institute of Intelligent Vision and Image Information, China Three Gorges
University, Yichang, Hubei, 443002, P.R. China
Abstract: This paper, based on the relation between the survival function and the mean residual
life(MRL)function, obtains the sufficient condition of the convolution closure of IDMRL class of life distribution
and some relevant counterexamples, and then significantly presents the discovery of the SMC (scalar
multiplication closure) of IDMRL class of life distribution, and consequently, in the final part, the Poisson shock
model is transformed into a mixture model, as serves more effectively in the analysis of survival and reliability.
Keywords: MRL; convolution closure; SMC; Poisson shock model; mixture
I. Introduction
IDMRL class of life distribution has received continous and increasing attention in the recent years.
Anis(2012) investigates the weak convergence of IDMRL distribution; and Anis(2010, 2012), Mitra and
Basu(1996), Mitra and Pandey(2011), etc. discuss the relation between IDMRL class of life distributions and
Poisson shock model. Chen(2000) studies the new two-parameter lifetime distribution with IDMRL properties.
Bebbington, Lai and Zitikis(2007) discover a two parameter flexible Weibull distribution which performs with
very complicated monotonicity of failure rate and MRL functions. Besides, Anis(2012) explores the closure of
IDMRL class of life distribution based on mixture model and parallel system. The closure of convolution
transformation which has been probed into inadequately is of much importance in analysis of survival and
reliability. This paper focuses on the closures of convolution transformation of the IDMRL class of life
distribution on the basis of the relation between the failure rate and the MRL funcution and obtains some
relevant counterexampers, which leads to some important findings.
II. Convolution Closure Of IDMRL Class Of Distribution
Let X be a certain random variable of life distribution with its corresponding common absolutely
continuous cumulative distribution function(cdf) )(tF , probability density function(pdf) )(tf , survival
function )(1)( tFtF  , failure rate function )(/)()( tFtftr  and mean residual life function






 

.0)(,0
,0)(),(/)(
]|[(
tF
tFtFduuF
tXtXEte t
F And, the definition of the IDMRL class of life
distribution is presented as follows:
Denition 2.1 A distribution F is called an Increasing then Decreasing Mean Residual
A Study Of Convolution Closure Of IDMRL…
12
Life(IDMRL) distribution if there exists a change point  such that
)()( tese FF  for ,0  ts
)()( tese FF  for  ts .
Theorem 2.1. Assume that kiXi ,...,1,  be some certain i.i.d. random variables of con-
tinuous life distribution with expectation )( iXE . Let .1

k
i iXY If the failure rates
of kiXi ,...,1,  and Y perform a bathtub shape, 1)0(  f and 1)0(  Yfk , then the
distributions of kiXi ,...,1,  and Y are within the con ne of IDMRL class of life distribution.
Proof: Notice that
,1)0()0(]0|0[)0()0(  ffXXEre iiXX ii
 and
,1)0()0(]0|0[)0()0(  YYYY fkfYYEre  by the statement of Gupta and
Lvin(2005), the above results can be easily obtained.
A significant result similar to the theorem above can be inferred as follows:
Theorem 2.2. Assume that X is a certain random variable of continuous life distribution with
expectation )(XE . k is a positive integer. If 1)0(  f and the failure rate of X is in a bathtub
shape, then both X and Xk  are within the confine of IDMRL class of life distribution.
Proof: Obviously,
  .1)0()()0(]0|0[)0()0( 0
1
 
ffkfkXkXEre tk
t
kkXkXkX 
Meanwhile, )()( 1
k
t
XkkX rtr  .
This means that the failure rate functions rX(t) and rkX(t) perform the same bathtub shape.
So, both X and Xk  are within the confine of IDMRL class of life distribution.
But in the general case, the closure of IDMRL class does not exist. Then, a type of counterexamples are
demonstrated as follows:
Counterexample: Take an example of Poisson shock
model 





 
 
