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On the Sampling Distributions of the
Estimated Process Loss Indices with
Asymmetric Tolerances
Y. C. Chang a , W. L. Pearn b & Chien-Wei Wu c a
Department of Industrial Engineering and Management , Ching Yun University , Taiwan
b
Department of Industrial Engineering and Management , National Chiao Tung University , Taiwan
c
Department of Industrial Engineering and Systems Management , Feng Chia University , Taiwan
Published online: 21 Nov 2007.
To cite this article: Y. C. Chang , W. L. Pearn & Chien-Wei Wu (2007) On the Sampling Distributions of the Estimated Process Loss Indices with Asymmetric Tolerances, Communications in Statistics -Simulation and Computation, 36:6, 1153-1170, DOI: 10.1080/03610910701569168
To link to this article: http://dx.doi.org/10.1080/03610910701569168
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ISSN: 0361-0918 print/1532-4141 online DOI: 10.1080/03610910701569168
Distributions and Applications
On the Sampling Distributions of the Estimated
Process Loss Indices with Asymmetric Tolerances
Y. C. CHANG
1, W. L. PEARN
2, AND CHIEN-WEI WU
31Department of Industrial Engineering and Management,
Ching Yun University, Taiwan
2Department of Industrial Engineering and Management,
National Chiao Tung University, Taiwan
3Department of Industrial Engineering and Systems Management,
Feng Chia University, Taiwan
Pearn et al. (2006a) proposed a new generalization of expected loss index Le to handle processes with both symmetric and asymmetric tolerances. Putting the loss in relative terms, a user needs only to specify the target and the distance from the target at which the product would have zero worth to quantify the performance of a process. The expected loss index Le may be expressed as Le= Lot+ Lpe, which
provides an uncontaminated separation between information concerning the process accuracy and the process precision. In order to apply the theory of testing statistical hypothesis to test whether a process is capable or not under normality assumption, in this paper we first derive explicit form for the cumulative distribution function and the probability density function of the natural estimator of the three indices
Lot Lpe, and Le We have proved that the sampling distributions of Lpe and Lotmay be expressed as the chi-square distribution and the normal distribution, respectively. And the distribution of Le can be described in terms of a mixture of the chi-square distribution and the normal distribution. Then, we develop a decision-making rule based on the estimated index Le. Finally, an example of testing Le is also presented
for illustrative purpose.
Keywords Asymmetric tolerances; Decision-making rule; Process capability
indices; Process loss indices; Sampling distributions.
Mathematics Subject Classification Primary 62E15; Secondary 62P30.
1. Introduction
Process capability indices (PCIs), including Cp Ca Cpk Cpm, and Cpmk (see Chan et al., 1988; Kane, 1986; Pearn et al., 1992, 1998), are convenient and powerful tools
Received May 28, 2005; Accepted March 23, 2007
Address correspondence to Y. C. Chang, Department of Industrial Engineering and Management, Ching Yun University, 229 Chien-Hsin Road, Jung-Li 320, Taiwan; E-mail: ycchang@cyu.edu.tw
1153
for measuring performance from many different perspectives. Those indices convey critical information regarding whether a process is capable of reproducing items satisfying customers’ requirement. In recent years, PCIs have received substantial research attention in quality assurance and statistical literatures as well. The use of PCIs in industry did not begin in the United States until the early 1980’s. Soon after, this explosion of use expanded into other industries such as automated, semiconductor, and IC assembly manufacturing industries, to measure product qualities that meet specification. Based on analyzing the PCIs, a production department can trace and improve a poor process so that the quality level can be enhanced and the requirements of the customers can be satisfied. These well-known PCIs have been defined respectively as:
Cp= USL− LSL 6 Ca= 1 − − m d (1) Cpk= min USL− 3 − LSL 3 Cpm= USL− LSL 62+ − T2 (2) Cpmk= min USL− 32+ − T2 − LSL 32+ − T2 (3)
where is the process mean, is the process standard deviation, USL is the upper specification limit, LSL is the lower specification limit, m= USL + LSL/2 is the mid-point of the specification interval, T is the target value, and d= USL − −LSL/2 is half length of the specification interval.
