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Optimal burn-in time under cumulative free replacement warranty
Won Young Yuna,*, Yang Woo Leea, Luis Ferreirab
aDepartment of Industrial Engineering, Pusan National University, Pusan 609-735, South KoreabSchool of Civil Engineering, Queensland University of Technology, Brisbane, Qld, Australia
Received 25 July 2000; accepted 6 May 2002
Abstract
In this paper, optimal burn-in time to minimize the total mean cost, which is the sum of manufacturing cost with burn-in and cumulative
warranty-related cost, is studied. When the products with cumulative warranty have high failure rate in the early period (infant mortality
period), burn-in procedure is considered to eliminate the early product failures. After burn-in, the posterior product life distribution and the
cumulative warranty-related cost are dependent on burn-in time; long burn-in period decreases the warranty-related cost, but it increases the
manufacturing cost. The paper provides a methodology to obtain the total mean cost under burn-in and cumulative warranty. Properties of
the optimal burn-in time are analyzed here. Numerical examples and sensitivity analysis are used to demonstrate the applicability of the
methodology derived in the paper. q 2002 Elsevier Science Ltd. All rights reserved.
Keywords: Burn-in; Cumulative warranty; Bathtub failure rate; Mean total cost
1. Introduction
Most durable products are sold today with some type of
warranty to protect consumers from unexpected early
product failures. The manufacturer’s warranty-related
costs are becoming a significant portion of production
cost. High product reliability in the early period of the
product life cycle is crucial to reduce warranty-related costs.
In the product life cycle, there are generally three phases
in terms of failure rate. Three phases can be represented by
the bathtub pattern as shown in Fig. 1.
Definition. Let us assume that the product has a bathtub
failure rate, rðtÞ if there exist 0 # t1 # t2 # 1 such that
rðtÞ is
strictly decreasing; for 0 # t # t1;
constant; for t1 # t # t2;
strictly increasing; for t2 # t;
8>><>>:
where t1 and t2 are called the change points of rðtÞ: The time
interval ½0; t1� is called the infant mortality period; the
interval ½t1; t2� where rðtÞ is flat and attains its minimum
value is called the normal operating period or useful period;
the interval ½t2;1� is called the wear-out period.
To reduce damage from early failures, a burn-in
procedure is carried out by operating the products under
electrical or thermal conditions that approximate the
working conditions in field operation before shipment to
customers (e.g. IC chips for large systems, satellites, and
space ships).
Early failures result in a high warranty cost which is
dependant on burn-in period and warranty type. We
consider a special warranty, cumulative free replacement
warranty (cumulative FRW) which is distinguished from
standard warranty policies. Rather than covering each item
separately for a period T, the cumulative warranty covers the
group of items for a total service time of nT.
This paper is related to economic optimization problem
of how long burn-in procedure should be to minimize the
total mean cost. The latter is the sum of the manufacturing
cost with burn-in and the warranty cost under cumulative
warranties. The studies for burn-in testing began with the
advent of transistors in the early 1950s (Kececioglu and Sun
[5], Kuo and Kuo [6], Leemis and Beneke [7], Block and
Savits [2]). Nguyen and Murthy [11] first proposed a model
to determine the optimal burn-in time for products sold with
warranty. They considered two types of warranty policy
(failure-free and rebate policies) and derived the total cost as
the sum of the manufacturing cost and the warranty cost for
repairable and nonrepairable products. Mi [8] considered
the same situation as Nguyen and Murthy [11] by assuming
0951-8320/02/$ - see front matter q 2002 Elsevier Science Ltd. All rights reserved.
PII: S0 95 1 -8 32 0 (0 2) 00 0 49 -2
Reliability Engineering and System Safety 78 (2002) 93–100
www.elsevier.com/locate/ress
* Corresponding author. Tel.: þ82-51-510-2421; fax: þ82-51-512-7603.
