estimation of the mean life of the exponential

78
.. ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL DISTRIBUTION FROM GROUPED DATA WHEN THE SAMPLE IS CENSORED - WITH APPLICATION TO LIFE-·TESTING by PETER JAMES KENDELL and Rt L, ANDERSON Institute of Statistics Mimeograph Series NOt 343 February) 1963

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Page 1: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

..

ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIALDISTRIBUTION FROM GROUPED DATA WHEN THE SAMPLEIS CENSORED - WITH APPLICATION TO LIFE-·TESTING

by

PETER JAMES KENDELL

and

Rt L, ANDERSON

Institute of StatisticsMimeograph Series NOt 343February) 1963

Page 2: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• ERRATA SHEET

Page 6, Last line:

" re = zi=l r I • • •

Should be:

rZ t i + (n-r)t

&= i=l rr - , .. . .

Page 7, Line 7A re = z

1=1

t i + (n-r)t

r .. . .

Should be:

rZ t

i+ (n-r)t

&=...1....=1 _r . .. ..

. . .

Page 14, Line 7:

Should be:

(X~fi - X~-lf)(Fi - Fi - 1 ) •• •

(X~fi - X~-lfi-l){Fi - Fi - 1 )

Page 14, 2nd line from bottom:

.. • • ni < n .. · •

Should be: • • · ~ <n .. · ·Page 14" Last line:

· • • n = n .. · ·i

Should be: · · • ~ = n • · ·"Page 17" Equation (3.,.8):

" 1e =:2 • • •

Should be:A 1e =-1 2 • • •

Page 22"

· . .

· . .

Page 3: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Page 2

ERRATA SHEET

Page 24, 2nd line of Equation (4.2.9):• pt

::: nQ2e •

Page 24, Equation (4.2.11): R(e; 00 1 8,k) •••

Should be: = ptnQ2e

A

Should be: R(eoj 00" 8"k) •

11 + '14: • • •

"" A eoe =e --r.- g1 0 If

Should be:

Should be:

Page 26" Last line of Equation (4.3.7):::: Q~ ••• Should be: = Q1 •••n~~ nk~

{8e8 t k 8 1}2Page 27" Last line of Equation (4.3.10): + - - - - - + nt E(-) - 1

e8_1 ~+1 2 k r

+{

8e8 _ ~t_k~ 8 ntk 1 ]2Q_ e - ;:; + -e E(-) - 1 •

~-1 ~~ ~ rA

,., " eo {e1 = eo - T g

t1 + l; .. ·" c= eo (1 - 'ij:)' say,

Page 35, First line of Equation (4.5.1):

Page 35, Last line of Equation (4.5.1):

A CShould be: = eO (1 - 'ij:)' say,

. . .

Page 35, Line 7:

Page 35,

Should be:

Should be: C= g \1 +

* 2I: nihi

{z2

l'<

1 PigihiPage 37, Line 9: • . • =E(-)~+1

• • •r

21 t* P1

g1

hiShould be: • . • = E(-) - • • •r Qk+l

" A

Page 40, Line 4: • . . relatively small eO" e2A A

Should be: • . • re1ative1y small n eo" e2

Page 4: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

rex) = ••

,Page 48, First line:

ERRATA SHEET

Should be: rex) = . . .

Page 3

Page 49, Line 10; lt g(x) =s-> 0

Should be: lt g(s) =s-> 0

• • •

Page 53, Line 14; ~-2,1 . . . h ~-2,k-lk-2-k-2

Should be: ~-2,1 ~-2,k-2 ~-2,k-l

Page 55, Line 12; ( _1)k-2d • . • 2 + ~,k+l11

Should be;

Page 65, Second line: "-e =1 . . .

Should be: '"e =1

. . .

Page 68, Line 3: Should be:

Page 69, Reference 5 (EPstein): Add; Detroit, Michigan.

Page 70, References 19 and 20 (Lehman and Mendenhall):

Add: (Un1versity Microfilms, Ann Arbor)

Page 5: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•iv

TABLE OF CONTENTSPage

CHAPrER 1 - INTRODUCTION •• • • • • • • • • • • • • • • • • • • • 1•

CHAPrER 2 - REVIEW OF LITERATURE • • • • • • • • • • • • • • • • • 4

CHAPrER 3 - MAXIMUM LIKELIHOOD ESTIMATION OF a • • • • • • • • • • 10

3.1 Test Procedure • • • '. • • • • • • • • • • • • • • • • • •• 103.2 Derivation of' the Maximum. Likelihood Estimator • • • • • •• 103.3 Existence and uniqueness of the Maximum Likelihood Estimator 123.4 Iterative Estimation Procedure • • • • • • • •• • • • • •• 153.5 Simplif'ication of' the Maximum. Likelihood Equation • • • • • 153.6 Modif'ied Maximum Likelihood 'Estimator •• • • • • • • • •• 17

A

CHAPrER 4 -PROPERTIES OF THE ESTIMATOR ~O ••• • • • • • • • •• 19A

4.1 Mean and Variance of' aO ••••••• • • • • • • • • • • • 19A '

4.2 Bias in ao • • • • • • • • • • • • • • • • • • • • • • • • • 22- A

4.3 An EXpression f'or Var(e.o) ••••••••••••••••• 244.4 On the Non-Monotonicity Property • • • • • • • • • • • • • • 28

A

4.5 Eff'ect of' Neglecting Terms in al

• • • • • • • • • • • • • • 35A,

4.6 Comparison between e.0 and the M.L.E. (Equal Spacing) • • • • 46

CHAPrER 5 - OPrIMAL DECOMPOSITION OF THE SAMPLE SPACE •

5.1 Introduction. • ~. • • • • • • •5.2 Determination of' the Decomposition5.3 A Numerical Exa:rrq>le •••••••

• •• •· .

• •• •• •

• • • • • •

• • • • • • • • •• • • • • • • • •• • • • • • • • •

47

474757

• •

CHAPrER 6 - Stnv1MARY, CONCLUSIONS AND RECOO1ENDATIONS FOR FURTHERRESEARCH • • • • • • • • • • • • • • • • • • • • • • • • • •

LIST OF REFERENCES • • • • • • • • • • • • • • • ~ • • • • • •

• • 63

69

Page 6: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•v

LIST OF TABLES

Page

4.2.1(a). E(~) = ~ ~ (~) ~+l ~~~ / l-~+l •• • • • • • • • • 29r=l .

4.2.1(b). V(~) = E(~) - (E(~»2, wherer

1E('"'2)

r• • . . . . . . . 30

4.5.3.

4.5.4.

" ,Bias of e.O N ~qually spaced case • • • • • • •• • • • • 31,.. "

Variance of eON equally spaced case • • • • • • • • • • 33

Approximations to the upper bound of the correctionfactor N equally spaced 'case (as percentages of e) • • 38

, A

Approximate bias of e.2 N equally spaced case • • • • •• 41.A

App~oximate variance of e2 N equally spaced case. • •• 42

A "Comparison of the mean square ... errors of eo' e2 and the

maximum likelihood estimator (ungrouped) - -equallyspaced c~se • • • • • • • • • • • • •• • • • • • •• 43

Page 7: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• CHAPI'ER 1

INTRODUCTION

The 'longevity of animate and inanimate objects under certain

environmental conditionsis -of the utmost importance in :rna.ny fields.

Actuaries have long been interested in the life-span of human beings,

and, +n more recent times, industrialists and engineers have been con­

cerned with the reliability 'of a product, a component, or a system of

components, under certain decremental stimuli.

In each 'instance the obj ect under study is characterized by a

measurable life-span which varies with the amounttm.d ty,pe of stimulus

applied. The process is analogous to the variation in crop yield in an

agricultural experiment. The length of life is determined by some pre­

stated definition of "failureft, whether it is the inability of the

object to measure up to some prescribed standard or even outright de-

struction.

To investigate the ftmortality' characteristics of an obj ect under

certain stress conditions we require knowledge of its underlying mor­

tality curve or failure distribution. Although the form of this dis­

tributionvaries according to the' item studied, most generally it

follows an exponential or modified exponential type, e.g. Weibull dis­

tribution [29]:

g(t) =

o

t ~ t'" a, M > 0

t < t' •

(1.0.1)

Page 8: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• If a sample of items is place'!: on test and subjected to a 'stress,

for economic reasons it may be inappropriate to continue testing until

all have failed. This arises firstly, because the failure time of the

last item may be indeterminably long, and secondly, because in practice

it may be too costly to destroy all of the units on test. In other

words, exact infol"Illation about some of the units and partial informa­

tion on the others is often a prer'equisite of a life-test. Such a

procedure is called a censored sampling plan. Here, we mustdistin­

guish between censoring and truncation. A censored sam;ple may be

defined as one in which all variate values beyond a certain range are

unknown, but their number is known; whereas, in a truncated procedure

we have no way of determining either the values or the number of var­

iates beyond a certain range. It is this partial statistical informa­

tion which, except in the simplest cases, tends to complicate the

statistical techniques associated with censoring.

Most generally life-tests are of the single censoring variety, the

type depending on the particular stopping rule adopted.: e.g.,

I. Stop after a prescribed number of units (1') have failed,

(O<r<n),

II. Stop after a prescribed duration of time (t) has elapsed,

(t > 0),

III. Stop after a prescribed time t if l' or more units, have

failed, otherwise continue the test until l' have f~led,

and in particular, most of the research yet performed has considered

the effect of a single stress on the life-span of a subject. A more

Page 9: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

3 _

practical result" however" would be a study of the effect of several

factors acting together. Some notable research along this line was

published by Zelen [31; 32]" who considered the estimation and inferen-

tial problems arising from such a factorial arrangement under the

assumption of an underlying exponential failure distribution.

However" an objection to almost all of the research yet published

in the field of life-testing is that it presupposes that individual

failure times are recorded. In certain experiments on electronic

equipment and so forth" this may not present a problem" but in life­

tests 'on component parts of machinery" for example, this requirement

may necessitate an expensive timing arrangement, whether it is human or

mechanical; and,. in certain biological studies where the effect of a

stress on a primitive organism is measured in terms of dilution, it may

be absolutely impossible to obtain exact failure times.