0
!
)(
)( k
t
k
Pe
k
t
tH 
: 10 P 4/11 P , 20/132  PP , 4,0  kPk 4(Belzunce,
Ortega and Ruiz, 2007).
Obviously, the corresponding distribution is within the confine of IDMRL class of life distribution with the
change point .2
Assume that ,2,1),(~ iHX ii  .9.0,3.0 21   Let ,21 XXY  the density function of Y is
tttt
Y teteeetf 9.03.09.03.0
0175.00240.03506.03506.0)( 

A Study Of Convolution Closure Of IDMRL…
13
.0018.00001.00072.00010.0 9.033.039.023.02 tttt
etetetet 

The corresponding survival function
tttt
Y teteeetF 9.03.09.03.0
0128.00848.04037.04512.1)( 

.0020.00004.00145.00007.0 9.033.039.023.02 tttt
etetetet 

The associated mean residual life function
tttt
Y teteeete 9.03.09.03.0
0661.03895.05220.01359.6[)( 

).(/]0022.00014.00233.00160.0 9.033.039.023.02
tFetetetet Y
tttt 

It is obvious that the distribution of random variable Y is not within the confine of IDMRL
class of life distribution. The comparison of the mean residual life function of YXX ,, 21 are
demonstrated in the following Figure 1(I, II, III):
Figure 1: The plots of MRL of .,, 21 YXX
Indeed, there are a large number of  values which fulfill this condition.
In fact, Poisson shock model can be viewed as a mixture. Notice that
 )()( tH
dt
d
th   ,
!
1
0
1




  kk
t
k
kk
PPe
k
t 
Denote ,
!
)(
1
t
kk
k e
k
t
tf  

 .1 kkk PPp
Then 0kp , 10


k kp and )(th ).(0
tfp kk k


Meanwhile, many achievements have been made in the study of the mixture model which can be employed for
further research on IDMRL class of life distribution.
III. Discussion
There is no doubt that the failure rate and the mean residual life of random variables, especially for
IDMRL class of life distribution, become more complicated in the condition of convolution transformation. At
present, the function structures employed for the study IDMRL class mainly include mixture model, piecewise
function, flexible Weibull distribution(Bebbington, Lai and Zitikis, 2007), and a new two-parameter lifetime
distribution(developed by Chen(2000)), etc. However, these function structures usually mean mechanical and
ineffective calculation, which suggests the necessity of exploration of a simpler and more effective model.
A Study Of Convolution Closure Of IDMRL…
14
References
[1] Anis, M.Z., 2010. Poisson shock model leading to IDMRL class of life distributions. Technical Report No: SQCOR-2010-01. Indian
Statistical Institute, Calcutta, March 2010.
[2] Anis, M.Z., 2012. On some properties of the IDMRL class of life distributions. Journal of Statistical Planning and Inference. 142,
3047-3055.
[3] Bebbington M., Lai C.D., Zitikis R., 2007. A flexible Weibull extension. Reliability Engineering and System Safety. 92(6), 719-726.
[4] Bekker, L. ,Mi, J., 2003. Shape and crossing properties of mean residual life functions. Statistics and Probability Letters. 64:
225-234.
[5] Belzunce, F., Ortega, E. M., Ruiz, J. M., 2007. On non-monotonic aging properties from Laplace transform with actuarial
applications. Insurance Mathematics and Economics. 40,1-14.
[6] Chen Zhenmin, 2000. A new two-parameter lifetime distribution with bathtub shaped or increasing failure rate function. Statistics
and Probability Letters. 49: 155-161.
[7] Gupta, R.C., Lvin, S., 2005. Monotonicity of failure rate and mean residual life function of a gamma-type model. Applied
Mathematics and Computation. 165, 623-633.
[8] Mitra, M., Basu, S.K., 1996. Shock models leading to non-monotonic ageing classes of life distributions. Journal of Statistical
Planning and Inference. 55, 131-138.
[9] Mitra, M., Pandey, A., 2011. Poisson shock models leading to new classes of non-monotonic aging life distributions.
Microelectronics Reliability. 51, 2412-2415.
[10] Tang, L.C., Lu, Y., Chew, E.P., 1999. Mean residual life of lifetime distributions. IEEE Transaction Reliability. 48(1): 73-78.