E-mail address: [email protected] (W.Y. Yun).
that burn-in procedure continued until the first products
surviving the burn-in period, although they used a different
cost structure. Mi [8] also proved some important proper-
ties, namely that the optimal burn-in time occurs no later
than the first change point of bathtub failure rate. Mi [9]
compared policies with renewable warranties and burn-in.
Monga and Zio [10] studied the reliability-based design of a
series–parallel system considering burn-in, warranty and
maintenance. They assumed that the system life cycle cost
included costs of burn-in, warranty, installation, preventive
maintenance, and minimal repair. They obtained optimal
values of system design, burn-in time, preventive mainten-
ance intervals, and replacement time. Kar and Nachlas [4]
studied warranty and burn-in strategies together in order to
examine the possible benefits of coordinated strategies for
product performance management.
In this paper, a cumulative FRW is considered as follows.
Cumulative FRW [1]. A lot of n items are warranted for a
total (aggregate) period of nT. The n items in the lot are used
one at a time. If the total lifetimes of the whole batch,
Sn , nT, free replacement items are supplied, one at a time,
until the first instant when the total lifetimes of all failed
items plus the service time of the item then in use is at least
nT.
This type of policy is applicable to components of
industrial and commercial equipment bought in lots as
spares and used one at a time as items fail. Example of
possible applications is mechanical components such as
bearings and drill bits. The policy would also be appropriate
for military or commercial airline equipment such as
mechanical or electronic modules in airborne units.
Burn-in procedure [8]. We consider a nonrepairable
product and for given burn-in period b, all the new product
is tested under environment situation similar with field
condition failed product during burn-in period is replaced
with a new one. Burn-in test is continued until the first
product surviving the burn-in period b is obtained.
In addition, we assume that the products have a bathtub
failure pattern. Given cumulative FRW and bathtub failure
rate, we consider optimal burn-in problem.
2. Total mean cost model
In this section, we derive cost parts under burn-in and
cumulative FRW and property of optimal burn-in period is
proved.
Theorem 1. If products are sold with cumulative FRW
without burn-in, the total mean warranty cost is given by
wCFðT ; nÞ ¼ ðc0 þ c4ÞMCFðnTÞ ð1Þ
where
MCFðnTÞ ¼X1j¼0
FðnþjÞðnTÞ
and FðnÞðxÞ is n-fold convolution of FðxÞ with itself.
Proof. See Ref. [1] (p. 248–9).
Nomenclature
FðtÞ failure time cumulative distribution function
f ðtÞ failure time probability density function�FðtÞ survival function ¼ 1 2 FðtÞ
rðtÞ hazard rate function ¼ f ðtÞ= �FðtÞ
b burn-in time
FbðtÞ distribution function of product survived
burn-in period b ¼ ðFðb þ tÞ2 FðbÞÞ= �FðbÞ
T warranty period on individual item
MðtÞ renewal function with interarrival time distri-
bution FðtÞ
MbðtÞ renewal function with interarrival time distri-
bution FbðtÞ
MCFðtÞ expected number of replacement
MCF;bðtÞ expected number of replacement with burn-in
period b
c0 manufacturing cost per item without burn-in
c1 fixed set-up cost of burn-in per item
c2 cost of burn-in per item per unit time
c3 shop replacement cost per failure during burn-
in period, includes the manufacturing cost and
set-up cost
c4 extra replacement cost per failure during the
warranty period
hðbÞ random manufacturing cost incurred until the
first item survives burn-in period
vðbÞ expected manufacturing cost ¼ E½hðbÞ�
kCFðn; bÞwarranty cost for a lot size n, and burn-in
period b
wCFðn; bÞ mean warranty cost ¼ E½kCFðn; bÞ�
CCFðT ; nÞ total mean cost with warranty period T, lot
size n, without burn-in
CCFðT ; n; bÞ total mean cost with warranty period T,
lot size n, and burn-in period b
Fig. 1. Bathtub failure pattern.
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–10094
2.1. Mean burn-in cost
Under given burn-in, let Z be the total burn-in time until
first product survives the burn-in time b, and X1;…;Xn; be
independently and identically distributed lifetimes of the
products with common c.d.f. F. Let also h 2 1 be the
random variable that is the number of shop replacements
until the first product surviving burn-in time is obtained.