The above" then, is the genesis of the problem considered in this

research. How do we estimate the parameters of a failure distribution

when the data are collected not individ~ly but at certain sampling

points" and what effect does this grouping of info:rma.tion have on the

properties of the estimator? In particular, wenll consider the

estimation of the mean life, e, when the mortality distribution is of

the exponential type:

e.

1 te exp- e 'g(t) =

o

t > 0" e > 0

otherwise •

(1.0.2) .

Page 10: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

4

CHAPrER2

REVIEW OF LITERATURE

The problem of' analyzing f'or essentially continuous variates

grouped data is f'air1y old in the realm of' statistical methodology. As

long ago as 1898 Sheppard [26] asserted that if' one used equally spaced

intervals1 corrections could be made to the moments of' the discrete

distribution to bring them closer to those of' the continuous distribu-

tion.

In 1934 Wold [30] 1 again f'or the case of'equal spacings1 gave the

general expression f'or any moment of'the continuous distribution in

terms of' the "raw" moments of' the discrete distribution1 except for an

error term. Kendall 117] investigated this error term and gave condi­

tions for the validity of Sheppard's corrections.

Gj eddeba~k in a series of papers ([ 7 ]" [8 L [9], [10] 1 [11])

considered the problem of estimating the mean and variance of a normal

distribution from coarsely grouped data" by use of maximum likelihood.

The likelihood equations requir.ed an iterative solution. The asymptotic

eff'iciencies of the estimators were considered along with their asymp-. .

totic distributions. Kul1dorf [18] considered the necessary and suf'fi-

cient conditions for the existence and the uniqueness of estimators f'or

the case of a normal distribution and determined an optimum allocation.

Walker [28] investigated the more general problem of the estimation

of a parameter from a continuous distribution by the use of maximum

likelihood1 when the data are arbitrarily grouped1 and gave a proced'l.:Q:'e

for obtaining a deco~osition of' the sample-space which is optimal in

Page 11: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•5

the sense that it maximizes the information (in the Fisher sense)

inherent in the sample.

In more recent times a great deal of research, as evidenced by the

bibJiogralib.Y of Mendenhall [21], has been carried out on the statistical

theory of censored sa.m;pliDg, and in its application to life-testing

prob).ems. Although a censored sample differs from one that is trun­

cated, research on both has often appeared jointly in the literature.

One of the earliest papers in this field was that of Hald U5] who

considered maximum likelihood estimation of the mean and variance of a

normal distribution for both truncated and censored samples, and gave

tables for iteration of the estimates and for evaluating the asymptotiC

covariance matrix.

Cohen £2] darived maximum likelihood estimators for siDgly and

doubly truncated normal distributions under fixed time censoriDg, the

solutions being in a form suitable for· the use of normal tables. In a

later paper [3] he obtained moment estimators for the parameters in

truncated Pearson type distributions and stated that these 'Would pro­

vide suitable first approximations for iteration of maximum likelihood

estimates.

A more general paper was that of Halperin [16] who considered the

maximum likelihood estimation of a parameter e from censored· and. trun­

cated samples, when the underlyiDg probability density function f(x; e),

is subject to certain mild regularity conditions. He found that the

estimator is consistent, asymptotically norinal and of minimum variance

for large samples.

Page 12: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•6

Gupta [14] studies the estimation problem for a normal distribution

when censoring occurs after a fixed number of units has failed. Best

linear unbif¥led estimators of the mean and standard deViation were ob­

tained by· using the method of least squares on the ordered vat"iates

~ < ~ < ••• < xr " r ~ n" trom a s~le of sizen. The estimators

were of the form

,. rC1 = 1: c.x. ,- i=l ~ ~

the coefficients bi , ci being tabulated for samples of size n = 3(1)10

and r = 2(1)n-l. The variances and covariances are given.

Best linear unbiased estimation was also- used by Sarhan and

Greenberg [25] again for the parameters of a normal distribution when

the sam;pling procedure was such that the smallest kl and the largest

k· items were not measured (i.e., doubly censored).2

Epstein and Sobel [6] gave procedures for estimation and tests of

hypotheses in the case of. sampling trom an: exponential distribution in

which only the first r ordered units from a sample of size n are

measured. In a later .pa;per Epstein [5]· gave more general results· for

censored sampling with and without replacement of failures. Procedures

were given for the case of a fixed number of failures r" and a -fixed

test termination time t. In the first instance the :maximum likelihood

estimates of the average life is

e= ~ t i + (n-r)tr. i:i;l . r '

without :replacement case

Page 13: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•7

, 'With replacement case.

. A .

When r is specified, e has the property of being unbiased, su:f'ficient2· A

and of minimum variance, V(~) =!... The distribution of 2r ~ isr· 1;1

that of chi-square 'With 2r degrees of freedom. When censoring occurs

at a fixed time, t, the number of failures r (r > 0), being a random

variable, then

A re = 1:

i=l

A nte = ­r

t i + (n-r)t

r 'Without replacement case"

'With replacement case.

The estimator is not unbiased although it has all of the usual asymp-

totic properties of consistency and minimum variance.

Mendenhall (20] considered the estimation problem for santPling

from a mixed failure population in particular when the probability

density function is of the form:

e -tl/Ol -t/a2p - + (l-p) !L

.Ol ~f(t) =o

, t>o

otherwise•

He considered' the maximum likelihood estimators of p, Ol and ~

along 'With their .. large sample properties. The estimators are badly

biased and· have large variances for small sample sizes and test termina­

tion time t. Mendenhall and Hader Ha] extended the above results to

a mixture of k sub-populations •

Lehman (19] considered the estimation of the scale parameters of a

Weibull distribution for sampling under a mixture of two stopping rules--

Page 14: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•8

stop at time t if r or more units have failed, otherwise continue

the test until r have failed. The bias and variance of this esti-

mator are both non-monotonic as functions of the sample size.

This same non-monotonic property is exhibited by the estimator of

t]:J.e· exponential parameter when censoring occurs at a fixed time (see

e.g. Bartholomew [1]).

When censoring occurs at a fixed time the maximum likelihood

estimators are functions of inverse moments of a truncated binomial

distribution. Several writers (e.g. Bartholomew [1], Grab a.I+d Savage

[121, Mendenhall and Lehman [23], and Stephan [271) consider large

sample approximations to these moments, and Grab and Savage give the

exact results tabulated for .

p = .01, .05 ( .05) .95, .99 and n = 2(1)20

( .05)~

and for p = .01, .05 .50, .99 and n = 21(1)30.

One of the few papers to consider the joint problem of censored

sampling and grouping of the data was that of Grundy [13], who investi­

gated the estimation of the parameters.ofa nornial distribution when

censoring is to the right and the data groUJ;>ed. Using as class bound-

aries

where Xo = 0:; ~ = 00

and observed frequencies

and defining ~'adjusted" moments of the form

Page 15: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•9

he obtained likelihood equations as fmctions of ~ and ~ • After

expanding M:t and ~ as power series, tTl.mcating the series and

substituting for M:L and ~, the likelihood equations were reduced to

a form which enabled a simpler iterative procedure using tables from

Ha.ldt s [15] paper.

A recent pSsPer by Ehrenfeld [4] considers the estimation of the

mean life of a component when the failure distribution is of the expo­

nential form and sampling stops at some time t k, the interval (0, t k )

being divided into k equal groups. For the case of equal spacing the

likelihood permits an explicit solution

§ = -~.....;;A:::...----r--

In.[ 1+ ~ xj / ~ s J 'j=l j=l ~

where

Xj = observed frequencies j = 1, ••• ,k •

Sj = n - (Xl +~ + •••. + x.) •J....

The asymptotic variance of e is derived and compared With that for the

ungrouped case.

Page 16: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• CHAPrER 3

MAXIMUM LIKELIHOOD ESTIMATION OF e

3.1 Test Procedure

A number of items (n} are subjected to a certain stress condition

for a predetermined period of time (t = tk

). At certain time intervals

(ti

_l , t i ) during the life.,.test the number of items that do not come up

to specification or have failed since the previous inspection are

counted, and removed from the life-test.

Asa direct result of this sampling plan we have a multinomial

situation in which the probability of an item failing in a specified

interval of· time is a function of the unknown parameter (e).

The class boundaries are:

'With observed frequencies:

~, ~, ... , ~, ~+l; where the number of items having failed is

kr = i~l ni and the number of survivors iS~+l = n:-r •

3.2 Derivation of the Maximum Likelihood Estimator

The probability of an i tern failing in the interval (ti

_l , t i ) is

given by

Since the distribution of failure times is assumed to. follow the

exponential law

Page 17: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•11

t > 0 ,- ,

g(t)=o , otherwise

then,

fl ­G(t) :: 10

texp- .~, t > 0

otherwise •

Putting Xi:: tile then

hob (ti_l~t<ti) = hob (xi_l~x<xi)

= F(Xi

) - F(xi

_l

)

Xi ~ 0

otherwise •

From the multinomial property the joint density of the sample can

be wr~tten 11

•hence

Differentiating with respect to the unknown parameter (e) yields

butdFi dFi dX. ":xif .

J. . J.

~= dix

e,

W::;, e- ,

i

l/For purposes of'notation we will henceforth use

k+l k1:;;: 1:, 1:* =:;. ~, Fi = F(Xi ), f 1 = exp- Xi •

1=1 1=1

Page 18: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•12

hence

C~.2.,5)

a result analogous to that obtained by Gjeddebaek [7J in estima.ting

from grouped data" the standard deviation of a normal distribution.A

The maxim:um likelihood estimator (9) is thus a solution" if one

exists" to the equation

3.' Existence· and tJniqueness of the Maximum Likelihood Estimator

To determine the existence of a root to equation (3.2.6) we must

Gonsider the sign' of the first derivative" . O~riL" over the parameter

space" (o~' 9 <'0).