1.1. Loss Measure with Symmetric Tolerances
Johnson (1992) developed the so-called relative expected loss Lefor symmetric case,
which is defined as the ratio of the expected quadratic loss and the square of the half specification width:
Le= − x− T2 d2 dFx= − T d 2 + d 2 (4)
where Fx is the cumulative distribution function (cdf) of the measured characteristic. If we denote the first term − T/d2 by L
ot and the second
term /d2 by L
pe, then Le can be rewritten as Le= Lot+ Lpe. Unfortunately,
the index Le inconsistently measures process capability in many cases, particularly for processes with asymmetric tolerances, and thus reflects process potential and performance inaccurately.
1.2. Loss Measure with Asymmetric Tolerances
To remedy for this, Pearn et al. (2006a) proposed a modification of expected loss index, which referred to as Le, to handle processes with both symmetric and asymmetric tolerances. Regardless of whether the tolerances are symmetric or asymmetric, the new index obtains the minimal value at = T. Additionally, the
half specification width d is substituted by d∗. This generalization of expected loss index may be expressed as follows:
Le = A d∗ 2 + d∗ 2 (5)
where A= max − T · d/Du T− · d/Dl, Du = USL − T Dl= T − LSL, and
d∗= min Du Dl. Note that Le is sensitive to target value T and it obtains larger value when T is away from the mid-point between the upper and the lower specification limits. We denoted A/d∗2 by L
ot /d∗ 2 by L
pe, and hence Le =
Lot+ Lpe. Obviously, if the tolerances are symmetric T = m, then Lpe reduces to the original index Le.
A process is said to have a symmetric tolerance if the target value T is set to be the mid-point of the specification interval (LSL, USL). In general, asymmetric tolerances (T= m) simply reflect that deviations from target are less tolerable in one direction than the other (see Wu and Tang, 1998). Recent research and advances made in this subject are Boyles (1994), Vännman (1997), Jessenberger and Weihs (2000), and the more recent Pearn et al. (2006a,b). Asymmetric tolerances can also arise from a situation where the tolerances are symmetric to begin with, but the process follows a non normal distribution and the data is transformed to achieve approximate normality as shown by Chou et al. (1998).
For statistical inferences problems, in order to develop a successfully decision-making rule based on the estimated index Le to test whether a normally distributed process is capable or not, the cdf of Le is needed. In this article, we first derive explicit forms for the cdf and probability density function (pdf) of the natural estimators of Lot, Lpe, and Le when sampling is drawn from a normal distributed data. Those sampling distribution results greatly simplify the complexity on analyzing the statistical properties of the estimated indices. Then, we develop a reliable decision-making rule based on the estimated index Le, which can be used to test whether the process is capable or not.
2. Contour Plots of L
eWe investigate some effects of the process mean and the process variance 2on L e
when the specification tolerances are symmetric or asymmetric. From the inequality Le ≥ A/d∗2, it is not difficult to show a necessary condition for L
e ≤ C is T−Dd ∗√C d ≤ ≤ T + Dud∗√C d (6)
where C is a constant. If the tolerances are symmetric, the necessary condition for Le ≤ C reduces to
m− d√C≤ ≤ m + d√C (7)
Figures 1 and 2 display the contours of Le in the plane for the symmetric case (LSL, T , USL= 20 30 40 and the asymmetric case (LSL, T, USL = 20 35 40, respectively. Contours are shown for Le = 011 006 005 004, and 0.03 from top to bottom in each plot.
Figure 1. Contours of Le in plane with Le = 011, 0.06, 0.05, 0.04, 0.03 (top to bottom) for symmetric case Du= Dl.
To obtain the estimated value of Le, sample data must be collected, and a great degree of uncertainty may be introduced into capability assessments owing to the sampling errors. The approach by simply looking at the calculated values of the estimated indices and then make a conclusion on whether the given process is capable, is highly unreliable since the sampling errors have been ignored. As the use of the capability indices grows more widespread, users are becoming educated and sensitive to the impact of the estimators and their sampling distributions on constructing confidence intervals and performing hypothesis testing.
Figure 2. Contours of Le in plane with Le = 011, 0.06, 0.05, 0.04, 0.03 (top to bottom) for asymmetric case 3Du= Dl.