Denoting Xbi as XilXi # b; the manufacturing cost
incurred until the first product survives the burn-in time b
is given by [8]
hðbÞ ¼ c0 þ c1 þ c2Z þ c3ðh2 1Þ; ð2Þ
where
Z ¼Xh21
i¼1
Xbi þ b:
E½h2 1� ¼½1 2 �FðbÞ�
�FðbÞ¼
FðbÞ
�FðbÞ: ð3Þ
Product lifetime Xbi has the following distribution:
Pr Xbi , x
n o¼
1 x . b
FðxÞ
FðbÞ0 # x # b
0 otherwise
8>>><>>>:
for i ¼ 1; 2;… ð4Þ
Thus
E Xbi
h i¼
ðb
01 2 Pr Xb
i , xn o� �
dx
¼1
FðbÞ
�bFðbÞ2
ðb
0FðxÞ dx
� �
for i ¼ 1; 2;…
ð5Þ
since h 2 1 is a stopping time with respect to i.i.d. random
variables {Xbi }
E½Z� ¼FðbÞ
�FðbÞ
�1
FðbÞ
�bFðbÞ2
ðb
0FðxÞ dx
� �þ b
¼
ðb
0½1 2 FðxÞ� dx
�FðbÞ: ð6Þ
Therefore, the mean time burn-in cost, vðbÞ; is
vðbÞ ¼ E½hðbÞ� ¼ c0 þ c1 þ c2
ðb
0
�FðtÞ dt
�FðbÞþ c3
FðbÞ
�FðbÞ:ð7Þ
These results (Eqs. (2), (3) and (7)) are identical with those
of Mi [8].
Additionally, by the result of Mi [8], the lifetime of the
product which has survived burn-in time b is Xh 2 b, and is
distributed according to
Pr{Xh 2 b . s} ¼�Fðb þ sÞ
�FðbÞ; ;s $ 0: ð8Þ
2.2. Mean cumulative warranty cost
For a product survived burn-in time b, its distribution
function is
FbðtÞ ¼Fðb þ tÞ2 FðbÞ
�FðbÞ; t $ 0: ð9Þ
Using FbðtÞ and Theorem 1, we can obtain expected
warranty cost with burn-in. Let MbðtÞ be the renewal
function with interarrival time distribution FbðtÞ; and
MCF;bðtÞ be the expected number of replacement under
Cumulative FRW, then
MbðxÞ ¼X1j¼1
FðjÞb ðxÞ; ð10Þ
and
MCF;bðnTÞ ¼ MbðnTÞ2Xn21
j¼1
FðjÞb ðnTÞ: ð11Þ
Let NðT ; n; bÞ be the number of replacement under
cumulative FRW with burn-in procedure and the warranty
cost is given by
kCF;bðT ; nÞ ¼ ðhðbÞ þ c4ÞNðT ; n; bÞ: ð12Þ
The expected warranty cost is given by
wCF;bðT ; nÞ ¼ E½kCF;bðT ; nÞ� ¼ ðvðbÞ þ c4ÞMCF;bðnTÞ: ð13Þ
2.3. Total mean cost
Under burn-in period, b and cumulative FRW, nT, the
total mean cost is given by
CCFðT ; n; bÞ ¼ n £ vðbÞ þ wCF;bðT ; nÞ
¼ n £ vðbÞ þ ðvðbÞ þ c4ÞMCF;bðnTÞ; ð14Þ
and the per-item total mean cost is given by
CUCFðT ; n; bÞ ¼ vðbÞ þ wCF;bðT ; nÞ=n
¼ vðbÞ þ ðvðbÞ þ c4ÞMCF;bðnTÞ=n: ð15Þ
For special case, if burn-in is not executed, the total mean
cost is given by
CCFðT ; nÞ ¼ n £ c0 þ wCFðT ; nÞ
¼ n £ c0 þ ðc0 þ c4ÞMCFðnTÞ; ð16Þ
For a cumulative FRW policy with burn-in period, optimal
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–100 95
burn-in time b p to minimize the total mean cost function,
Eq. (14) occurs no later than first change point t1 in Fig. 1.