Putting

since Xi > xi _l " we can write

From the definition of Xi we can see that

~t xi = 00" i = 2" ••• "k+l ,8->0

hence" ~t Yi = ~t

xi -> 0). xi _l -> 00

Xi

_l [8i

- ex,p- xi

_l (1-8i

)J

1 - exp- xi _l (1-8i '= -00 ,

i = 2" ••• , k •

Page 19: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•13 -- --

= 0

.et Yk;+l .. .et - "k ;: -co •

*k-> 00 ~->··oo

Thus.et O~nL = 00 if at lea.stone observation exceeds t 1 ,e":"'> 0 . '.

Sim;tla.:rly, for large e,

.et xi = 0 i =1",.,k,e-> Q)

hence, .et Yi =x

i_1-> 0

.et

xi~i-> 0

Xi_1

(5i-exp- Xi _

l(1-8:i)J

l' - exp- X:i-l(1-51 )= 1,

= 1,Xl exp- ~

1 - exp- Xlx1-> 0

.et Y =.et1~->o

and, .et - ~Xk-> 0

= 0-,

from which we can infer that .et· oW' = 0- if at least one obser-9-> 00"

vation is less than t k, Hence a root exists to the equation (3.2,6)

if ~ rn and ~+1 rn.

The uniqueness of a root can be determined by consideration of the2 .

. .' olnLsign of the second, derivative, . . 2 • Now,

. oe '

d~r =_~2 1: ni[<xi -2;~f~;~~~i~~_1>fH' + (l'~:i:X~~~ri"1>J.

(3.3,1)

Page 20: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•14

'021nLFor values of e satisfying the likelihood equation (3.3.1), .;;...;;~;.... ?j32

becomes

Let us consider the expression in the square brackets:

say,

then,

Since Fi - Fi-l = -(fi - f i _l ) when F(x) = 1 - exp- x" x ~ 0 ,

then

~2

Tl+erefore" 0 l~ . < 0 for all 8, (0 < 8 < GO), which im,plies that the'de

likelihood eqUation (3.2.6) possesses at most one root which is a ma.xi-

mum. " The above may be summari~ed as "follows:

Theorem 3.".1

The likelihoodecauation for 8 is given by

t i exp- tile - ti_l,exp- t i _1/81: ni ( exp-t /e _ exp- t /8 ) = 0"

i-l " i

and possesses a root which is a unique"maximum if nJ < n and ~+l <n,

but has no a.cceptable root if either ." n, = n or ~+l =n.

Page 21: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•15

3.4 Iterative Estimation Procedure

Using (3.3.2) and the property of the multinomial distribution

E(ni ) = n(Fi - 'i-l) ,

we obtain

2-E(~ lnL)

?lJ2

G(e)

Denoting the left hand side of (3.2.6) by g(e) and putting

2(xifi - xi_lfi _l )

= 1: " F _ F 'i i-l

then by the method of scoring (see, e.g. Rac> [24], pp. 166-167) startingA

with an initial value of e we can USe the iterative formula

'"~j+l=

e'"

'" '" AIn practiceG(~j) will tend to stabilize quickly as ~j-> e and

hence it will be unnecessaI-y to recompute it after each iteration. If

we have a large number of classes, however, the' i terat1ve procedure can

become tedious atLd we might ask ourselves the question:"Is there a,

simp~e:t: wq of obtaining a solution to the likelihood equation? "-

The following is an attempt at, answering this question.

3.5 Simplification of the Ma.x:LmUm Likelihood Equation

Let us define ,gi = (ti + t i _l )/2 ,

ui = gi/8 , i = 1,2, .... ,k,

and hi =ti - ti~l'

Page 22: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

then Xi = Ui + hi/2a

:-X.i~l= ui - hi/28,

16

from which we can write,

Similarly,

thus

Expanding coth hi/2a .as a power series we have

xi:f'i- xi_l1'i_l = u. _ h 12a{ 28 [1 + !(h 128)2 + O(h 128)4])1'i - 1'i_l ' J. i l hi _ 3 i i·

=~ - (1 + h~/12a2) + O(hi/2a)4 • (3.5 •.2)

The likelihood equation (3.2.6) can be written as

* Xi1'i - xi_l:f'i_lE. ni ( 1'i -1'1_1 ) + ~+l xk = 0,

and substituting (3.5.2) into (3.5.3) we obtain, except for O( hi /28 )4,

= r.

But ui = gila, hence (3.5.4) becomes* 2

2 ~ nigi + (n-r) t k * nilli8 . - ( . r .' ) 8 + ~ 12r = 0

Page 23: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

17

• and putting

A

~O =*1:_ niSi. (n-r) t k

r

it reduces further to

The solution to this equation.,

is an approximation to the maximum likelihood estimator of e.· WeA

observe from (;.5.6) that ~o exists if r > 0 (Le., ~ < n), and

2A A 2 * ni 11i ..... r:: "-

from (;.5.8) that ~l exists if ~o > 1:, 3r or max [hi] < V; eo •"-

If ~ = n, from (;.5.6) we can see that eO = Sl and from (; •.5.8)

that 81 <V3~, hence ~l does not exist for ~. ~ n.

;.6 Modified Maximum. Likelihood Estimator

From (;.5.8) we observe that

"-and if in this expression max [hi] is small relative to eo" such that

we may neglect the correction term., the approximate maximum. likelihood

estimator reduceS to

Page 24: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•18

We know (Section 3.3)thS.t a non-zero m. 1. estimator is non-

existent for the case when z:t= n, however, in general an experimenter

would desire an estimate when this occurred, even though it would not

"be m. 1. :From thedefinitioIi of 80 (3.5.6), we see that we can obtain

"an estimate when n=z:t, since 80 exists and is given by

the mid-point of the first time interval.

""As a result, it is suggested that 8.0 would be a suitable esti-

mate of 8, which would include the case when n ='.ll..

Page 25: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

19

CHAPrE'R 4

PROPERTIFS OF -Tim FSTIMATOR ~0

~

4.1 Mean and Variance of ~o

'"Since ~0 is defined eJtcept for r = 0 we Will derive the mean and

variance conditional upon the event r > O.

in consequence given by

But,

A I 1 * I n-rE(80 !) =r E(E nigi !) + r tIt '- -. ..

The mean value of ~ is,0

(4.1.1)

. where

Hence,

A Pigi 1 21E(8 ) = E* -- + nt E(-Ir> 0) - t .-

,0 _ \:+1 k r ~ It

/

In a similar fashion:

var(~o) =Var("E* nig

i ) + var(ntk ) + 2nt,. cov(!, E* nig

i ) •_ r ' r. A r . r

Considering each term of (4.1.;) separately we obtain:

(4.1.2)

(4.1.;)

!/Where two expectation signs appear together the inner one willdenote eXPectation over the ni(i=l, ••• ,k) such that I:*'ni=r, and

. the outer one over r given that r >0 •

g/For simplicity we will denote .E(~I! > 0) by E(~).

Page 26: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

20

but,

Hence, 2 2n·gi . * PigJ.· P g

Va:r(r.*....L.) =, [r. - - (r.*.J:..l) 1 E(!) •,r Qk+l - ~+l r

Simila:rly,

'e

and,

(4.1.6)

Page 27: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

21

Thus, stibstituting(4.1~4), (4.1.5) and (4.1.6) into (4.1.3) we obtain

p 2 P 2

var(~o) =(Jrtk)2 var(f) + £1:* ~~. (F.* ~:~) 1 E(f). (4.1.7)

A. ....

From (4.1.2) and (4.1.7) we observe that bothE(~O) and var(~o)

are functions of certain truncated inverse moments of r, which can be

obtained directly from:

1 n 1 n) ~+1 ~~~E(~) = Z ~ (r n·

r r=l r 1 - Pk+l(4.1.8)

For large values of n and Qk+l' such that n~+l > 10, Grab and

Savage [12] suggest the approximation

and Bartholomew [1],

(4.1.10)

Mendenha;J..l and Lehman [25] suggest approximating (4.1.8) by equatins.'

the momeniis of a Beta distribution. Their solutions for the mean and

variance are

1 n-2E(;) = n(a-l)

where a = (n-l) ~+1 •

(4.1.11)

Page 28: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•22

A

4.2 Bias in ~o

We have seen from (4~1.2) that

It is of interest to obtain an explicit,solution where possible for the

A

In general, of course, the bias B(~O; n, tk'~) is given by

A AB(eo; n,tk,.!!) = E(~o) - e ,

* Pigi 1= (1:_ ~+l - t k + ntk E(r» - e • (4.2.1)

However, in the special case of equally spaced time intervals, the

expression for the bias ~ be reduced to a simpler form. Since

.p _ -(i-l)h/e -ih/e _ .-ih/e ( h/e -1) '-12· ki - e . - e - e e , 1-, , •.• ,

and·

gi = (2i-l) h/2 ,

then

., .But,

-t /e* -ih/e _ -h/e· (l-e k )

1: e - e .. . 1 _ e-h/e ' where t k = kh ,

and

(4.2.2)

hIe •e - 1

Page 29: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

•23

Combining these results and substituting in equation (4.2.:H we obtain:

/, -tie /, /,* heh/8(1_e k) -tk/8 h ' -tk/8E, Pigi = - - - tke - ;:; (l-e ).eh(e _ 1 c;

Hence

h/eheh/6 'e -1

-t /et e k

k- , -t J6

l-e ' k

h- '2 " (4.2.4)

as

Thus the bias may be written as

B(§ . n,t ,h) ~ {heh

/e

- Pk+ltk - '~,'~' - t + nt E(!)3 - e •0 ' k ' hie 0-+1 2 k k r. e -1 ~

"Putting 8 = h/e the relative bias in E(eo) m.ay be written

"" B(~O; n,tk,b) I8e8 ,tk 8 ntk,l, 1

R(~O; n,8,k) = e ' = T""' - '\: e - 2' + T E(r)f - 1 •e -1 +1 '

(4.2.6)

Expanding the first t,erm of (4.2.6) as a power series and neglect­

ing terms of 0(84) we obtain:

8,2 t nt

k +, k E(l)12 - ':""\:""';+1;;;";'9 T r •

As 8--> 0, With t k = t fixed, the relative bias becomes

R(e; n,t) = ~ -: + ntE(~) }/e , (4.2.8)

which a.part from changes in notation agrees With the result given by

Page 30: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• Bartholomew [1] for the case of estimating e using a fixed censoring

time and the indiVidual failure times are known.

