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International Refereed Journal of Engineering and Science (IRJES)
ISSN (Online) 2319-183X, (Print) 2319-1821
Volume 2, Issue 10 (October 2013), PP. 26-30

Tolerance Interval for Exponentiated Exponential
Distribution Based on Grouped Data
C. S. Kakade1, D. T. Shirke2
1

Principal, Anandibai Raorane Arts,Commerce and Science College, Vaibhavwadi, Sindhudurga. 416810,
India.
2
Head, Department of Statistics, Shivaji University, Kolhapur. 416004, India.

Abstract:- Upper -expectation and -content -level tolerance interval for exponentiated exponential
distribution based on grouped data are considered. The adequacy of proposed tolerance intervals are evaluated
using simulation study and through real life data due to Lawless (1982).
Keywords : Exponentiated Exponential Distribution, Upper  expectation and  content  level tolerance
interval, Maximum likelihood estimator, grouped data.

I.

INTRODUCTION

Gupta et al. (1998) introduced the Exponentiated Exponential Distribution (EE) as a generalization of
the standard exponential distribution. Gupta and Kundu (2001) Studied this distribution and observed that it can
be used quite effectively in analyzing many life time data particularly in place of two parameter gamma and
Weibull distributions. In their series of papers on EE distribution
( also named as Generalized exponential
distribution), they discussed different estimation procedures, testing of hypothesis, construction of confidence
interval, estimating the stress and strength parameter and closeness of generalized exponential with Weibull,
gamma and lognormal distribution. Shirke et al. (2005) obtained -expectation and -content -level tolerance
interval for this distribution based on ungrouped data. Many times in a life testing problem, it is not possible to
record exact time of failure of a components due to several reasons. Hence it is more economical to observe no
of failures of components in predefined time intervals which form grouped data. The main aim of this paper is to
construct  expectation and  content  level tolerance interval for EE distribution based on grouped data.
Let U be a statistic based on data observed from a distribution with density function f(x, θ ) where θ
represents a vector of unknown parameters then the interval (-, U) is a -expectation tolerance interval (TI) if

U

E   f ( x, θ)dx   β





for every

θ 

(1.1)

and interval (-, U) is upper  content  level TI if

U

P   f ( x, θ)dx  β  γ





for given ,  є (0,1).

(1.2)

U

C is called the coverage of TI (-, U) if

C

 f (x, θ)dx .



One sided TI’s when f(x,) is a two parameter EE distribution based on maximum likelihood
estimators for ungrouped data were discussed by Shirke et al. (2005). This paper extends the procedure for
setting TI based on grouped data. In section 2 we provide upper -expectation TI along with its approximate
expected coverage. -content -level TI based on MLE’s of  are discussed in section 3. We study the
performance of both these TI using simulation technique in section 4. In section 5 we illustrate the practical
applications of the procedure by applying it to real life data set.

II.

-EXPECTATION TOLERANCE INTERVAL

Gupta and Kundu (2001) defined EE distribution in the following way. Let Y be a two parameter EE
random variable with distribution function

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Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data

F( y, λ, α)  (1  e λy ) α

,,y>0,
Therefore corresponding probability density function is given by

f ( y, λ, α)  αλ(1  e λy ) α1 e λy .

(2.1)

,y>0

(2.2)

Suppose Xj , j=1,2,….,k be the number of observations in the interval (t j-1, tj] with t0=0 and tk= such that
k

 xi  n . Thus we have grouped data from the underlying distribution .
i 1

The log likelihood function for the grouped data can be written as
k

L(λ, α / x )  C   x i ln F( t i )  F( t i 1) , where c is independent of  and  and F(.) is defined in (2.1).
i 1

Therefore to obtain MLE of  and , we differentiate L(,) partially w.r.t.  and  and equating it to zero. This
gives

k
k
L
x i ln(1  e  λt i )
x i ln(1  e  λt i 1 )