Proof. For cumulative FRW, assume that burn-in procedure
is implemented at certain time b0 . t1. Then, from Eq. (14),
the total mean cost is given by
CCFðT ; n; b0Þ ¼ n £ vðb0Þ þ ðvðb0Þ þ c4ÞMCF;b0ðnTÞ;
and if the burn-in time b ¼ t1; the total mean cost is given by
CCFðT ; n; t1Þ ¼ n £ vðt1Þ þ ðvðt1Þ þ c4ÞMCF;t1ðnTÞ:
The failure rates of Fb0ð·Þ and Ft1
ð·Þ are given by
rb0ðtÞ ¼
f ðb0 þ tÞ= �Fðb0Þ
�Fðb0 þ tÞ= �Fðb0Þ¼
f ðb0 þ tÞ
�Fðb0 þ tÞ¼ rðb0 þ tÞ; and rt1
ðtÞ
¼ rðt1 þ tÞ:
Note that F has the bathtub shaped failure rate rðtÞ:
Therefore
�Fb0ðtÞ ¼ exp 2
ðt
0rb0
ðxÞ dx
�¼ exp 2
ðt
0rðb0 þ xÞ dx
�;
and
�Ft1ðtÞ ¼ exp 2
ðt
0rt1ðxÞ dx
�¼ exp 2
ðt
0rðt1 þ xÞ dx
�:
Obviously, �Fb0ðtÞ # �Ft1
ðtÞ; and Fb0ðtÞ $ Ft1
ðtÞ; since rðb0 þ
xÞ $ rðt1 þ xÞ; for b0 ^ t1; for all t $ 0;and n-fold con-
volution functions FðnÞb0; FðnÞ
t1are the same relation as Fb0
; and
Ft1: That is, FðnÞ
b0ðtÞ $ FðnÞ
t1ðtÞ; for n $ 1.
Thus, by using above relation, for all b0 . t1
MCF;b0ðnTÞ ¼
X1j¼n
FðjÞb0ðnTÞ $ MCF;t1
ðnTÞ ¼X1j¼n
FðjÞt1ðnTÞ;
since for all j, FðjÞb0
$ FðjÞt1:
Also, it is easily seen that vðb0Þ $ vðt1Þ; for all b0 . t1.
Therefore, by using the two results, for MCF;bðnTÞ; vðbÞ;
CCFðT ; n; b0Þ $ CCFðT ; n; t1Þ; ;b0 $ t1:
A
3. Numerical examples
In this section, we consider some distribution functions
and optimal burn-in times for each one.
3.1. Mixture of two exponential distributions
First we consider a hyper-exponential distribution of
which the distribution is
FðtÞ ¼ p½1 2 expð2ðl1tÞÞ� þ ð1 2 pÞ½1 2 expð2ðl2tÞÞ�
with 0 # p # 1: ð17Þ
Fig. 2 shows the optimal burn-in time and the related cost
for warranty period T, lot size n ¼ 1;…; 4 when c0 ¼ 126;
c1 ¼ 2; c2 ¼ 0:1; c3 ¼ 130; and c4 ¼ 80: As the lot size n
increases, the optimal burn-in time b p decreases. In this
Fig. 2. Optimal burn-in time and per-item total menu cost for mixture of two exponential distributions with p ¼ 0:2; l1 ¼ 44; l2 ¼ 0:1 when c0 ¼ 126; c1 ¼ 2;
c2 ¼ 0:1; c3 ¼ 130; and c4 ¼ 80:
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–10096
case, when the lot size is 4, no burn-in is the best economical
policy.