3. Sampling Distributions of the Estimated Process Loss Indices
Let X1 X2 Xnbe a random sample of size n from a normally distributed process
N 2with mean and standard deviation . To estimate the generalization L e,
Pearn et al. (2006a) proposed the natural estimator Le, which is defined as:
Le = A d∗ 2 + Sn d∗ 2 (8)
where A= maxX− T · d/DuT− X· d/Dl , the mean is estimated by the sample mean, X=ni=1Xi/n, and the variance 2by S2
n =
n i=1
Xi− X2/n, the maximum likelihood estimator. By letting Lot =A/d∗2 and Lpe= Sn/d∗2,
the relationship Le = Lot+ Lpe may be established.
For the case where the production tolerance is symmetric, Amay be simplified asX − T. Therefore, the estimator Le reduces to Le = n−1d−2·ni=1Xi− T2, the
natural estimator of Le discussed in Johnson (1992). Consequently, we may view
the estimator Le as a direct extension of Le. In the following, we focus on sampling distributions of the estimated process loss indices Lpe Lot, and Le.
In attempt to derive the cdf and pdf of Lpe, Lot, and Le, we first introduce the following notation: (1) B= nd∗2/2; (2) K= nS2 n/ 2which is distributed as 2 n−1;
(3) Z= n1/2X− T/which is distributed as N 1, where = n1/2− T/;
(4) Y = max2 d
uZ−dlZwhere du= d/Du dl= d/Dl.
After some algebraic manipulations, the following expressions Lpe= K/B, Lot = Y/B, and Le = Y + K/B can be established.
3.1. Sampling Distribution of Lpe
Theorem 3.1. Let X1 X2 Xn be a random sample of size n from a normally
distributed process N 2. Then L
pe is distributed as 2/nd∗2 times a chi-square
distribution with n− 1 degrees of freedom. And the pdf and cdf of Lpe can be expressed respectively as: fLpex= nd∗2 2 fK nd∗2 2 x = BfKBx (9) FLpex= FK nd∗2 2 x = FKBx for x >0 (10)
where FK· and fK·, respectively, denote the cdf and the pdf of K, which is distributed as 2
n−1.
Proof. Since Lpe= K/B, the cdf of Lpecan be obtained directly as: FL pex= PL pe≤ x = PK ≤ Bx for x > 0 (11)
Differentiate (11) with respect to x, the pdf of Lpemay be derived.
If the specification tolerance is symmetric (i.e., T = m), then d∗= d and the inconsistency loss index estimator Lpereduces to Lpe. Therefore, the pdf and the cdf of Lpe can be simplified, respectively, as:
fL pex= nd2 2 fK nd2 2 x (12) FL pex= FK nd2 2 x for x > 0 (13)
Let · and · denote the cdf and the pdf of the standardized normal distribution N0 1, respectively. Then we can express the cdf of Z as FZz= z − and the pdf of Z as fZz= z − , respectively. The cdf of Y can be written as:
FYy= PY ≤ y = PY ≤ y Z < 0 + PY ≤ y Z ≥ 0 = P−d−1 √ y≤ Z < 0 + P0 ≤ Z ≤ d−1u √y = d−1 √ y+ + d−1u √y− − 1 for y > 0 (14) Taking the derivative of FYywith respect to y to obtain the pdf of Y as:
fYy= 1 2√y
d−1 d−1 √y+ + du−1d−1u √y− for y > 0 (15) If the tolerance is symmetric, then du= dl= 1, and the corresponding pdf of Y can be simplified as:
fYy= 1 2√y
√y+ + √y− (16)
For symmetric case, since Y = Z2reduces to the non central chi-square distribution
with one degree of freedom and non centrality parameter = n1/2− T/. The pdf
of Y , an alternative form of (16), can be expressed as: fYy= j=0 Pj/2fYjy y >0 (17) where Yj is distributed as 2 1+2j Pj/2= e−/2/2j/j! = PW = j, and W
follows a Poisson distribution with expected value /2, where = 2.
3.2. Sampling Distribution of Lot
Theorem 3.2. Let X1 X2 Xn be a random sample of size n from a normally distributed process N 2. Then the pdf and the cdf of L
ot can be expressed, respectively, as: fL otx= √ B/x 2 d−1 d−1 √Bx+ + d−1u d−1u √Bx− (18) FLotx= d−1√Bx+ + du−1√Bx− − 1 for x > 0 (19)
where · and · are the cdf and the pdf of the standardized normal distribution N0 1, respectively.