0
α 11
 λt i 1  α
 λt i  α
1 e
i 1  1  e


 1
1 
 1  e  λt i 
 1  e  λt i 1 




k
k
L
αt i x i e  λt i (1  e  λt i )α 1
αt i 1x i e  λt i 1 (1  e  λt i 1 )α 1


0
λ 11 (1  e  λt i )α  (1  e  λt i 1 )α i 1 (1  e  λt i )α  (1  e  λt i 1 )α
It is clear that no closed form solution is possible. We can use Newton-Raphson method to solve above two
equations.
The th percentile of (2.2) is given by X( θ )=-1ln(1-1/). Since θ  (λ, α) is unknown, we replace it by its
MLE

  
θ  ( λ , α ) and
ˆ1



I1 (x)  0, λ

we

propose

ˆ
ln(1  β1 / α )



approximate



upper

expectation

TI

as

.

Expected coverage of I1(X) is given by following theorem.
Theorem 1: An expected coverage of I1(X) is given by


2
E[ F{X β ( θ ); θ}]  β  A( θ)σ1  B( θ)σ 2  C( θ)σ12 ,
2

where

(2.3)

 G t G t 

λ
Aθ   0.5α1  α Gt α  2 G t 2  αGt α 1  xλ
 0.5G t  ,
λ
λλ
 Gx t 


 α  1Gλ t  Gxλ t 


.
Gt 
Gx t  


Bθ  α-1Gt α log Gt  1  0.5α log Gt , Cθ   Gt α log Gt  



G(t)  1  eλt

 Gx t  
,

G(t)/x, G t   G(t)/, G λ t   2G(t)/x,
λ
x

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27 | Page
Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data



Gλλ t   2G(t)/ 2 while 12, 22 are asymptotic variances of
 
 
Cov( λ , α ) is an asymptotic covariance of λ , α .



λ and α respectively and 12 =

Proof : Follows from the result of Atwood (1984). We omit the same for brevity.
The performance of I1(X) is studied using simulation experiments and has been reported in the Section 4. In the
following we obtain -content -level TI for the distribution (2.1).

III.

-CONTENT -LEVEL TOLERANCE INTERVAL


Let I2(X) = ( 0,  Xβ ) be an upper -content -level TI for the distribution having cdf (2.1). The
factor  > 0 is to be determined such that I2(X) is a -content -level TI for (0, 1) and (0, 1).

i.e.


ln 1 - β1/α  



 γ
P Xβ  

 λδ 




  


P F δ Xβ ; λ, α   β   γ . This implies

 


 






Assuming consistency and asymptotic normality of the MLE’s λ and α , we have

(3.1)



X β (θ) is

σ 2 (θ)
2
'
, where σ (θ)  H  H with  as a
n
  
xβ (θ) 
 xβ (θ)
variance covariance matrix of θ  ( λ , α ) and H  
,
.
α 
 λ
asymptotically normal with mean X β (θ) and variance

If Z is a standard normal variate then we can write from (3.1)
1/α



 ln (1 - β )
 n 
  1  γ ,
P Z  
 x β ( θ)
λδ

 σ(θ) 






 ln (1 - β1/α )
 n 


th

Z1 - γ  
 x β ( θ)  
Suppose
 σ(θ)  , where Z1- is the 100(1-) percentile of the
λδ





1
λ Z1  γ σ(θ) 

 .
standard normal variate then we have δ  1  ln(1 - β1/ α ) n 



Note that  depends on both the parameters  and . Replacing  and  in  by their respective MLEs an
asymptotic upper -content -level TI I2(X) is


  1


ˆZ
ˆ
λ 1  γσ(θ)  ln 1  β1 / α


0 ,  1 



ˆ
λ


ˆ
1/ α

ln 1  β
n




















(3.2)

The performance of I2(X) is studied using simulation experiments and has been reported in the Section 5.

IV.