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  • 1. Research Inventy: International Journal Of Engineering And Science Issn: 2278-4721, Vol.2, Issue 6 (March 2013), Pp 11-14 Www.Researchinventy.Com 11 A Study Of Convolution Closure Of Idmrl Class Of Life Distribution Fuxiang Liu Science College and Institute of Intelligent Vision and Image Information, China Three Gorges University, Yichang, Hubei, 443002, P.R. China Abstract: This paper, based on the relation between the survival function and the mean residual life(MRL)function, obtains the sufficient condition of the convolution closure of IDMRL class of life distribution and some relevant counterexamples, and then significantly presents the discovery of the SMC (scalar multiplication closure) of IDMRL class of life distribution, and consequently, in the final part, the Poisson shock model is transformed into a mixture model, as serves more effectively in the analysis of survival and reliability. Keywords: MRL; convolution closure; SMC; Poisson shock model; mixture I. Introduction IDMRL class of life distribution has received continous and increasing attention in the recent years. Anis(2012) investigates the weak convergence of IDMRL distribution; and Anis(2010, 2012), Mitra and Basu(1996), Mitra and Pandey(2011), etc. discuss the relation between IDMRL class of life distributions and Poisson shock model. Chen(2000) studies the new two-parameter lifetime distribution with IDMRL properties. Bebbington, Lai and Zitikis(2007) discover a two parameter flexible Weibull distribution which performs with very complicated monotonicity of failure rate and MRL functions. Besides, Anis(2012) explores the closure of IDMRL class of life distribution based on mixture model and parallel system. The closure of convolution transformation which has been probed into inadequately is of much importance in analysis of survival and reliability. This paper focuses on the closures of convolution transformation of the IDMRL class of life distribution on the basis of the relation between the failure rate and the MRL funcution and obtains some relevant counterexampers, which leads to some important findings. II. Convolution Closure Of IDMRL Class Of Distribution Let X be a certain random variable of life distribution with its corresponding common absolutely continuous cumulative distribution function(cdf) )(tF , probability density function(pdf) )(tf , survival function )(1)( tFtF  , failure rate function )(/)()( tFtftr  and mean residual life function          .0)(,0 ,0)(),(/)( ]|[( tF tFtFduuF tXtXEte t F And, the definition of the IDMRL class of life distribution is presented as follows: Denition 2.1 A distribution F is called an Increasing then Decreasing Mean Residual
  • 2. A Study Of Convolution Closure Of IDMRL… 12 Life(IDMRL) distribution if there exists a change point  such that )()( tese FF  for ,0  ts )()( tese FF  for  ts . Theorem 2.1. Assume that kiXi ,...,1,  be some certain i.i.d. random variables of con- tinuous life distribution with expectation )( iXE . Let .1  k i iXY If the failure rates of kiXi ,...,1,  and Y perform a bathtub shape, 1)0(  f and 1)0(  Yfk , then the distributions of kiXi ,...,1,  and Y are within the con ne of IDMRL class of life distribution. Proof: Notice that ,1)0()0(]0|0[)0()0(  ffXXEre iiXX ii  and ,1)0()0(]0|0[)0()0(  YYYY fkfYYEre  by the statement of Gupta and Lvin(2005), the above results can be easily obtained. A significant result similar to the theorem above can be inferred as follows: Theorem 2.2. Assume that X is a certain random variable of continuous life distribution with expectation )(XE . k is a positive integer. If 1)0(  f and the failure rate of X is in a bathtub shape, then both X and Xk  are within the confine of IDMRL class of life distribution. Proof: Obviously,   .1)0()()0(]0|0[)0()0( 0 1   ffkfkXkXEre tk t kkXkXkX  Meanwhile, )()( 1 k t XkkX rtr  . This means that the failure rate functions rX(t) and rkX(t) perform the same bathtub shape. So, both X and Xk  are within the confine of IDMRL class of life distribution. But in the general case, the closure of IDMRL class does not exist. Then, a type of counterexamples are demonstrated as follows: Counterexample: Take an example of Poisson shock model           0 ! )( )( k t k Pe k t tH  : 10 P 4/11 P , 20/132  PP , 4,0  kPk 4(Belzunce, Ortega and Ruiz, 2007). Obviously, the corresponding distribution is within the confine of IDMRL class of life distribution with the change point .2 Assume that ,2,1),(~ iHX ii  .9.0,3.0 21   Let ,21 XXY  the density function of Y is tttt Y teteeetf 9.03.09.03.0 0175.00240.03506.03506.0)(  