In particular using approximation (4.1~10), for large n (4.2.8)

reduces to

R(~j n,t) == {-t + nt·nQ,+P } IeI Q. (nQ.{J·

.. Pt_.--r ·nQe

(4.2.10)

and hence asymptotically it is approximated by -

(4.2.11)

r

which is negligible for small h compared with e •

On the other hand, as· 5--> co, with k fixed we see from (4.2.6)

that R(~oj n,5,k) ->R('oj n,oo,k) = (l) •

...4.3 An EXpression for var(~o)

--When the intervals are' equally spaced we ~proceed in a manner

analogous to that adopted in Section 4.2 and obtain 'an~ression forA .

Var(~o) in terms of 8 = hie •

Page 31: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

25

Thus>

Now>

since t = kh > and CL = 1 - P = 1 - e-tk/ek '"'k+1 k+1 . •

Hence (4.3.1) reduces to

Squaring expression (4.2.4) and subtracting from (4.'.2) we obtain: .

* Pig~ * Pi gi2

¥Jeh/e t~Pk+11: - - (1:.Q.. _.. ) = -

- ~+l '""1(+1 ..~e~/e _1)2 ~+1·

Substituting (4.'.3) into (4.l.T) yields

Page 32: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

26

Hence

(4.,.4)

the result for the case when the exact failure times are known and t

fixed, (see e.g. Mendenhall and Lehmann [23J).

. . .' ; .. 1. nPk+l ~+lAs n-.-> oo~ va.r{;);: . Ii"' and hence (4.3.5) becomes:

(n~+l)

2• 1 '. !.§. cosech ~}

n~+l 2 2

whereas (4.3.6) becomes:

/1:: _..nQ (4.;.8)

Page 33: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

The. result in (4.3..7) d:1f~ers from that given by Ebr~nfeld [ 4],

which is for large n

<.

""where 9 t is the m.l. estimator of 9 when the data is grouped at

equal intervals' and censoring is the Same as for §o.

The two results have the same limiting form when 8 --;> 0, but not

when 6 --;> 00, since then Var(~0)-> 0 and var(~') -> 00. The

reason for this apparent con:tradi.ction is presumably because ~0 is in. ·A •

reality a linear approximation to a non-linear estimator 9'. By ad.d-

"-ing extra terms to ~o (Section 4.5) we tend to reduce the bias but

increase the variance. Even though§o has a decreasing variance for

increasing 8 such a situation is hardly reaiistic and a more

pertinent investigation would be to consider the mean square errorA

(m.s.e.), of S.O for small 8.

Denoting the m.s.e. of ~o by D(§O; n,8,k) then

A

D(~o; n,8,k) =9'2

(4.3.10)

Page 34: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

28

From the results "given in Tables. ~"4.2.2) and (4.2.;) we see thatA

for small samples both the bias and variance of" eo are non-monotonic

~d hence so is the m. s .e. As the·' sample size increases the bias and

variance and thus the m.s.e. become monotonic, as would be expected.A

This non-monotonicity property is also exhibited by the m.l.e. e,

for the ungrouped data, and has occurr~d in other research (see e.g.

Lehman .U9], Bartholomew [1J).

4.4 On the Non-Monoto.~cityPropertyA ~

The reason for the non-monotonicity of E(~O) and var(t10 ) is

that they are functions of certain inverse moments of a truncated

binomial"distribution. The restriction that for small samples r > 0,

means that even for large values of Pk+l = p( t > t k ) we 'Will consider

only those cases where there has been at least one failure. Thus forA

n = 1 we Will obtain an estimate whose expected value [E(e01)' S8\Y]

'Will be less than t k• .When n = 2, we now permit one of the variates

to range over the entire real line, or at least that part of it which

occurs in the experiment. Hence

Depending on the various t i (and hence the Pi) this ~ard trend

of E(30 ) presumably continues with increasing n" until the effect of

the law of large numbers becomes dominant and

The initial bias may be negative or positive depending on t k, and k.A

The variance of ~O behaves in an analogous manner.

Page 35: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Ii ' - e <e

i'

1 n 1 (n rlf-r / 1fTable 4.2.1(a). E(iJ == ,1: r'r) Qk+1 k+1' 1- k+1r==l

"~+1 .329680 .393469 .550671 .698806n

1 1 1 1 ,1

2 .90131238 .87754071 .81002551 .731475053 ' .80942789 ' .76641101 .65279861 .539290084 .72507005 ' .66765587 .52804560 ,.4093Q3725 .64861487 .58146167 .43184100 .322569066 .58011211 '.50735368 .35873204 .263654077 .51933488 .44436690 .30331261 .222226688 .46584491 .39126013 ., .21600917 .191922809 .41906207 .34669306 .22828267 .16891432

10 .37832805 .30935466 .20253180 .1508752211 .34295963 .27804279 .,18189569 .1363515812 .31228779 '~2517P301 .16505753 .1244015315 .24246364 .19430063 .12926419 ' .6985578920 .17327547 .13987827 .09511688 .0732581130 .10957792 .08983081 .06234503 .0484322840 .08030070 ~06628375 .04639278 .0361799650 ' .06342971 .05254350 .03694586 .0288766470 .04469338 .03715780 .02625679 .02057236

100 .03098312 .02582377 .01831187 .01437295

.798103~:

1

.66798193

.46377298

.34301829

.26916248

.22099519

.18747295

.16284980

.14398990

.12907109

.11696815

.10694883

.08510359

.06350723

.04213678

.03153020

.02519017

.01796568

.01256187

.864665

1

.61920264

.41580268

.30615197

.241112104

.,19933807

.16983438•1479a451.13113857..li774762.10684446.09779312.077984:72.05831073.03876098.02902991.02320470.01655930.01158349

~

Page 36: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• e ,e

() (1)' (1 ). «1)2 .. :, . (:'1) .' n. 1,' (n\:"Q~ " -n-r/1 Jf' .Table 4.2.1 b. V r =E,~,'- E r'. ".Where E:7: ::: rfi r2"'7:'i:~+1' ·J:."k+l. - k+l

!

n ~1

1

23456789

101112152030405070

100

.329680

.03960453

.06466577

.07802955

.08257731

.08095~4

.07542173

.06773183

.05918153

.05064396

.011265472, .03549806 ..01961121.00714687.00131142.•00045848.00020963.000068112.00002119

.393469

.04623341

.01094299

.01990829

.01853496

.07126243~06134091.05089506,,04114367.03266204 '.02561132.01994749•.00935535.00291504.00060041

...00021121.00010281.00003458.00001121

.•550671

.05889695

.07345688

.06'9741J2

.05~7056

.03684411

.02531248,.01113100.01152503.00781669•.00538923.003797112.00154185.00052036.00012962.00005082.00002491.00000870•00000289

.698806

.06215686

.05708293

.03756936

.0218814a

.01229315

.00698811

.00413267

.00251465

.00:).69320

.00116991

.00084316

.OOP37896

.00014330

.00003858

.00001551

.00000177

.00000275

.00000092

, .798103

.05517306-.03152801.01875935·°°889049

, .00441134.00238622.00141315.00090552.00061653.00043986.000325112

, .00015358.00006018.00001665.00000680.00000341.00000121.00000041.

.864665

.04539210

.02281990

.00923883,,00393120.00190692.00105401.00064485.00042465.00029513.00021368.00015980.00007692.00003062.00000858

, ~OO000352.00000117.00000063

.•00000021

VIo

..-/"

Page 37: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e ,eT

Table 4.2.2. Bias of.e'o - Eq~Spaced Case

8=1000t k

h' "Sample size en)1 2 3 4 5 . 6 7 8 9 10

400 200 -810.0 -488.9 -238.7 -~9.9 87.3 1~.3 244.~ 2eo.7 298.7 30'.~100 -812.5 -491.4 -241.2 -52.4 84.8 179.8 241.7" 278.2 " 296.2 300.9Ungrouped -813.3 -492.2 ':'242.0 -53.1 83.9 179.0 240.9 z/7·4 295.4 300.0

500 250 -765.5 -388.0 -115.9 69.8 188.1 256.5 289.7 299·5 294.6 281.2Ungrouped ~770.7 -393.2 -121.1 64.6 J,.82.•9 251.3 284.5 294.3 289.4. 276.1

800 .400 -639.5 -143.4 ·12~2 250.3 287.9 282.4 2591.1 231.0 204.2 180.8200 -649.4" -153.4 117.3 240.3 277.9 272.5 249.1 221.0 194.2 170.8Ungrouped -652·8 -159.7 113.9 237.0 274.6 269.1 "245.8 227.7 190.9 166.5

1200 600 -487.4 68.1 254.1 277.3 248.0 210~9 179·3 155.1 136~9 123..•1400 -503.9 51.6 237.5 260.7 231·5 194.4 162.8 138.5 120.4 106.6200 -513·9 41.7 227.6 250.8 221.5 184.4 152.8 128.6' 1l0.4 96.6Ungro~ed -517.2 38.3 .224.3 2~7.5 218.2 180.1 149.5 125.3 107.1 93.3

1600 800 --352.0 185.6 274.1 243.3 ~O;I..' 169.6 147.7 132.5 ·121.5 113.2400 -391.5 146.1 234.7 203.9 161.9 130.1 "108.2 93.0 82.0 73'.7200 -401.4 136.1 224.7 193.9 151.9 120.1 98.3 83.1 72·0 63.7Ungro~ed -404.8 132.8 221.4 190.6 148.5 116.8 94.9 79·7 68.7 60.4