3.2. Mixed-Weibull distribution
Consider the following mixed-Weibull distribution:
FðtÞ ¼ p 1 2 exp 2ðt=a1Þb1
� �j kþ ð1 2 pÞ
� 1 2 exp 2ðt=a2Þb2
� �h k
with 0 # p # 1:
ð18Þ
Fig. 3 shows the optimal burn-in time and the related cost
for warranty period T, lot size n ¼ 1;…; 4; and cumulative
FRW, when c0 ¼ 100; c1 ¼ 2; c2 ¼ 0:1; c3 ¼ 102; and c4 ¼
40:
3.3. Weibull-exponential distribution
Chou and Tang [3] introduced the following distribution
to model the failure pattern of product in the burn-in studies.
The failure rate function is given by
rðtÞ ¼bð1=aÞbtb21 0 # t # t1
bð1=aÞbtb211 t1 # t;
8<: ð19Þ
where 0 , b , 1 is the shape parameter, a is the scale
parameter, and t1 is the change-point. Because 0 , b ,
1; the failure rate function is strictly decreasing in the
interval ½0; t1� and stays at a constant level bð1=aÞbtb211 ;
for t1 # t: Fig. 4 shows the optimal burn-in time and
the related cost for warranty period T, lot size n ¼
1;…; 4; and cumulative FRW, when c0 ¼ 126; c1 ¼ 2;
c2 ¼ 0:01; c3 ¼ 127; and c4 ¼ 95: As the lot size n
increases, the optimal burn-in time b p decreases; however,
the difference between no burn-in and optimal burn-in
policy is small in each case.
3.4. Weibull-exponential–Weibull distribution
We use the following distribution to model the bathtub
failure pattern. The failure rate function is given by
rðtÞ ¼
b1ð1=a1Þb1 tb121 0 # t # t1
b1ð1=a1Þb1 t
b1211 t1 # t , t2
b1ð1=a1Þb1 t
b1211 þ b2ð1=a2Þ
b2 ðt 2 t2Þb221 t2 # t
8>><>>:
ð20Þ
where 0 , b1 , 1 and b2 . 1 are the shape parameters, a
is the scale parameter, and t1 and t2 are the change-points.
Fig. 5 shows the optimal burn-in time and the related cost
for warranty period T, lot size n ¼ 1;…; 4; and cumulative
FRW, when c0 ¼ 126; c1 ¼ 2; c2 ¼ 0:01; c3 ¼ 127; and
c4 ¼ 95: As the lot size n increases, the optimal burn-in time
b p decreases.
The optimal burn-in time clearly depends on the model
parameter ci, and the underlying distribution function F.
Thus, we consider a Weibull-exponential–Weibull distri-
bution with a1 ¼ a2 ¼ 12; b1 ¼ 0:55; b2 ¼ 1=0:55; t1 ¼ 2;
t2 ¼ 8 and use a numerical study to investigate how the lot
size, n and the individual warranty period T affect the per-
item total mean cost and the optimal burn-in time. The
effects of the model parameter ci on the optimal burn-in time
are also studied. Table 1 shows the effects of the lot size n
Fig. 3. Optimal burn-in time and per-item total mean cost for mixed-Weibull case with p ¼ 0:1; a1 ¼ 1:2; b1 ¼ 8; a2 ¼ 100; b2 ¼ 30 when c0 ¼ 100; c1 ¼ 2;
c2 ¼ 0:1; c3 ¼ 102; and c4 ¼ 40:
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–100 97
and the individual warranty period T on the per-item total
mean cost and the burn-in time, respectively, for cumulative
FRW.