  • 3. A Study Of Convolution Closure Of IDMRL… 13 .0018.00001.00072.00010.0 9.033.039.023.02 tttt etetetet   The corresponding survival function tttt Y teteeetF 9.03.09.03.0 0128.00848.04037.04512.1)(   .0020.00004.00145.00007.0 9.033.039.023.02 tttt etetetet   The associated mean residual life function tttt Y teteeete 9.03.09.03.0 0661.03895.05220.01359.6[)(   ).(/]0022.00014.00233.00160.0 9.033.039.023.02 tFetetetet Y tttt   It is obvious that the distribution of random variable Y is not within the confine of IDMRL class of life distribution. The comparison of the mean residual life function of YXX ,, 21 are demonstrated in the following Figure 1(I, II, III): Figure 1: The plots of MRL of .,, 21 YXX Indeed, there are a large number of  values which fulfill this condition. In fact, Poisson shock model can be viewed as a mixture. Notice that  )()( tH dt d th   , ! 1 0 1       kk t k kk PPe k t  Denote , ! )( 1 t kk k e k t tf     .1 kkk PPp Then 0kp , 10   k kp and )(th ).(0 tfp kk k   Meanwhile, many achievements have been made in the study of the mixture model which can be employed for further research on IDMRL class of life distribution. III. Discussion There is no doubt that the failure rate and the mean residual life of random variables, especially for IDMRL class of life distribution, become more complicated in the condition of convolution transformation. At present, the function structures employed for the study IDMRL class mainly include mixture model, piecewise function, flexible Weibull distribution(Bebbington, Lai and Zitikis, 2007), and a new two-parameter lifetime distribution(developed by Chen(2000)), etc. However, these function structures usually mean mechanical and ineffective calculation, which suggests the necessity of exploration of a simpler and more effective model.
  • 4. A Study Of Convolution Closure Of IDMRL… 14 References [1] Anis, M.Z., 2010. Poisson shock model leading to IDMRL class of life distributions. Technical Report No: SQCOR-2010-01. Indian Statistical Institute, Calcutta, March 2010. [2] Anis, M.Z., 2012. On some properties of the IDMRL class of life distributions. Journal of Statistical Planning and Inference. 142, 3047-3055. [3] Bebbington M., Lai C.D., Zitikis R., 2007. A flexible Weibull extension. Reliability Engineering and System Safety. 92(6), 719-726. [4] Bekker, L. ,Mi, J., 2003. Shape and crossing properties of mean residual life functions. Statistics and Probability Letters. 64: 225-234. [5] Belzunce, F., Ortega, E. M., Ruiz, J. M., 2007. On non-monotonic aging properties from Laplace transform with actuarial applications. Insurance Mathematics and Economics. 40,1-14. [6] Chen Zhenmin, 2000. A new two-parameter lifetime distribution with bathtub shaped or increasing failure rate function. Statistics and Probability Letters. 49: 155-161. [7] Gupta, R.C., Lvin, S., 2005. Monotonicity of failure rate and mean residual life function of a gamma-type model. Applied Mathematics and Computation. 165, 623-633. [8] Mitra, M., Basu, S.K., 1996. Shock models leading to non-monotonic ageing classes of life distributions. Journal of Statistical Planning and Inference. 55, 131-138. [9] Mitra, M., Pandey, A., 2011. Poisson shock models leading to new classes of non-monotonic aging life distributions. Microelectronics Reliability. 51, 2412-2415. [10] Tang, L.C., Lu, Y., Chew, E.P., 1999. Mean residual life of lifetime distributions. IEEE Transaction Reliability. 48(1): 73-78.