2000 1000 -231.2 245.6 263.6 218.0 183.0 160.9 146.5 136.6 129.3 123.8500 ";292.4 "184.4 202.4 156.8 121.8 99.6 85.3 " 75.3 68.1 62.5400 -299·7 177.1 195.1 149.5 114.6 92·3 77.9 68.0 60.8 55·2Ungrouped -313.0 163.8 181.8 136.2 101.2 79.0 64.6 54.7 47.5 41.9

~f-I

Page 38: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e ,-Tah1e 4.2.2 (continued)

8=1000t k h Sa.m;p1e size (n)

11 12 15 20 30 40 50 70 ~1oo 00

1(.00.. 200 299.1 2~9.0 244.8' 176.2 105·9 7U..8 58.6 !+1.1J. 29,•.9- .3.3100 296.6 286.5 242.2 173.7 102.5 72.4 56.1 38.9 26.9 0.8Ungrouped 295.8 285.7 241.5 172.9 101.6 71·5 55.3 38.1 26.0 0

500 250 263.7 244.7 191.7 133.2 81.9 60.1 48.0 35.0 25.7 5.2Ungrouped 258.5 239.5 186.5 128.0 76.7 5#-~O. 42:;;6· 29.~S 20.5 0

800 400 161.2 145.1 111.7 82.4 56.8 45.1 38.4 30.9 25-.5 13·3200 151.2 135.1 101.7 72.4 46.8 35.1 28.4 20.9 15.5 3.3UJ:lgrouped 147.9 131.8 98.4 69.1 43.5 31.8 25.1 17.6 12.2 0

1200 600 112.4 104.0 86.6 70.8 56.2· 49.2 45.2 40.7 37.4 29.8400 95.9 87.5 70.1 54.3 39.6 32.7 28.7 24.2 20.8 13.3200 86.0 77.5 60.2 44.3 29.7 22.7 ..18.7 14.2 10.9 3.3Ungrouped 82.6 74.2 .56.8 41.0 26.4 19.4 15.4 10·9 7.6 0

1600 800 106.7 101.4 90·5 80.2 70.6 66.0 63.2 60.2 57.9 52.8400 67.2 62.0 51.0 40.8 31.1 26.5 23.8 20.7 18.4 13.3200 '57·2 52.0 41.1 30.8 21.1 16.5 13.8 10.7 8.5 3.3Ungrouped 53.9 48.7 37.7 27.5 17.8 13.2 10.5 7.4 5.1 0

-2000 1000 119.4 115.9 108.4 101.3 94.5 91.2 89.3 87.1 85.5 81.9

500 58.2 54.6 47.1 40.0 33.3 30.0 28.1 25.9 24.3 20.6400 50.8 47.3 39.8 32·7 25.9 22.7 -20.7 18.6 17.0 13.3

Ungrouped 37.5 34.0 26.4 19.4 12.6 9.4 7.4 5.3 3·7 0

\}II\)

Page 39: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e #e

Table 4.2.3. Variance of §0 .. equally spaced case

e=1000

t k h Sample size2 3 4 5 6 7 8 9 10

400 200 34270 101132 206934 336730 472068596447 698185 771075 814049100 36518 103150 208742· 338348 473515 597742 699347 772186 814992Ungrou;ped 37269 103825 209346 338888 473998 598175 699735 772469 815307

500 250 59732 ;rn.~:I2 ~~990:? li99781 649165 15~60 ~0'31 858!i.90 821307Ungrou;ped 64287 175389 333368 502805 651798 760567 822368 840289 822913

,-'800 400 181914 448206 695876 836929 862693 807340 711719 606232 508053200 189934 454669 701104 841205 866245 810343 714303· 608492 510058Ungrouped 192629 456840 702861 842641 867438 811352. 715171 609249 510731

1200 600 418268 784211 899309 814298 658992 511431 396673 314218 256246400 430148 792969 905956 819537 663274 515040 399790 316961 258696200 437390 798309 910008 822730 665884 517240 401690 318633 260190Ungrouped 439824 800103 911371 823804 666762 517979' 402329 319195 260692

1600 800 66~562 928132 815338 605835 436799 324988 253919 207477· 175497400 688241 945961 828524 616182 445295 ·332195 260179 213013 180459200 6948;54 950553 831920 618847 447483 334051 261792 214438 181737Ungrouped 697075 952094 833061 619742 448218 334675 262333 214917 182166··

2000 1000 847982 903247 651463 440515 313779 239967 194170 163364 141195500 884317 927646 669428 454741 325476 249933202853 171059 148104400 888945 930754 611716 456546 326966 251202 203959 172039 148984Ungrouped 891136 936254 675766 459~9 ~~96P3 ~53449 205917 J.73774 159542

~

Page 40: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e ,e

Table 4.2.3. (continued)

e=1000

t k h Sam,p1esize1l 12 15 20 30 40 50 70 100

400 200 829191 820967 708404 459115 198569 118165 84479 54083 35175100 830046 821746 709009 459547 198842" 118365. 84637 54194 35253Ungrouped 830331 822006 709211 459691 i98933 118432 84690 54232 35279

500 250 779198 721979 529224 299654 136487 (81902 65099 42935 28436Ungrouped 780641 723285 530233 300380 136953 '88246 65372 43128 28570

800 400 424333 356314 226994 '136869 77058 53820 41371 28295 19194200 426134 '357949 228274 137811 77675 54280 41737 28555 19376Ungrouped 426739 358498 228704 138127 ',77882 ,'54434 41860 28642 19437

\~

1200 600 215084 185080 130898 88572 53990 38853 30348 21107 14483400 217298 i87101 132499 89762 54776 3944130817 21441 ~, 14717'200 218648 188332 133475 90487 55256 39799 3110? 21645 14859Ungrouped 219102 188746 133803 .. 90731 55417 35?919 31199 21713 14907

1600 800 152261 134599 100112 70311 44129 32162 25299 17729 12225400 156757 138711 103383 72753 45749 33374 26268 18419 12708200 151915 139770 104226 73381 46166 33686 26517 18597 12832Ungrouped 158304 140125 104509 73593 ,46306 33791 26601 18657 12874

2000 1000 124J125 111266 (8~557 60456 38538 28289 22346 15739 10900500 130695 117004 89133 63878 40812 29992 23707 16711 11579400 131493 117735 ,89716 64314- '41102 30209 23881 16834, 11666Ungrouped 132907 119029 90748 65085 41615 30593 24188 17054 '11819

\X-t="

'.

Page 41: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Putting

A

4.5 Effect o~ Neglecting Terms in.~l

From (.3.5.8) we ~bserve that

2i§1 = i[80 + 80(1 - E*ni~)] if max hi < V3 ~o -.

. ..... - .31'90

2* nihig=E -, then" .3re"2

,0.

A A $o{~1 =~()- "4"'". g

A C= ~0(1 "'4),

where

35.

Putting s>l

thenT < ssg i'· . 1·.3.5.·· (2s-1) < 1s nce .. . •

. . 2s (s+l)~

Hence an upper bound for the factor. C can be obtained' by rep1ac-

ing th.eterms of C by those of a geometric series which is term by

term greater than those of C.· Thus

equality being attainedorily when' the intervals are equally· spaced.

Page 42: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

36

Hence the correction to §o is less than

which for large sa.JIWles may. be approximated by

6 - F Ihi~147· 362 - max 1h~ ~

hence the percentage error is less than

An i~roved bound on C can be obtained by noting that

Hence the bound on the· correction factor becomes for the equally spaced

case

and thus the percentage error- is less than

2552 (4-52 )4(3-52 ), .

..

Page 43: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

37

However, in general the important term in the bias reduction will

2* nillibe the first, namely 1:: .... The amount of this reduction is given12~o

by

1 * nih~/r= --12 E(1:: ... ). e9

(... * 21) jCOy eo' 1:: n.ll. r, J. J.

When the inte:rvals are, equally spa.ced (4.5.5) reduces to

.... '

E( h~ ) = . h2

... ..1. 1 + v~:eo) 1:: h2

... ' , (4.5.6)12eO" : 12E(eO) [E(eo)]2., 12E(eO)

, ~ ., 2 ,d

which :t'or,la:rg.e n_' __["bea~te~)b~~r:9:' ;. 'tpe p'~ce~t~e

a.pproximation being

The tb:ree a.pproximations to th.e bound are comp8J:'ed in th.e follow-

ing table.

Page 44: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Table 4.5.1. Approximations to the upper bound of the correctionfactor - equally spaced case (as percentage of e)

.05 .10 .20 .25 .40 .50 .60 .80 1.00 1.50 .

APirox. (4.5.3) .02 .08 .34 .53 1.41 '2.27 3.41 6.78 12.5 75.0(4.5.4) .02 .08 .33 .52 1.35 2.13 3.10 5.69 9.37 32.81

II (4.5.7) .02 .08 .33 .52 1.33 2.08 3.00 5.33 8.33 18.75

From the above table it is apparent that for a < 1 almost all of"-

the correction to ~o is a~coUnted for by using the first term of (4.5.:1)

only. It is to be expected that for a > 1 the first term is insuffi-

cient since the series expansion of exp- 8 converges only slowly for

8 > 1.

For the. equally spaced case denoting

then

For e:: 1000 and certain values of n, t k and'h expression (4.5.9)

is tabulated in ,Table 4.5.2, and the results compared with the ungrouped

case. Even for Widely grouped data the addition of the extra, term to

tJ0 is su,fficient to reduce the bias to almost that' of the ungrouped

da.ta.

Page 45: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

39

The effect of the extra ter.m on the variance of the estimator is

derived below.