It can be seen from Table 1 that as the lot size n increases,
the optimal burn-in time b p decreases; this means that if we
sell a large size of products with cumulative FRW, the short
burn-in is economical, and when the individual warranty
period T increases, the optimal burn-in time b p increases;
this result is identical with the known existing results. The
change of the lot size n is more sensible to the change of the
optimal burn-in time b p than that of the individual warranty
period T. The effect of the cost parameter ci is shown in
Fig. 4. Optimal burn-in time and per-item total mean cost for Weibull-exponential case with a ¼ 12; b ¼ 0:55; and t1 ¼ 2 when c0 ¼ 126; c1 ¼ 1; c2 ¼ 0:01;
c3 ¼ 127; and c4 ¼ 95:
Fig. 5. Optimal burn-in time and per-item total mean cost for Weibull-exponential Weibull case with a1 ¼ a2 ¼ 12; b1 ¼ 0:55; b2 ¼ 1=0:55; t1 ¼ 2 and
t2 ¼ 8:
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–10098
Table 2
Optimal burn-in time for Weibull-exponential–Weibull with a1 ¼ a2 ¼ 12; b1 ¼ 0:55; b2 ¼ 1=0:55; t1 ¼ 2; and t2 ¼ 8
T ¼ 8; n ¼ 2;
c0 ¼ 100
c3/c0
c4/c0, 1.00 c4/c0, 1.02
0.5 0.8 1.0 2.0 0.5 0.8 1.0 2.0
c1/c0 0 c2/c0 0 0.0632 0.1415 0.1964 0.4423 0.0562 0.1319 0.1856 0.4297
0.0001 0.0631 0.1413 0.1962 0.4420 0.0562 0.1317 0.1855 0.4294
0.001 0.0624 0.1401 0.1945 0.4393 0.0556 0.1305 0.1839 0.4268
0.01 0.0564 0.1282 0.1793 0.4138 0.0503 0.1195 0.1695 0.4021
0.01 c2/c0 0 0.0656 0.1442 0.1991 0.4444 0.0585 0.1345 0.1883 0.4318
0.0001 0.0655 0.1441 0.1989 0.4441 0.0585 0.1344 0.1881 0.4315
0.001 0.0648 0.1428 0.1973 0.4414 0.0578 0.1332 0.1866 0.4289
0.01 0.0586 0.1307 0.1818 0.4159 0.0523 0.1220 0.1720 0.4042
0.02 c2/c0 0 0.0680 0.1470 0.2018 0.4465 0.0608 0.1372 0.1910 0.4339
0.0001 0.0679 0.1468 0.2016 0.4462 0.0608 0.1370 0.1908 0.4336
0.001 0.0672 0.1455 0.2000 0.4435 0.0601 0.1358 0.1893 0.4310
0.01 0.0608 0.1333 0.1844 0.4179 0.0544 0.1245 0.1746 0.4062
0.05 c2/c0 0 0.0754 0.1552 0.2100 0.4528 0.0679 0.1452 0.1991 0.4402
0.0001 0.0753 0.1550 0.2098 0.4525 0.0678 0.1451 0.1989 0.4399
0.001 0.0745 0.1537 0.2081 0.4498 0.0671 0.1438 0.1972 0.4373
0.01 0.0676 0.1409 0.1920 0.4240 0.0609 0.1319 0.1821 0.4123
c3/c0
1.05, c4/c0 1.10, c4/c0
0.5 0.8 1.0 2.0 0.5 0.8 1.0 2.0
c1/c2 0 c2/c0 0 0.0467 0.1182 0.1702 0.4113 0.0331 0.0975 0.1465 0.3819
0.0001 0.0467 0.1181 0.1701 0.4110 0.0331 0.0974 0.1463 0.3816
0.001 0.0462 0.1170 0.1687 0.4085 0.0328 0.0965 0.1451 0.3793
0.01 0.0418 0.1072 0.1556 0.3850 0.0297 0.0886 0.1340 0.3577
0.01 c2/c0 0 0.0488 0.1208 0.1728 0.4134 0.0349 0.0999 0.1490 0.3840
0.0001 0.0488 0.1207 0.1727 0.4131 0.0349 0.0998 0.1488 0.3837
0.001 0.0483 0.1196 0.1713 0.4106 0.0346 0.0989 0.1476 0.3814
0.01 0.0437 0.1096 0.1580 0.3871 0.0313 0.0908 0.1363 0.3597
0.02 c2/c0 0 0.0510 0.1233 0.1755 0.4155 0.0368 0.1023 0.1514 0.3861
0.0001 0.0509 0.1232 0.1753 0.4152 0.0367 0.1022 0.1513 0.3858
0.001 0.0504 0.1221 0.1739 0.4127 0.0364 0.1013 0.1501 0.3835
0.01 0.0457 0.1120 0.1604 0.3891 0.0330 0.0930 0.1386 0.3617
0.05 c2/c0 0 0.0576 0.1311 0.1833 0.4218 0.0425 0.1095 0.1589 0.3923
0.0001 0.0575 0.1310 0.1832 0.4215 0.0425 0.1094 0.1588 0.3920
0.001 0.0569 0.1298 0.1817 0.4190 0.0421 0.1085 0.1575 0.3897