SIMULATION STUDY

The approximate value of the actual coverage of the proposed  expectation TI is given by (2.3). The

ˆ
ˆ
performance of the said TI is illustrated by simulation technique by replacing  and  by its MLE’s λ and α .
In the simulation study of I1(X), we generate n (=10, 25, 50, 75, 100) observations from EE distribution with
=2 , =2 and groupe into five equal spaced intervals as 0- 0.5, 0.5- 1.0, 1.0- 1.5, 1.5- 2.0 and above 2.0. MLE’s
of  and  are otained and are used to compute upper - expectation TI of I1(X) for =.90, .95, .975 and .99.
Repeating the above procedure 10,000 times and estimate expected coverage reported in Table 4.1. Same
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28 | Page
Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data
procedure is repeated by grouping observations into five unequal spaced intervals as 0- 0.4, 0.4- 0.9, 0.9- 1.5,
1.5- 2.2 and above 2.2. The expected coverage reported in Table 4.2. We observe from Table 4.1 and 4.2 that for
small sample size TI underestimates expected coverage while as sample size increases coverage converges to
the desired level. It verifies the consistency property of the proposed interval.
Table 4.1: Expected coverage of - expectation TI (equally spaced)
n
10
25
50
75
100

0.90
.8518
.8794
.8854
.8934
.8982
0.95
.9042
.9422
.9456
.9470
.9482
0.975
.9330
.9650
.9687
.9728
.9766
0.99
.9520
.9802
.9842
.9864
.9880
Table 4.2: Expected coverage of - expectation TI (unequally spaced)
n
10
25
50
75
100

0.90
.8594
.8874
.8923
.8970
.8990
0.95
.9146
.9328
.9384
.9428
.9500
0.975
.9386
.9660
.9821
.9740
.9762
0.99
.9596
.9826
.9856
.9890
.9900
Upper -content -level TI given in (3.2) require asymptotic variance covariance matrix of the MLE’s

ˆ
ˆ
λ and α which involve complicated integrals to be solved numerically. This problem is resolved by using
bootstrap technique. In the following section we illustrate an application of the procedure by applying it to real
life data set.
V.

APPLICATION

Lawless data set (1982, page 228) is best fitted to EE distribution than two parameter Weibull and
Gamma as reported by Gupta and Kundu (2001).The data are regarding arose in test on endurance of deep
groove ball bearings. The data are the class of number of million resolutions before failure for 23 ball bearings
in the life test with equally spaced intervals as
Class interval
: 0-35
35-70 70-105 105-140 140No of ball bearings
: 3
12
3
4
1
For equally spaced data MLE’s of  and  are 0.0326 and 4.9536 respectively and upper  expectation
tolerance limits (say U1(X)) for various ’s are

: 0.90
0.95
0.975
0.99
U1(X) : 118.4462 140.3613
161.9405
190.2356
If the above data are with unequally spaced intervals as,
Class interval
: 0-35
35-55 55-80 80-100 100No of ball bearings
: 3
7
5
3
5
MLE’s of  and  are 0.0302 and 4.4747 respectively and upper  expectation tolerance limits (say
U2(X)) for various ’s are

: 0.90
0.95
0.975
0.99
U2(X) : 124.6725 148.3370
171.6484
202.2216
Using bootstrap technique we generate 5000 random samples (with replacement) each of size 23 from
the original data and group them with intervals equally spaced . For each of the bootstrap sample we compute
MLE’s of  and . Based on such 5000 MLE’s we obtain variance covariance matrix of MLE’s and is used to
propose asymptotic upper  content  level tolerance limit (TL) with combinations of =.90, .95, .975,.99 and
= .90, .95 and tabulated in Table 5.1. We also generate 5000 random bootstrap samples (with replacement)
each of size 23 from the original data and group them with intervals unequally spaced. By repeating the same
procedure as above ,we propose asymptotic upper -content -level tolerance limit and reported in Table 5.2.