Since

A

Var(8,0)

[E(eo)]4

and

then

A

-var(~o).... [E(~0)]2

"'" "'" f If- h4

]Var(8 ) :: var(8) 1 + "'" + . "'" . •2 ,0 . . 6[E(8 )]2 l44[E(8 )]4

,0 . _0

Hence the addition of the bias reducing ter.m has an increasing effect

on the variance, the extent of this increase can be seen by comparing

"'"T~bles 4.2.3 and 4.5.3. A feature of the variance of 82 is that it

is an increasing function of 8 and hence is more in line with the

:maximum likelihood estimator (4.3.9). A more realist'ic comparison of. "'"

the estimators would be through their mean square errors, D(80; n,8,k)"'" A '

and D(~2; n,8,k}, where D(~o; n,8,k) is given by (4.3.10) and

"'"D(~2; n,8,k) by

Page 46: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

40

or directly

'"= D(~O; n,8,k)

'" ...From Table 4.5.4 it is evident that for relatively small" ~O' ~2

'"and the m.l.e. for ungrouped data, e, have approximately the same mean

square errors. In other words, no significant in:t'ormation is lost inA

grouping the data.. As 8 ->.:1, the mean square error of ~u tends

to exceed the others, .indicating tnat for fairly coarse grouping theI

addition of the bias correction term not only reduces the bias but

also reduce.sthe mean square error. In general, therefore, it would be

'"preferable to 'Work With ~2 •

Page 47: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e ·e ,e

Table 4.5.2. Approximate bias. of ~2 ... equally spaced case

t k h . .' Sample size' (n)20 30 40 50 10···· 100 00

400 200 172.5 101.5 71 ..4 55.2 38.1 26.1 0100 172.8 101.6 71.5 55.3 38.1 26.0 0Ungrom>ed 172.9 '101.6 71.5 55.3 38.1 26.0 0

.-,.500 250 127.5 76.6 54.8 42.7 29.8 20.5 0Ungrouped ' 128.0 76.7 54.9 42.8 29.8 20.5 0

800 400 68.7 43.3' 31.7 25.1 17.6 12.2 0.1200 ',68.9 43.4 31.7 25.1 17.6 12.2 0Ungrouped 69.1 43.5 31.8 25.1 17.6 12.2 0

1200 600 40.6 26.4 19.6 15.7 Ii.3 8.1 0.7400 40 .. ,6 26.1 19.3 15·4 10.9 7.6 0.22PO .40.8 26.3 19.3 15.4 10.9 7.6 0'lJ'ngrOuped 41.0 26.4 19,.4 15.4 10.9 7.6 0

1600 800 27·9 18.9 14.6 11.9 9·1 6.9 2.;1400 . 27·1 17.6 13.1 -10.5 7.4 5.2 0.1200 27.4 17.7 13·1 10.5 7.4 5.1 0Ungrouped 27·5 17.8 13.2 10.5 7.4 5.1 0

2000 1000 21.9 15.9 13.0 11.4 9.4 8.0 4~9

500 18.8 ' 12.4 9.2 ' 7.4 '5.3 3.7 0.2400 19·0 12.4 9.3 7.4 5.3 3.7 . 0.1Ungrouped 19.4 12.6 9.4 7.4 5.3 3.7 0

Values of .the bias below those of the ungrouped data are due to roundingE!rrors and the approximations used.

~

Page 48: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e -Table 4.5.3.

,.Approximate variance of e.2 ... equally spaced case

9=1000

i;c h S4(f'leSize (n) , .

20 30 o '" .50 70 100

400 200 461330 199668 118848 84982 54416 35397100 460104 199116 118537 84764 5~78 35309.

500 250 302090 137704 ~.·8'81J..9 65718 43354 28n8

800" 400 140002 78909 )55142 112400 29009 19684200 138611 78148 54618 42000 28737. 19501

1200 600 93267 56933 40999 32028 22293 15302400 91928 56136 40433 31598 21990 15096200 91041 55604 40053 31303 21786 14956

.1600 800 76886 48331 35252 27757 19451 13418400 ',14555 46903 ·34224 26940 18894 13036200 73843 46461 33904 26689 18719 "12916

2000 1000 69050 44086 32387 25595 18037 12496500 66363 42420 31183 24651 17379 12044400 65932 42150 30984 24496 17270 11969·

,e

is

Page 49: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e ·e

Table 4.5.4.: , A A

Comparison of the mean square eITors of 80, 82 and the maximum

likelihood estimator (ungrouped) - equaJ.1yspa.ced case!'/

8:::1000

t k h 20S~:Le~~ize (n)" 3·0·_·- . .4Cf~···---- 50 _.- 70" 100

400200

A . . ieo 490161 209594 123760 87913 55797 3~40A. e.2 491086 209970 123946 88029 55867 36078

10080 48971~: 2093~8 123607 87784 55708 35976Ae.2 489964 209438 123650 87~ 55730 35990A

Ungrouped. 8. u _ 489585 gQ~)9_ --..lli5_lt:5._ H.. 81748'55.6B3 35955

500250

"'"90 317396 143195 ' 9;Ji514 67403 44160 29097~

92 318346143572 91722 67541. 44242 29139A

Ung1;'o.!lp.~_ 9, ..31~164 142836 9l?60 67203 44016 28990:~800

400

...90 143659 80284 55854 42845 29249 19845

g2 144722 80784 56147 43030 29319' 19833

19616289914254355512A

90 143052 79865Ae.2 143358 80032 55623 42630 29047 19650

200

~Jli>-ed $ .142902 7977555445 42490 . 28952 19585.

!:IVa.lues of D(~o;n,~,k) below D($; n,5,k) are due to rounding errors.a.nd the

a.pproximationS used.' '

&"

Page 50: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e e

Table 4•.5.4. (continued)9=1000t k h S4?le size (n)

20 30 o . 50 ·-10__ 100...

227641200 90 93585 57148 4~74 32391 15882600 ...

94916 57630 41384 32284 22420 1536892-a 92710 56345 40510 31641 22027 15149400 0a 93577 56817 40805 31812 22109 151542...

92450 5613890 40314 31453 21847 149718200 ...

92 ·92706 56296 .40425 31540 21904 15014--....·92412 ;>6114 40296 31436'Utlgrouped 9 21832 14965

.16QC go 76743 49113 36518 29294 21353 15577800 ."

77664 48688 3546592 27898 19534 13465A90 74417 46716 34076 26834 18848 13046

400#2 75289 47213 34396 27050 18948 13063...

74330 46611 26708 18712 129048; 33958200 ",0

9.2 74593 46775 34075 26800 18773 12942....

74349 46623 33965 2671.1 18712Vngrouped e 12900

·e

t:

Page 51: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

• e

Table 4.5.4. (continued)

9=1000t k h S4?le size (n)

'20 30 o 50 70 100,..

2000 9 ' 10718 41468 36606 30293 23325 182101000 ,,0

69529 44339 32556 1~125 1256092 25725-,..65478 41921 30892 24491 175§2!o 12170

5008.2 - 66716 42574 -31261 24706 17407' 12057-,..e 65383 41773- 30725 24309 17180 11955

400 ,..042304e 66293 31011 24551 17298 11980;2

§ "

Ungrouped 65462 41773 30682 24243 17082 11833

·e

~

Page 52: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

46A _.

4.6 Comparison between e.oand the M.L.E. (Equal.Spacing)

Ehrenfeld [4] shows that for the equally spaced case the maximum

likelihood estimator has the form:

e= -hIn(l _ * r _ )

I: ini + k(n-r)

(4.6.1)

For the same case, since g. = (2i-l) h/2, thenJ. ..

A I:*ini + (n-r)k h .e = ( . ')h - - •.0 r 2

Substituting in (4.6 •.1) we obtain

(4.6.2)

·e

e= -_h=::--__

In(l _ A2h )

2e.O+ h

A

:: e ­o2h

A

6(2e.o+ h)(4.fj.; )

Hence,

A A

If h is relatively smaJ.lthen e.2 and e are almost identical.

Page 53: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

47

CHAPrER 5

OPI'IMAL DECOMPOSITION OF TEE SAMPLE SPACE

5.1 Introduction

The experimenter in fixing the number of time intervals (k) and

the censoring time (tk ) for his experiment would" in some cases prefer

k equal time intervals as a matter of technical convenience. However"

in general" a k-fold decomposition of the interval (O"tk ) which would

:maximize the 'iinformation" provided by the experiment would be more

desirable. The problem" therefore" is to find that decomposition into

k-abutting intervals which is optimal among all admissible decomposi;;"

tions.

Of the ma.ny aVailable criteria upon which to base such a decompo­

sition" a reasonable one would be that which would minimize the variance

"of 90• The intractability ,of this criterion leads us to· consider the

use of the asymptotic variance of the maximum likelihood estimator

(:5.3.3) in its place. Empirically it has been shown (Table 4.2.3) that

for relatively small 5 as n,-;-> 00" var(ao) -> var(G)" thus in the'A

neighbourhood of the minimum of var(9) a small change in the decom,posi-

tion would not greatly alter the variance" i.e. it is suggested that

" ". II Athe optimal decom,position for e would be almost optimal for ~O.

5.2 Determination of the Decomposition

It has been shown (3.4.1) that the information (in the Fisher

sense) intrinsic in the sample is given by

Page 54: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

48

e"

The problem then, is one of finding that decomposition or parti­

tion X = (~, •••'~-l) which maximizes the information I(X) or

equivalently I*(X), where

But f~ = -fi' hence (5.2.3) can be written

(e2) *.I* = f [Xi+lfi +l - xifi _ Xifi - Xi_lfi _l ]

n Xi i fi-fi +l fi_l-fi

" [Xifi .- xi_lfi _l . Xi+lfi+l-xifi . .]. . f -f + f -f· - 2(1-xi ) •

i-l i i i+1

dI* .Setting ~ = 0 (i=l, ••• ,k-l), yields the equations to be solved for

oXi .

the Xi' and hence the t i • The following mathematical ;argwnent is

similar to that adopted by KUlldorf [18] and Walker 1.28] for the case of .

the normal distribution.