0.01 0.0516 0.1192 0.1678 0.3952 0.0382 0.0996 0.1456 0.3678
Table 1
Optimal burn-in-time, and per-item total mean cost for Weibull-exponential–Weibull case with a1 ¼ a2 ¼ 12; b1 ¼ 0:55; b2 ¼ 1=0:55; t1 ¼ 2 and t2 ¼ 8
when c0 ¼ 100; c1 ¼ 1; c2 ¼ 0:01; c3 ¼ 102; and c4 ¼ 70
n ¼ 1 n ¼ 2 n ¼ 3 n ¼ 4
b p CUFR b p CUFR b p CUFR b p CUFR
T 1 0.1013 144.7905 0.0000 109.4184 0.0000 103.2515 0.0000 101.7564
2 0.1636 167.1283 0.0000 119.1756 0.0000 107.8769 0.0000 104.0556
4 0.1715 207.7131 0.0124 144.0542 0.0000 124.7433 0.0000 116.0949
6 0.1742 248.2421 0.0650 175.4177 0.0303 152.6116 0.0131 140.8109
8 0.1727 288.8050 0.1080 214.3014 0.0887 189.0428 0.0772 175.7549
10 0.1507 332.7030 0.1276 258.2180 0.1188 231.9296 0.1153 218.3473
12 0.1408 380.1895 0.1330 304.9668 0.1286 278.5800 0.1271 265.1836
W.Y. Yun et al. / Reliability Engineering and System Safety 78 (2002) 93–100 99
Table 2. It can be seen that when the fixed set-up cost c1
increases, the optimal burn-in time b p increases. That is, as
the burn-in set-up cost c1 increases, there is a corresponding
increase in the burn-in cost. Thus the optimal burn-in time
b p is increased until warranty cost reduction is compensated
for. When warranty cost reduction does not cover the burn-
in cost increment, the optimal burn-in time b p decreases.
When the cost of burn-in per item per unit time c2 increases,
the optimal burn-in time b p decreases. When the shop
replacement cost c3 increases, the optimal burn-in time b p
decreases. When the extra replacement cost during the
warranty period c4 increases, the optimal burn-in time b p
increases.
4. Conclusions
In this paper, the cost model, and the determination of
optimal burn-in time to minimize a total mean cost for
product sold under cumulative warranty are studied. When
the products have failure rate with the infant mortality
period, that is, the probability that the product fails in the
early period is greater than that in the useful period, burn-in
procedure must be taken into consideration to reduce
manufacturing cost.
To determine optimal burn-in time, however, we
consider burn-in and warranty costs under cumulative free
replacement warranty. Then for distributions with infant
mortality period, the total mean cost is calculated, and
optimal burn-in time is obtained. Then sensitivity analysis
on cost parameters was analyzed. The main conclusions
from the analysis based on numerical studies with specific
distributions and restricted ranges of cost parameters are as
follows.
For large lot size n, short burn-in time is better and for
very short or very long period, T, short burn-in is better in
respect of total mean cost. For cost parameters, if c1 or c4 are
large, we run burn-in test longerly and if c2 or c3 are large,
we finish burn-in shortly.
Our results will be a good reference to manufacturers for
military products or components when they estimate the
warranty costs and try to find burn-in procedure because
cumulative FRW is usually used in military contracts. For
further research, other warranty policies can be considered
and some cost estimation problems for buyers are also
promising areas.
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