Proof. Since Lot = Y/B, the cdf of Lot can be derived easily by (14): FL otx= PL ot ≤ x = PY ≤ Bx = d−1√Bx+ + du−1√Bx− − 1 for x > 0 (20) The pdf of Lot follows by differentiate (20) with respect to x.
If the specification tolerance is symmetric, then Du = Dl= d du = dl= 1, and the off-target loss index estimator Lot reduces to Lot. The pdf and the cdf of Lot therefore can be simplified, respectively, as:
fL otx= √ B/x 2 √Bx+ + √Bx− (21) FL otx= √ Bx+ + √Bx− − 1 for x > 0 (22) 3.3. Sampling Distribution of Le
Theorem 3.3. Let X1 X2 Xn be a random sample of size n from a normally distributed process N 2. Then the pdf and the cdf of L
e can be expressed, respectively, as: fLex= 1 0 B3x/t 2 fKBx1− t ×d−1 d−1 √Bxt+ + du−1du−1√Bxt− dt (23) FL ex= Bx 0 FKBx− y 1 2√y ×d−1 d−1 √y+ + du−1du−1√y− dy for x > 0 (24) where fK· and FK·, respectively, denote the pdf and the cdf of K, which is distributed as 2
n−1.
Proof. Since Le = Y + K/B, the cdf of Le can be expressed as: FLex= PLe ≤ 0x = PY + K ≤ Bx = 0 PK≤ Bx − Y Y = yfYydy = Bx 0
FKBx− yfYydy for x≥ 0 (25)
The last equality is valid since Bx− y ≥ 0 for 0 ≤ y ≤ Bx, and Bx − y < 0 for y > Bx. Thus, FKBx− y = 0 for y > Bx. Using (15) the distribution function FLe(x) can be expressed as (24).
On the other hand, since d dx ux 0 fx tdt = ux 0 xfx tdt+ fx uxu x
(see Varberg and Purcell, 1992) and fLex=
d
dxFLex
we may obtain the pdf of Le as:
fLex=
Bx 0
BfKBx− yfYydy+ BFK0fYBx Note that K is distributed as 2
n−1, so FK0= 0. By changing variable t = y/Bx in
the above integral, we have y= Bxt and dy = Bx dt. Hence,
fL ex=
1 0
B2xfKBx1− tfYBxtdt
Using (15) the pdf fLexcan be expressed as (23).
For the case when the specification tolerance is symmetric, then Du = Dl= d,
du= dl= 1, and estimator of the expected loss index Le reduces to Le. The pdf (23) and the cdf (24) of Le reduce to those of Le. Hence, the cdf and the pdf of Le can be expressed, respectively, as:
fL ex= 1 0 B3x/t 2 fKBx1− t √Bxt+ + √Bxt− dt (26) FL ex= Bx 0 FKBx− y 1 2√y √y+ + √y− dy for x > 0 (27)
Furthermore, for symmetric tolerances since Y follows a non central chi-square distribution with one degree of freedom and non centrality parameter , we can substitute the pdf of Y as expressed in (17) into (25). Hence, the cdf of Le can be expressed in an alternative form as:
FL ex= j=0 Pj/2 Bx 0 FKBx− yfY jydy for x > 0 (28) where Yj is distributed as 2 1+2j, = 2, and Pj/2= e−/2/2j/j!.
Taking the derivative of FL
ex in (28) with respect to x to obtain the pdf of
Le as: fL ex= j=0 Pj/2 Bx 0 BfKBx− yfY jydy for x > 0 (29)
Now by changing variable t= y/Bx in the above integral, we have y = Bxt and dy= Bxdt. Hence, the result follows:
fL ex= j=0 Pj/2 1 0 B2xfKBx1− tfY jBxtdt for x > 0 (30) Since fKBx1− t = 2 −n−1/2 n− 1/2Bx1− t n−3/2e−Bx1−t/2 fYjBxt= 2 −2j+1/2 2j+ 1/2Bxt 2j−1/2e−Bxt/2 we have fL ex= 2−n/2Bn/2xn/2−1 n− 1/2 j=0 Pj 2 e−Bx/2Bx/2j 2j+ 1/2 1 0 t2j+1/2−11− tn−1/2−1dt = B/2n/2xn/2−1 n− 1/2 j=0 Pj 2 Pj Bx 2 j+ 1 2j+ 1/2 2j+ 1/2n − 1/2 2j+ n/2 = B/2n/2xn/2−1 j=0 Pj 2 Pj Bx 2 j+ 1 2j+ n/2 for x > 0 (31) where Pj/2= e−/2/2j/j!