Page 55: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

In (5.2.4) we observe that f i > 0, (i=l, ... ,k-l), and that the

second term is negative and non-vanishing. This last point II1S\Y be

demonstrated as follows:

Putting

(s) =(X+Stf~X+S) - xf(x)g, f x - f(x+s) ,

then (a) 11#, g(s) = 1-xs..:.-> 0

(b) g( s) is a decreasing function of s, 0 < s < 00 ,

(c) g(s) ~ -(s+.x-1), 0 < s < 00 •

By application of l'Hepital t s rule we see that

1t g(x) =,1t (x+s )f(x+s) - xf)X)s-> 0 s-> 0 f(x) - f(x+s

=1t -(x+s )f(X+s) + f(x+s)s-> 0 f(x+s)

= 1-x •

If we can show gt(s) < 0 for 0 < s < 00, then we have ,proved (b).

Now

gt(s) = ,f(x+S),' 2 {Xf(X) - (x+s)f(x+s) - (s+.x-1)[f(x) - f(X+S»)) ,[f(x)-f(x+s)] , :

but 'f(x+s) > 0 for all S > 0, hence the sign of g(s)[f(x) - f(x+s»)2

depends on the sign of

h(s) =x rex) - (x+s)f(x+s) - (s+.x-1) [f(x) - f(x+s») •

Since h(O) =0 and

ht(s) = (x+s)f(x+s) - f(x+s) - (s+.x-l)f(x+s) - f(x) + f(x+s)

= f(x+s) .. f(x) < 0 for all s > 0 ,

then h( s) < 0 for all S > 0 and consequently so is, g t ( S ).

Page 56: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

50

Part (c) has been proved in the process of showing h( s) < o.

Putting x = 'xi _l and s = xi-xi _l we then find g(s) becomes

> 1 - x- i

by (c) above.

by (a) and. (b) above.

Thus from (5.2.5) and (5.2.6) we see that

g(s') < l-xi

< g(s) ,

and hence

g(s') - g(s) < 0

Expression (5.2.7) implies that equation (5.2.4) vanishes if, and only

if, the term in the last bracket vanishes, which gives the resulting

system of equations:

Putting

di +l + di - 2ei = 0,

which may be Written

(i=l, ••• ,k-l) ,

Page 57: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

i-l, ()i-lDi = di +l - 2 1: (_l)J ei -

J, + -1. cL = 0 ,

.1=0 -:L

51

(i=l, ••• ,k-l) •

(5.2.10)

The system of equations Di = Di(xl'~' ••• ,xi +l ) = 0 may be solved by

the generalized Newton procedure. Then

*-l?~(m) = ~(m-l) - D(m_l) ~(m-1) ,

where starting 'With a trial solution ~(O)' the mth itera~ion yields

*-1~(m)' 'With D and D each eValuated at ~(m-l)' and

~t = (~,D2' ••• '1\:-1) •

aDl aD1 :

~ d~ :~-----I

aD2 aD2 aD2 ;'~ dX; di3:

I

• •• •• •• •

* • 0

D = • 0

•••

• • • • • • • • • • • • • •

• • 0 • 0 • • • • • • • 0 •

II

\.-- - - -aD

k_2

d~_l

~~

However, the matrix inversion may be simplified if we note from

(5.2.10) that

Page 58: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e.52

j ~ 2 •

adiIn a.ddition, if we put ~ = d , then.oxj ij

j=i

j=i-1

o , j < i-1, or j > i ,

Thus

and

. It should be noted that

i =1, ••• ,k-1 •

AlsoaDi i-1 ·i-1~ = 2( -1) + (-1) d- 1, i ,= 2, ••• ,k-1oX1 ~ '.

and i =3, ••• ,k-1

j = 1, ••• "i-2 •

*Hence if we add each successive column of D' to tha.t preceding it we

Page 59: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

obtain a matrix H of the form:

53

H =

hii~l

~lh41••

'~I 0 •••••••••••••L,.._,

~2 h23 , 0 •••••••••••L __ ,

~2 Ij3 ~41 0 •••••••••,..--- I ~, ,: 0 I h43 h44 h45 :I L_--a II· I

•I •I •I

• ••

• • •

• • •

o

o

o

••• •

• •• I • •

I • •• ,I 0'. •, ---.. L_ - - - -

~-2,1: 0 • • • • • .0. I~-2,k-3 ~-2-k-2 ~-2"k-iJ __ -:- __•

~-l,l :0 • • • • • • • '0 I

~-1,k-2 ~-l,k-lI

The elements of H are given by

ODi obi-_\~

=1" •••"k-ldXj

+ dXj +l =1" ••• ,k-2

hij =cD!,

{~= 1, •••"k-ld '

~-l = k-l

Hence,

i = 2, ••• "k-2

i =k-l

Page 60: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e. " .i=l, .. 0 .,k-2 •

54

ODi ODi ' -fih - + - d = [e d ]i . 1 - "':::':':"""~ - i+1 i f -f· . i- 1+1 ',1- OXi OX1_l ' i i+l

( )i-l ()1-l f l [ ]-1 <L = -1 - e -<L, i=3, 00 o,k-l~l l-fl 1 ~

i=4, 00 o,k-l

j=2,.oo,j-2 •

The number of' elements of the matrix H that need to be calculated

In8\V be reduced by using the following relations':,

i=2

i=3, ••• ,k-2

h.. -h. =2.--k-l,k-l -It-l,k-2

Page 61: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

55

e Thus the matrix H is really of the form:

1 + du d22

0 0 • • • • • • • • • • • • • • 0

2~

~1 1 0 • • • • • • • • • • • • • • 0

d11 d43 1 d44 0 • • • • • • • • -. • • • • 0

-~1 -0 0,4 1 •

H= ~1 0 0 d65 •

• • • •.. • • •• • •

• 0

(-1)k-1du 0 0 • • • • 0 ~-1 k-2 1 ~-1 k';'l

(_:l.)k-2d 0 0 • • • • • • • 0 !\,k-1 2~,k+111

This matrix manipulation may be expressed by the equation

*DA=H,

Where A is a matrix of the form

1 0 • • • • • • • • • • 0I

1 1 0 • • • • • • • • 0

0 1 1 0 • • • • • • 0

• •A • •= •• •

• •• •• •

10 • • • • • • • 0 1 1 0

0 • • • • • • • • • 0 1 1

Since D*-l = Al:I-1 we may obtain D*-l by computing B-1 and

adding successively the (i_1)st row of B-1 to the i th (i~, ... ,k-1).

Page 62: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

56

·The number of iterations may be reduced by a judicious choice of !(Or

Perhaps the simplest approac:p.. which would tend to simplify the imtial

matrix algebra would be to start with equal spacings. Wben this occurs

we have:

Hence

x = i8i

xi-x

i_1

=8

f = e-i8i

i=1" ••• "k •

1 ,

e-(k.-l)8 .. ' [. 8e-k8_1]-(k-1)1) -k5 -{k-1'5-k8 '. + 2e -e e., -e

e

8[5 J=~-r- -1 + 2 =2-~1"e -Ie -1

i=2" ••• ,k-2

i=k-1 •

i=l" ••• "k-2 •

...

hi ,i+1 =.L [1 - :::i] ~. hn-1 ,

.(l.5~~ -~ -/1 [1 ".:~~] =1-2hn' i=2

h =i"i-1

e5

[ I) j~ ...~ -1. = -hr1e -Ie -1

1::=3" ••• "k-1 •

(-ll-l

e5_11=3" ••• "k-1 •

Page 63: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

<.

5-1

From the above we see that starting with equal spacings reduces all of

the non-zero el.ements of the matrix H( 0) to functions of the first

element ~1• The computation of H(0) is consequen~ly a simple

matter. The calculation. of ~(0 ) is similarly simplified since:

i=l" ••• "k

i=l" ..."k-1 •

_ i.-1 j i 1D d 2 't' ( 1) + (-1) - ....d.. •i+1 - 1+1 -j~ - ei _j ~ .. i=l" ••• "k-1

8e8 i+1 i+1 ~ )= ""8 (1+(-1) ] - 8[i+1+(-1) ]-2 1[1-i81~[l-(i-18]e -1 - - --

+•••+(-1)~+1[1-8]1

i odd,

i even.•

t>o

ot4erwise •

5.3 ANumerical..Ex:am:ple

We will il1l.\S_trate the above procedure by considering the optimum

spacings .for a 6-:f'old decomposition of the interval (0,,1200) when

f 1

0

;00 0l\P- l~Of(t)-= t

Page 64: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Connnencing with eql,18.l spacings the initial solution is

!(0) = [.2, .4, .6, .8, 1.0] •

Consequently,

1 2 .2hll ·= 1 + .2- [1 - ,e2 ] = .53329

e -1· e' -1

~2 = ~3 = h44 = 1

58

~5 =2-~1 = 1.46671

hi,i+l = ~l-l = - .46671

. l 1-2~1 =-.06958h = .i,i-1 . -

-~1 = ·~,53329

i = 1, ••• ,k-2

i = 2

i =3, ••• ,k-1

i = 3, ••• ,k-1 •

Bence the matrix BeO) is·

·5333 -.4667 • • •

-.0666 1.0000 -.4667 .. •

H(O) = -.4667 -,5333 1.0000 -.4667 •

,4667 • -.5333 1.0000 -.4667

-.4667 • • -.5333 1.4667

and its inverse

Page 65: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

2.8893 2.0920 1.3943 .7837 .2494

1.1589 2.3905 1.5933 .8955 .2850-1 2.0703 2.6805 3.2147 . 1.8068 .5750H(O) =

.2225 .9199 1.5304 2.0645 .6570

1.0000 1.0000 1.0000 1.0000 1.0000

Since *-1 ·-1 thenD =AH

2.8893 2.0920 1.3943 .7837 .2494

4.0482 4.4825 2.9876 1.6792 .5344*-1 3.2292 5.0710 4.8080 2.7023 .8600D(O) =

2.2928 3.6004 4.7451 3.8713 1.2320

1.2225 1.9199 2.5304 3.0645 1.6570

The elements of B( 0) are given by

59 m_ ... _

D =i

.00666, i = 1,3,5

i = 2,4

hence.00666.00000

'B(o} = .00666 •.00000.00666

Using the ~elation

Page 66: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

tit we obtain

'.