Table 5.1: Upper -Content -level TL (equally spaced)
=.90
=.95
( θ )
U(X)
U(X)



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29 | Page
Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data
0.90
0.95
0.975
0.99

20.0795
23.5777
27.8883
34.3264


0.90
0.95
0.975
0.99

1.0475
1.0470
1.0482
1.0507

124.0667
146.9582
169.7526
199.8735

1.0615
1.0609
1.0626
1.0658

125.7353
148.9154
172.0740
202.7460

Table 5.2: Upper -Content -level TL (unequally spaced)
=.90
=.95
( θ )
U(X)
U(X)


20.9688
26.4637
32.4806
40.8536

1.0471
1.0501
1.0533
1.0571

130.5397
155.7630
180.7905
213.7621

1.0610
1.0650
1.0692
1.0742

132.2806
157.9746
183.5240
217.2288

It is observed that -content -level TI for equally spaced intervals has a wider length as against the
unequally spaced intervals.
The simulation study indicates that for small sample size TI underestimates expected coverage while as
sample size increases coverage converges to desired level. The performance of both the proposed TI’s are
satisfactory and can be used in practice. The method developed here can be extended for distributions belongs to
exponentiated scale family of distributions such as exponentiated Weibull, Exponentiated gamma or
Exponentiated Rayleigh distribution.

REFERENCES
[1].
[2].
[3].
[4].
[5].

Atwood C. L.(1984) : Approximate tolerance intervals based on maximum likelihood estimates, J.
Amer. Stat. Assoc. 79, 459-465.
Gupta R.C. and Gupta P.L. and Gupta R.D.(1998): Modeling failure time data by Lehman alternatives,
Communications in Statistics, Theory and Methods 27,887-904.
Gupta R. D. and Kundu D.(2001): Exponentiated Exponential Family: An alternative to Gamma and
Weibull Distributions, Biometrical Journal ,43 , 1,117-130.
Lawless J.F. (1982) : Statistical Models and Methods for life time data , John Wiley and Sons, New
York, pp. 228.
Kumbhar R. R. and Shirke D. T. (2005): Tolerance Intervals for Exponentiated Scale Family of
distributions , Journal of Applied Statistics, 32, 10, 1067-1074.

www.irjes.com

30 | Page

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International Refereed Journal of Engineering and Science (IRJES)