Figure 3. The pdf of Le with a= −1, b = 3, and n = 10 30 50 100 300 (bottom to top in plot) for 3Du= Dl.
Figure 4. The pdf of Le with a= −05 b = 3, and n = 10 30 50 100 300 (bottom to top in plot) for 3Du= Dl.
Figure 5. The pdf of Le with a= 05 b = 3, and n = 10 30 50 100 300 (bottom to top in
plot) for 3Du= Dl.
Figure 6. The pdf of Le with a= 1 b = 3, and n = 10 30 50 100 300 (bottom to top in
plot) for 3Du= Dl.
4. Distribution Plots of
L
eWe plot the pdf of Le when the underlying process is normal for several selected cases. Figures 3–6 depict the plots of the pdf of Le for four levels of Le index value with parameter a set to a= − T/ = −10 Le = 016 a= −05Le = 012 a= 05Le = 022, and a= 10Le = 056, respectively. The asymmetric case is considered by setting 3USL− T = T − LSL b = d∗/= 3, and sample size n = 10, 30, 50, 100, and 300 from bottom to top in each figure.
From Figures 3–6, we discover that as the value of Le increases, the spread of the distribution also increases. For small sample size n= 10 as example, the distributions are skew to the right (have positive skewness) and have large spread. As sample size n increases, the spread decreases and so does the skewness. We also observe that Le is approximately unbiased and bell-shaped for sample size n greater than 50.
5. A Decision-Making Rule for Testing L
eUnder normality assumption, we proved that the cdf and the pdf of Le can be represented in terms of a mixture of the central chi-square distribution and the normal distribution. Using the index Le, the engineers can assess the process performance and monitor the manufacturing processes on routine basis. To obtain an effective decision-making rule, we consider a testing hypothesis with the null hypothesis and the alternative hypothesis, respectively, as
H0 Le ≥ C (incapable) versus H1 Le < C (capable)
The null hypothesis H0 will be rejected if Le < c, where the constant c, called
the critical value, is determined so that the significance level of the test is , i.e., PLe< c Le = C= . The decision-making rule to be used is then stated as follows: for given (the probability of wrongly reject null hypothesis when it is true) and sample size n, the process will be considered capable if Le < c and incapable if Le ≥ c.
We note that, by setting a= − T/ and b = d∗/, the indices Lot and Lpe can be rewritten as Lot= dla/b2 for a < 0, L
pe= dua/b2 for a > 0, and Lpe=
1/b2, where d
u = d/Du dl= d/Dl . Hence, the value of Le = Lot+ Lpe can be
calculated when values of a, b, du, and dlare given. For example, if a b du dl= 1 3 2/3 2 then Le = 2 × 1/32+ 1/32= 5/9 If L e = C, from Le = Lot+ Lpe, we have C= da 2 b2 + 1 b2 for a≤ 0 and C = dua2 b2 + 1 b2 for a > 0 then b2=d a2+ 1 /C for a≤ 0 and b2=d ua2+ 1 /C for a > 0. In addition, we have B= nd∗2/2= nb2. Therefore, if L e = C, then
B= nda2+ 1/C for a≤ 0 and B = ndua2+ 1/C for a > 0 (32) Furthermore, we have the equality = n1/2− T/ = n1/2a. From the result
of Theorem 3.3, we can use the central chi-square distribution and the normal distribution to find the critical value c satisfying PLe < c Le = C= , i.e., FLec= given L e = C, or equivalent to Bc 0 FKBc− y 1 2√y d−1d−1 √y+√na+ du−1du−1√y−√nady= (33) where B is given in (32).