2nd Iteration:

.~alculation of the elements of "~ and B( 1) •••

60

if

'. ;t f""0" "". 1 :--~io •.1;1-.1;1+1 """ J."

1 .1698 .8438 .1562 5.4020 6.0792 .1433 .9174 ".8302

2 .3496 .7050 .1388 5.0792 5.7457 .2465 .7435 .6504-

3 .5408 .5823 .1227 4.7457 5.4167 .3149 .5574 .45924 .7449 .4748 .1075 4.4167 5.0835 .3537 .3609 ".2551

5 .9640 .3814 .0934 4.0835 4.7556 .3677 .1499 .03606 1.2000 .3012 .0802 3.7556 .3614 - .0786

~1 =1 + 5.4020 [.8302 - .9174] = .5290

h22 ° = Il;3 = h44 = 1

~5 = 2 - 4.7556 ~ .0360 + .0786] = 1.4550 •

"

h21 = -5.74~7 [.6504 - .5574] - 5.4020 [.8302 - .9174] = -.0633. .

~3 = - .5290 + .0633 := - .4657 •

Il;2 = -5.4167 [.4592 - .3609] = - .5325

11;4 = -I'· + .5325 = - .4675 •

h43 = -5.0835 [.255i - .1499] = -.5348

h45 =-~.+ .5348 =-.4652 •

Page 67: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

". ~4 =1.4550 - 2 = -.5450

i(. i;hil = (-1) 1 - .5290) ,= (-1) (.4710) •

Also,

61

:01 =~ - 2e1 + c;.

:02 = CJ - 2( e2~el) - c;.:03 = d4 ~ 2( e3-e2+e1) + c;.

:04 = a., - 2(e4-e3+e2-e1) - 'c;.

= .0005

=-.0004,

= .0003

= .0003

.".

Hence

.5290 -.4729

-.0633 1.0000 -.4657

H(I) = -.4710 -.5325 1.0000 -.4675

.4710 • -.5348 1.0000 -.4652

- .4710 . • • - .5450 1.4550.

and its inverse

2.9363 2.1550 1.4394 .8149 .2605

1.1700 2.4107 1.6102 ~9116 .2915·f -1

H(I) = 2.1132 2.7363 3.2619 1.8467 .5904

.2293 .9360 1.5541 2.0908 .6685

1.0364 1.0482 1.0481 1.0470 1.0220

Page 68: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

Using D(l) and proceeding in the s~ way as for the previous

iteration we find after iterating 4 times the solution (to the 4th

significant digit)

~(4) = [.1695, .3492, .5403, .7445, .9636] •

Page 69: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

63 _ n

CHAP.J:IER 6

SUMMARY" CONCLUSIONS AND RECOMMENDATIONS·FOR FURTHER RESEAiwH

This dissertation considers the estimation of the mean life of

i tams for the case of censoring from the right and grouped data when

the mortality follows the exponential law given by

[

1 t

:r( t) =: exp- et ~ 0" e > 0

otherwise •

Censoring occurs at some presta-ted time (tk ) where k is the number

of inspections made in the interval (0" t k ) •

Maximum likelihood estimation is considered and the conditions for

the existence and uniqueness of a- solution examined. Using the notation

Xi = tile and f i = exp- Xi it is found that the likelihood has the

form

k+l(1: E 1:"

i=l

k *and 1: == 1: ) ,i=l

where ni = number of items failing in the interval (ti_l"ti ). If

~ = n or ~+l = n the solutions are 0 and ex> respectively, both of

which are of' no practical value. The method of maximum likelihood has

the, drawback therefore that With positive probabilitythere are two

instances where the sample Will provide little information.· If ~ =t n

and ~+l =t n" the solution to the likelihood equation is unique but

Page 70: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

cannot. be obtained without .iteration. Fisher' s method of scoring is

adopted which gives the (j+l)st iteration as

.......... _ ..... g(e j )ej +l - ej(l - x ). . G(e )

.j

where

and

.....e=e .

.J

,

The problem of a non-explicit solution to the likelihood equation

motivates the search for an tlal.mosttlmaximum likelihood estimator

(m.l.e. ) which can be wri.t.ten in an explicit form.

By defining

hi = t. - t' lJ. J.-

and i = 1, ••• ,k ,

..we may expand the elements of the likelihood equation as power series

giving:

xifi - xi_lfi _l h~. hi 4fi

_l

- ff = ui - (1 + 12e2) + 0(2e)' i = l.t~ •• ,k.

h 4Thus to 0(2~ ) the likelihood equation becomes

2* . * niJii *

1:. ni ui .+ '\:+1~ - 1: 12e2 = r , 1: ni = r •

Page 71: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

The solution to this equation is

where

Thus the initial problem of iteration has been reduced to that of

finding the solution to a quadratic equation.

In general the experimenter will have some idea as to the approxi-

mate dimensionality of e and using this prior information can attempt, hi

to make the ratios 2e' (i = 1, ... ,k), comparatively small. If this,..

is so,· the estimation problem may be reduced still further by using ~o

,..as the estimator. If the intervals are relatively Sma11~o will be

lIalmost" the m.l.e. and at the same time will possess the practical

advantage that it is defined for the case of ~ = n. For the case,..

~ =n, ~0 = gl the mid-point of the ,first time interval, which is a

reasonable and intuitive estimator.,..

The properties of e.o are investigated conditional upon the event

~+1 f n (i.e., r > 0) and it is found that both the bias and variance

are non-monotonic. The reason for this appears to lie in the condition-

ing restriction which means .that both the mean and variance are func-

tions of certain inverse mO!llents of a truncated binomial distribution.

" .The variance of ~o is a decreasing function of the interval width

(equally spaced case), whereas the m.1. e. is an increasing function.,..

The reason for this contradiction appears to be that ~o is essentially,..

a linear estimator whereas the m.1.e. is non-linear. If we adjust ~o

for bias by ~ubtracting a correction term, the variance pattern for the

Page 72: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

66A

new estimator ~2 (equally spaced case)

" "e = e ­.2 .0

is similar to that of the m.l.e. That is to say by a.ddingona~termof

a Taylor series expansion (so that the estimator is no longer linear)

the variance pattern changes to that of the m.l.e. However, since

" "eo' e2 and the m.l.e.'s for both the grouped and ungrouped data are

biased, a comparison of their mean square errors is carried out (Table

4.5.4).~ ~.From Table 4.5.4, it appears· that even for fairly broad group­

ing (of the order of e) there is little loss of information, which means

that the extra cost involved in a continuous sampling case -may be un-

necessary and that periodic inspection would suffice. In other words,

the amount of information per unit cost would be higher for the grouped

data than for a continuous inspection plan where costly timing mechanisms

are required.

The optimal decomposition of the time interval is investigated -

using as the criterion the minimal asymptotic variance. The reason for

this choice is that it leads to a fairly simple series of equations which

may be solved by the generalised Newton procedure. Such a criterion

has the drawback in that the optimal decomposition is a function of the

unknown parameter. However, for tests of hypotheses a decomposition

could be made under the null hypothesis.·-

The use of a sma.J.J.. number of inspection periods leads quite

naturally to other possible fields of research:

Page 73: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

67,.

1. The distributional properties .01' ~O and the power of tests of,.

~othesesusing the distribution of ~O compared with tests based

on other criteria" e.g. , the multiple contingency table approach

is of some importance.

2. Often the test equipment is a matrix of n "test compartments"

which is best operated when ·~h:e~· a:1".'e always full. Thismeans

at each inspection perlod the failures are replaced by new items.

If the items are fairly inexpensive the true saving of this proce-

dure as compared with the non-replacement case would be of interest.

3. This type of estimation procedure can be used for other stopping

criteria and problems. For example it may be applied to the case

when we stop the experiment when at least l' of the items haVe

failed. It would also be useful to apply this to the problem of

mixed failure distributions.

4. A practical application of this estimation procedure is in the field

of factorial life tests" where except in the simplest of cases the

estimation problem is different. Thus in two-factor expe:t"iments

defining

i = 1" ••• "caj = 1" ... "b

where (Xi" ~j correspond to the main effects and· '1ij to the

interaction" .then eiJ may be estimated ..USing the procedures of this

dissertation and applying the restrictions ~ (Xi ~.~ ~j = ~ '1ij =

n '1ij = 1 we obtainj

Page 74: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e• ~.. i = [It e ]lIb / ~

. j .ij .

68

(

A

~ij•

Page 75: ESTIMATION OF THE MEAN LIFE OF THE EXPONENTIAL

e•

..

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It..28. Walker, T. L. 1957. Optimal decomposition of a sa.nq>le space for·

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e--

INSTITUTE OF STATISTICS

NORTH CAROLINA STATlcOtLEGE

(Mimeo Series available for distribution at cost)

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298. Mallios, W. S. Some aspects of linear regression systems. Ph.D. Thesis. November, 1961.

299. Taeuber, R. C. On sampling with replacement: an axiomatic approach. Ph.D. Thesis. November, 1961.

300. Gross, A. J. On the construction of burst error correcting codes. August, 1961.

301. Srivastava, J. N. Contribution to the construction and analysis of designs. August, 1961.

302. Hoeffding, Wassily. The strong laws of large numbers for u-statistics. August, 1961.

303. Roy, S. N. Some recent results in normal multivariate confidence bounds. August, 1961.

304. Roy, S. N. Some remarks on normal multivariate analysis of variance. August, 1961.

305. Smith, W. L. A necessary and sufficient condition for the convergence of the renewal density. August, 1961.

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327. Adams, John W. Autoregressive models and testing of hypotheses associated with these models. June, 1962.