  • 1. International Refereed Journal of Engineering and Science (IRJES) ISSN (Online) 2319-183X, (Print) 2319-1821 Volume 2, Issue 10 (October 2013), PP. 26-30 Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data C. S. Kakade1, D. T. Shirke2 1 Principal, Anandibai Raorane Arts,Commerce and Science College, Vaibhavwadi, Sindhudurga. 416810, India. 2 Head, Department of Statistics, Shivaji University, Kolhapur. 416004, India. Abstract:- Upper -expectation and -content -level tolerance interval for exponentiated exponential distribution based on grouped data are considered. The adequacy of proposed tolerance intervals are evaluated using simulation study and through real life data due to Lawless (1982). Keywords : Exponentiated Exponential Distribution, Upper  expectation and  content  level tolerance interval, Maximum likelihood estimator, grouped data. I. INTRODUCTION Gupta et al. (1998) introduced the Exponentiated Exponential Distribution (EE) as a generalization of the standard exponential distribution. Gupta and Kundu (2001) Studied this distribution and observed that it can be used quite effectively in analyzing many life time data particularly in place of two parameter gamma and Weibull distributions. In their series of papers on EE distribution ( also named as Generalized exponential distribution), they discussed different estimation procedures, testing of hypothesis, construction of confidence interval, estimating the stress and strength parameter and closeness of generalized exponential with Weibull, gamma and lognormal distribution. Shirke et al. (2005) obtained -expectation and -content -level tolerance interval for this distribution based on ungrouped data. Many times in a life testing problem, it is not possible to record exact time of failure of a components due to several reasons. Hence it is more economical to observe no of failures of components in predefined time intervals which form grouped data. The main aim of this paper is to construct  expectation and  content  level tolerance interval for EE distribution based on grouped data. Let U be a statistic based on data observed from a distribution with density function f(x, θ ) where θ represents a vector of unknown parameters then the interval (-, U) is a -expectation tolerance interval (TI) if U  E   f ( x, θ)dx   β     for every θ  (1.1) and interval (-, U) is upper  content  level TI if U  P   f ( x, θ)dx  β  γ     for given ,  є (0,1). (1.2) U C is called the coverage of TI (-, U) if C  f (x, θ)dx .  One sided TI’s when f(x,) is a two parameter EE distribution based on maximum likelihood estimators for ungrouped data were discussed by Shirke et al. (2005). This paper extends the procedure for setting TI based on grouped data. In section 2 we provide upper -expectation TI along with its approximate expected coverage. -content -level TI based on MLE’s of  are discussed in section 3. We study the performance of both these TI using simulation technique in section 4. In section 5 we illustrate the practical applications of the procedure by applying it to real life data set. II. -EXPECTATION TOLERANCE INTERVAL Gupta and Kundu (2001) defined EE distribution in the following way. Let Y be a two parameter EE random variable with distribution function www.irjes.com 26 | Page
  • 2. Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data F( y, λ, α)  (1  e λy ) α ,,y>0, Therefore corresponding probability density function is given by f ( y, λ, α)  αλ(1  e λy ) α1 e λy . (2.1) ,y>0 (2.2) Suppose Xj , j=1,2,….,k be the number of observations in the interval (t j-1, tj] with t0=0 and tk= such that k  xi  n . Thus we have grouped data from the underlying distribution . i 1 The log likelihood function for the grouped data can be written as k L(λ, α / x )  C   x i ln F( t i )  F( t i 1) , where c is independent of  and  and F(.) is defined in (2.1). i 1 Therefore to obtain MLE of  and , we differentiate L(,) partially w.r.t.  and  and equating it to zero. This gives k k L x i ln(1  e  λt i ) x i ln(1  e  λt i 1 )   0 α 11  λt i 1  α  λt i  α 1 e i 1  1  e    1 1   1  e  λt i   1  e  λt i 1      k k L αt i x i e  λt i (1  e  λt