We note that the distribution characteristic parameter a= − T/ in (33) is usually unknown, which has to be estimated in real applications, naturally by substituting and 2by the sample mean X and the maximum likelihood estimator
S2 n=
n i=1
Xi− X2/n. To realize the relationship between c and a, we examine
the behavior of cagainst a= −3(0.05)3, which covers a wide range of applications with process capability analysis. The results indicate that the critical value reaches its minimum at a= 05 in all cases with accuracy up to 10−3. Figures 7–10 plot the curves of c vs. a for some selected cases.
5.1. Making Decision by Critical Value
Tables 1–2 display the critical values cfor 3Du= Dl, 3Du= 2Dl, respectively, with C= 005, sample size n = 100, a = −3(0.2)3, and = 001, 0.05, 0.10. To test if the process meets the capability requirement, we first determine the value of C and , then estimate the index Le and parameter a from the collected sample. If the calculated value of Le is smaller than the critical value c Le < c
, then we conclude that the process meets the capability requirementLe < C. Otherwise, we do not have sufficient information to conclude whether the process meets the preset capability requirement. In this case, we would believe that Le ≥ C (the process is incapable).
Figure 7. Plots of cvs. a for Le = 011, 3Du= Dl, n= 25 50 75 100 300 (bottom to top
in plot).
Figure 8. Plots of cvs. a for Le = 005, 3Du= Dl, n= 25 50 75 100 300 (bottom to top in plot).
Figure 9. Plots of c vs. a for Le = 011, 3Du= 2Dl, n= 25 50 75 100 300 (bottom to
top in plot).
Figure 10. Plots of c vs. a for Le = 005, 3Du= 2Dl, n= 25 50 75 100 300 (bottom to top in plot).
Table 1
Critical values cfor C= 005 with n = 100, a= −3(0.2)3, and = 001 005 010 under 3Du= Dl a = 001 = 005 = 010 −3.0 0.0431 0.0450 0.0461 −2.8 0.0427 0.0447 0.0458 −2.6 0.0423 0.0444 0.0456 −2.4 0.0418 0.0441 0.0453 −2.2 0.0413 0.0437 0.0450 −2.0 0.0408 0.0433 0.0447 −1.8 0.0402 0.0428 0.0443 −1.6 0.0395 0.0423 0.0439 −1.4 0.0388 0.0418 0.0435 −1.2 0.0380 0.0412 0.0430 −1.0 0.0373 0.0406 0.0425 −0.8 0.0365 0.0401 0.0420 −0.6 0.0358 0.0395 0.0416 −0.4 0.0353 0.0391 0.0412 −0.2 0.0349 0.0388 0.0410 0.0 0.0352 0.0392 0.0414 0.2 0.0334 0.0376 0.0400 0.4 0.0304 0.0351 0.0379 0.6 0.0300 0.0350 0.0379 0.8 0.0313 0.0362 0.0389 1.0 0.0331 0.0376 0.0401 1.2 0.0348 0.0389 0.0412 1.4 0.0363 0.0400 0.0421 1.6 0.0375 0.0410 0.0429 1.8 0.0386 0.0418 0.0435 2.0 0.0396 0.0425 0.0441 2.2 0.0404 0.0431 0.0445 2.4 0.0411 0.0436 0.0449 2.6 0.0417 0.0440 0.0453 2.8 0.0422 0.0444 0.0456 3.0 0.0427 0.0447 0.0459
5.2. Making Decision by p-value
We also can calculate the p-value, i.e., the probability that Le does not exceed the observed index given the values of C, du, dl, a, and sample size n, and then compare
this probability with the significance level . If the estimated index value is l0, then
the p-value can be calculated as:
p-value = Bl0 0 FKBl0− y 1 2√y d−1 d−1 √y+√na+ d−1u d−1u √y−√nady (34)
Table 2
Critical values c for C= 005 with n = 100 a = −3023, and = 001 005 010 under 3Du = 2Dl a = 001 = 005 = 010 −3.0 0.0431 0.0450 0.0461 −2.8 0.0427 0.0447 0.0458 −2.6 0.0423 0.0444 0.0456 −2.4 0.0418 0.0441 0.0453 −2.2 0.0413 0.0437 0.0450 −2.0 0.0407 0.0433 0.0447 −1.8 0.0401 0.0428 0.0443 −1.6 0.0394 0.0423 0.0439 −1.4 0.0387 0.0418 0.0435 −1.2 0.0379 0.0412 0.0430 −1.0 0.0372 0.0406 0.0425 −0.8 0.0364 0.0400 0.0420 −0.6 0.0358 0.0395 0.0416 −0.4 0.0353 0.0391 0.0413 −0.2 0.0350 0.0389 0.0411 0.0 0.0350 0.0390 0.0412 0.2 0.0349 0.0389 0.0411 0.4 0.0344 0.0385 0.0408 0.6 0.0344 0.0385 0.0408 0.8 0.0349 0.0389 0.0411 1.0 0.0357 0.0395 0.0417 1.2 0.0367 0.0403 0.0423 1.4 0.0377 0.0410 0.0429 1.6 0.0386 0.0417 0.0435 1.8 0.0394 0.0423 0.0439 2.0 0.0402 0.0429 0.0444 2.2 0.0408 0.0434 0.0448 2.4 0.0415 0.0438 0.0451 2.6 0.0420 0.0442 0.0454 2.8 0.0424 0.0446 0.0457 3.0 0.0429 0.0449 0.0460