i )α 1 αt i 1x i e  λt i 1 (1  e  λt i 1 )α 1   0 λ 11 (1  e  λt i )α  (1  e  λt i 1 )α i 1 (1  e  λt i )α  (1  e  λt i 1 )α It is clear that no closed form solution is possible. We can use Newton-Raphson method to solve above two equations. The th percentile of (2.2) is given by X( θ )=-1ln(1-1/). Since θ  (λ, α) is unknown, we replace it by its MLE    θ  ( λ , α ) and ˆ1  I1 (x)  0, λ we propose ˆ ln(1  β1 / α )  approximate  upper expectation TI as . Expected coverage of I1(X) is given by following theorem. Theorem 1: An expected coverage of I1(X) is given by  2 E[ F{X β ( θ ); θ}]  β  A( θ)σ1  B( θ)σ 2  C( θ)σ12 , 2 where (2.3)  G t G t   λ Aθ   0.5α1  α Gt α  2 G t 2  αGt α 1  xλ  0.5G t  , λ λλ  Gx t    α  1Gλ t  Gxλ t    . Gt  Gx t    Bθ  α-1Gt α log Gt  1  0.5α log Gt , Cθ   Gt α log Gt    G(t)  1  eλt  Gx t   , G(t)/x, G t   G(t)/, G λ t   2G(t)/x, λ x www.irjes.com 27 | Page
  • 3. Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data   Gλλ t   2G(t)/ 2 while 12, 22 are asymptotic variances of     Cov( λ , α ) is an asymptotic covariance of λ , α .  λ and α respectively and 12 = Proof : Follows from the result of Atwood (1984). We omit the same for brevity. The performance of I1(X) is studied using simulation experiments and has been reported in the Section 4. In the following we obtain -content -level TI for the distribution (2.1). III. -CONTENT -LEVEL TOLERANCE INTERVAL  Let I2(X) = ( 0,  Xβ ) be an upper -content -level TI for the distribution having cdf (2.1). The factor  > 0 is to be determined such that I2(X) is a -content -level TI for (0, 1) and (0, 1). i.e.  ln 1 - β1/α       γ P Xβ     λδ          P F δ Xβ ; λ, α   β   γ . This implies           Assuming consistency and asymptotic normality of the MLE’s λ and α , we have (3.1)  X β (θ) is σ 2 (θ) 2 ' , where σ (θ)  H  H with  as a n    xβ (θ)   xβ (θ) variance covariance matrix of θ  ( λ , α ) and H   , . α   λ asymptotically normal with mean X β (θ) and variance If Z is a standard normal variate then we can write from (3.1) 1/α     ln (1 - β )  n    1  γ , P Z    x β ( θ) λδ   σ(θ)         ln (1 - β1/α )  n    th  Z1 - γ    x β ( θ)   Suppose  σ(θ)  , where Z1- is the 100(1-) percentile of the λδ      1 λ Z1  γ σ(θ)    . standard normal variate then we have δ  1  ln(1 - β1/ α ) n    Note that  depends on both the parameters  and . Replacing  and  in  by their respective MLEs an asymptotic upper -content -level TI I2(X) is    1   ˆZ ˆ λ 1  γσ(θ)  ln 1  β1 / α   0 ,  1     ˆ λ   ˆ 1/ α  ln 1  β n               (3.2) The performance of I2(X) is studied using simulation experiments and has been reported in the Section 5. IV. SIMULATION STUDY The approximate value of the actual coverage of the proposed  expectation TI is given by (2.3). The ˆ ˆ performance of the said TI is illustrated by simulation technique by replacing  and  by its MLE’s λ and α . In the simulation study of I1(X), we generate n (=10, 25, 50, 75, 100) observations from EE distribution with =2 , =2 and groupe into five equal spaced intervals as 0- 0.5, 0.5- 1.0, 1.0- 1.5, 1.5- 2.0 and above 2.0. MLE’s of  and  are otained and are used to compute upper - expectation TI of I1(X) for =.90, .95, .975 and .99. Repeating the above procedure 10,000 times and estimate expected coverage reported in Table 4.1. Same www.irjes.com 28 | Page
  • 4. Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data procedure is repeated by grouping observations into five unequal spaced intervals as 0- 0.4, 0.4- 0.9, 0.9- 1.5, 1.5- 2.2 and above 2.2. The expected coverage reported in Table 4.2. We observe from Table 4.1 and 4.2 that for small sample size TI underestimates expected coverage while as sample size increases coverage converges to the desired level. It verifies the consistency property of the proposed interval. Table 4.1: Expected coverage of - expectation TI (equally spaced) n 10 25 50 75 100  0.90 .8518 .8794 .8854 .8934 .8982 0.95 .9042 .9422 .9456 .9470 .9482 0.975 .9330 .9650 .9687 .9728 .9766 0.99 .9520 .9802 .9842 .9864 .9880 Table 4.2: Expected coverage of - expectation TI (unequally spaced) n 10 25 50 75 100  0.90 .8594 .8874 .8923 .8970 .8990 0.95 .9146 .9328 .9384 .9428 .9500 0.975 .9386 .9660 .9821 .9740 .9762 0.99 .9596 .9826 .9856 .9890 .9900 Upper -content -level TI given in (3.2) require asymptotic variance covariance matrix of the MLE’s ˆ ˆ λ and α which involve complicated integrals to be solved numerically. This problem is resolved by using bootstrap technique. In the following section we illustrate an application of the procedure by applying it to real life data set. V. APPLICATION Lawless data set (1982, page 228) is best fitted to EE distribution than two parameter Weibull and Gamma as reported by Gupta and Kundu (2001).The data are regarding arose in test on endurance of deep groove ball bearings. The data are the class of number of million resolutions before failure for 23 ball bearings in the life test with equally spaced intervals as Class interval : 0-35 35-70 70-105 105-140 140No of ball bearings : 3 12 3 4 1 For equally spaced data MLE’s of  and  are 0.0326 and 4.9536 respectively and upper  expectation tolerance limits (say U1(X)) for various ’s are  : 0.90 0.95 0.975 0.99 U1(X) : 118.4462 140.3613 161.9405 190.2356 If the above data are with unequally spaced intervals as, Class interval : 0-35 35-55 55-80 80-100 100No of ball bearings : 3 7 5 3 5 MLE’s of  and  are 0.0302 and 4.4747 respectively and upper  expectation tolerance limits (say U2(X)) for various ’s are  : 0.90 0.95 0.975 0.99 U2(X) : 124.6725 148.3370 171.6484 202.2216 Using bootstrap technique we generate 5000 random samples (with replacement) each of size 23 from the original data and group them with intervals equally spaced . For each of the bootstrap sample we compute MLE’s of  and . Based on such 5000 MLE’s we obtain variance covariance matrix of MLE’s and is used to propose asymptotic upper  content  level tolerance limit (TL) with combinations of =.90, .95, .975,.99 and = .90, .95 and tabulated in Table 5.1. We also generate 5000 random bootstrap samples (with replacement) each of size 23 from the original data and group them with intervals unequally spaced. By repeating the same procedure as above ,we propose asymptotic upper -content -level tolerance limit and reported in Table 5.2.  Table 5.1: Upper -Content -level TL (equally spaced) =.90 =.95 ( θ ) U(X) U(X)   www.irjes.com 29 | Page
  • 5. Tolerance Interval for Exponentiated Exponential Distribution Based on Grouped Data 0.90 0.95 0.975 0.99 20.0795 23.5777 27.8883 34.3264  0.90 0.95 0.975 0.99 1.0475 1.0470 1.0482 1.0507 124.0667 146.9582 169.7526 199.8735 1.0615 1.0609 1.0626 1.0658 125.7353 148.9154 172.0740 202.7460 Table 5.2: Upper -Content -level TL (unequally spaced) =.90 =.95 ( θ ) U(X) U(X)   20.9688 26.4637 32.4806 40.8536 1.0471 1.0501 1.0533 1.0571 130.5397 155.7630 180.7905 213.7621 1.0610 1.0650 1.0692 1.0742 132.2806 157.9746 183.5240 217.2288 It is observed that -content -level TI for equally spaced intervals has a wider length as against the unequally spaced intervals. The simulation study indicates that for small sample size TI underestimates expected coverage while as sample size increases coverage converges to desired level. The performance of both the proposed TI’s are satisfactory and can be used in practice. The method developed here can be extended for distributions belongs to exponentiated scale family of distributions such as exponentiated Weibull, Exponentiated gamma or Exponentiated Rayleigh distribution. REFERENCES [1]. [2]. [3]. [4]. [5]. Atwood C. L.(1984) : Approximate tolerance intervals based on maximum likelihood estimates, J. Amer. Stat. Assoc. 79, 459-465. Gupta R.C. and Gupta P.L. and Gupta R.D.(1998): Modeling failure time data by Lehman alternatives, Communications in Statistics, Theory and Methods 27,887-904. Gupta R. D. and Kundu D.(2001): Exponentiated Exponential Family: An alternative to Gamma and Weibull Distributions, Biometrical Journal ,43 , 1,117-130. Lawless J.F. (1982) : Statistical Models and Methods for life time data , John Wiley and Sons, New York, pp. 228. Kumbhar R. R. and Shirke D. T. (2005): Tolerance Intervals for Exponentiated Scale Family of distributions , Journal of Applied Statistics, 32, 10, 1067-1074. www.irjes.com 30 | Page