where B is given in (32). The numerical calculations can be easily carried out using the computer software, to integrate the function based on the chi-square distribution and the normal distribution. If the p-value is smaller than , then we conclude that the process meets the capability requirement.
5.3. An Example of Testing Le
Due to low-power consumption, high reliability, and high brightness, Light Emitting Diode (LED) lamps have many applications in traffic signals, full-color displays, etc. As an illustrative example, we consider an LED manufacturing process. Suppose a customer has told his LED supplier that, in order to quality for business with his
company, the supplier must demonstrate that his process capability Le is less than 0.05. This problem may be formulated as a hypothesis-testing problem:
H0 Le ≥ 005 (incapable) versus H1 Le <005 (capable)
In statistical hypothesis testing, rejection of H0 is always a strong conclusion. The supplier would like to reject H0, thereby demonstrating that his process is capable. Moreover, he wants to be sure that if the process capability is below 0.05 there will be a high probability of judging the process capable (say, 0.95).
With a focus on the critical characteristic, the luminous intensity of LED sources, we examine a particular LED product model to test whether the production process of LED is capable or not. Historical data based on routine process monitoring shows that the process is under statistical control and the process distribution is shown to be fairly close to the normal distribution. The upper and the lower specification limits of luminous intensity are set to USL= 40 mcd, LSL = 20 mcd, and the target value is set to T = 35 mcd. Some calculations are made to obtain d= 10, Du= 5 Dl= 15, d∗= 5 du= 2 dl = 2/3. A random sample of
size n= 100 is taken, and calculated statistics are X = 3525 Sn= 03125, A= 05, ˆa = 08, and Le = 00325 Using Table 1 based on n = 100, we obtain c= 00362 Since the calculated Le ≤ 00362, we may claim that the process is capable at the significant level = 005.
Alternatively, we obtain the p-value = 0.015 via (34). We would conclude that the process meets the capability requirement if is set to be larger than 0.015. Otherwise, we do not have sufficient information to make a conclusion. We note that in the illustrative example, the estimated off-target loss index Lot = 002 which occupies 61.5% of Le value, and the estimated inconsistency loss index Lpe= 00125 which occupies 38.5% of Le value. Obviously, it can be seen that the variability is contributed mainly by the process departure in this case.
6. Conclusions
Pearn et al. (2006a) introduced a new generalization of expected loss index Le to handle processes with both symmetric and asymmetric tolerances. The relative expected loss Le = Lot+ Lpe, which provides an uncontaminated separation between information concerning the relative inconsistency loss Lpe and the relative off-target loss Lot. In this article, we considered the three indices, and derive the sampling distributions of their natural estimators under normality assumption. In addition, the theory of testing statistical hypothesis was used to determine whether a process is capable or not. For illustrative purpose, we demonstrated the use of derived results by presenting a case study on LED manufacturing process, to evaluate the process performance.
Acknowledgments
The authors are grateful to the anonymous referees, the Associate Editor, and the Editor for their insightful comments and suggestions, which substantially improve the presentation of this article. The research of Dr. Y. C. Chang was supported by the National Science Council of Republic of China (Grant No. NSC 95-2221-E-231-024).
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