Abstract
The exponential distribution has been widely used in engineering, social and biological sciences. In this paper, we propose a new goodness-of-fit test for fuzzy exponentiality using α-pessimistic value. The test statistics is established based on Kullback-Leibler information. By using Monte Carlo method, we obtain the empirical critical points of the test statistic at four different significant levels. To evaluate the performance of the proposed test, we compare it with four commonly used tests through some simulations. Experimental studies show that the proposed test has higher power than other tests in most cases. In particular, for the uniform and linear failure rate alternatives, our method has the best performance. A real data example is investigated to show the application of our test.
Introduction
The assumption of exponentiality is usually used in many fields due to its two main properties: the constant failure rate property and the memory less property. Many researchers developed different goodness-of-fit tests for exponential distribution against other life distributions (see, for example, Lilliefors [18], Finkelstein and Schafer [7], Ebrahimi et al. [6], Henze and Meintanis [10], Ghosh and Mitra [8], Majumder and Mitra [19]). However, only a few works focus on the goodness-of-fit tests for fuzzy distribution, even for fuzzy normal distribution. Hesamian and Taheri [13] established fuzzy Kolmogorov-Smirnov one sample test based on fuzzy cumulative distribution function and fuzzy empirical distribution function. Later, Grzegorzewski and Szymanowski [9] extended Hesamian and Taheri’s result to two-sided case. Moreover, they also constructed Cramér-von Mises test and Anderson-Darling test in fuzzy environment. Recently, Zendehdel et al. [22] studied several goodness-of-fit tests for fuzzy exponentiality. By using the α-pessimistic value introduced by Peng and Liu [20], they compared several tests and deduced that Cramér-von Mises test and Anderson-Darling test perform well in terms of power in most cases.
To test the goodness-of-fit for normality or exponentiality, many researchers used Kullback-Leibler information to construct the test statistics (Vasicek [21], Ebrahimi et al. [6] and Balakrishnan et al. [2]). As stated in [6], the goodness-of-fit test based on Kullback-Leibler information has larger power than those on Cramér-von Mises test and Anderson-Darling test. The aim of this paper is to construct the goodness-of-fit test for fuzzy exponential distribution using Kullback-Leibler information. In addition, we compare our test in terms of power with four popular tests: Cramér-von Mises test, Anderson-Darling test, Kolmogorov-Smirnov test and Watson test. The new test statistic is very easy to compute. In addition, experimental studies show that the proposed test has higher power than other tests in most cases. In particular, for the uniform and linear failure rate alternatives, the proposed method has the best performance.
The rest of this paper is organized as follows. In Section 2, we recall some basic theories of fuzzy number and fuzzy random variable. In Section 3, we propose the goodness-of-fit test for fuzzy exponentiality based on Kullback-Leibler information. The critical values of the test statistic are obtained by Monte Carlo simulations in this section. Section 4 is devoted to power comparisons between our test and four frequently used tests. A real data example is illustrated in Section 5. In Section 6, we draw some brief conclusions and the code is given in Appendix.
Fuzzy number and fuzzy random variable
In this section, we recall some basic theories of fuzzy number and fuzzy random variable needed in this paper. For more details, see Buckley [4], Klir and Yuan [14], and Lee [17].
Let
Throughout this paper, we use
In the following, we introduce the α-pessimistic value of a fuzzy number, which is crucial to state the definitions of fuzzy random variable and fuzzy exponential variable.
From Peng and Liu [20], the α-pessimistic value

The α-pessimistic value of
In the following, we introduce the definitions of fuzzy random variable and fuzzy exponential variable based on the α-pessimistic value. For more details, we refer the reader to [11–13].
The fuzzy random variables
Now, having these basic theories about the fuzzy exponential variable in hand, we are able to propose the goodness-of-fit test for fuzzy exponentiality.
In this section, we propose the goodness-of-fit test for fuzzy exponentiality based on the Kullback-Leibler information. Moreover, we obtain the critical points of the test statistic by using Monte Carlo simulations.
The test statistic
Let
Ebrahimi et al. [6] used Kullback-Leibler information to test the exponentiality. In the following, we extend this method to fuzzy environment and establish the corresponding test statistic. For any α ∈ [0, 1], we use
Although it is very easy to compute the test statistic KL mn based on Equation (3.2), we are unable to obtain its exact distribution under H0. In the following, we use Monte Carlo simulation to obtain the empirical critical points C mn (γ) for γ = 0.01, 0.025, 0.05 and 0.1. For each n, we generate 10,000 replications. To determine C mn (γ), we use the least conservative window size m which yields the maximum critical value and the maximum power. The least conservative window sizes according to n ≤ 100 are listed in Table 1. For more properties of the least conservative window size, see Ebrahimi et al. [6] and Vasicek [21]. The empirical critical points C mn (γ) are computed by the following five steps:
The least conservative window size m corresponding to the sample size n
The least conservative window size m corresponding to the sample size n
In this step, we generate a sample of triangular fuzzy numbers For i = 1, ⋯ , n and α = 0.01, ⋯ , 1, calculate the α-pessimistic value For each n, choose the least conservative window size m from Table 1. Then, for each α, compute KL
mn
(α) based on Equation (3.1). Compute KL
mn
approximately by
For each m and n, repeat Steps 1-4 10,000 times and determine the lower γ-quantile C
mn
(γ) with γ = 0.01, 0.025, 0.05 and 0.01.
Table 2 gives the critical values C mn (γ) for several sample sizes. It’s easy to see that C mn (γ) increases as the sample size n increases or the significance level γ increases.
Critical values of the KL mn statistic at significance level γ
In this section, to evaluate the performance of our test, we compare it with the following four popular goodness-of-fit tests: Cramér-von Mises type test statistic Anderson-Darling type test statistic Kolmogorov-Smirnov type test statistic Watson type test statistic
We study the the following five alternatives: Weibull distribution W (β, λ), Gamma distribution Ga (β, λ), log-normal distribution LN (υ, σ2), uniform distribution U (0, 1), and linear failure rate distribution LF (β). The above five alternatives have been widely used as alternatives to the exponential distribution by many researchers (e.g. Ebrahimi et al. [6], Henze and Meintanis [10] and Zendehdel et al. [22]). For 1 ≤ i ≤ n, the central value x
i
of
Monte Carlo power estimates of the KL
mn
, CVM, AD, KS and U tests at significance level γ = 0.01, 0.05 with sample size n = 5
Monte Carlo power estimates of the KL mn , CVM, AD, KS and U tests at significance level γ = 0.01, 0.05 with sample size n = 5
Monte Carlo power estimates of the KL mn , CVM, AD, KS and U tests at significance level γ = 0.01, 0.05 with sample size n = 10
Monte Carlo power estimates of the KL mn , CVM, AD, KS and U tests at significance level γ = 0.01, 0.05 with sample size n = 20
Monte Carlo power estimates of the KL mn , CVM, AD, KS and U tests at significance level γ = 0.01, 0.05 with sample size n = 30
In this section, we apply the proposed test to a practical dataset taken from Lawless [16]. This dataset was also studied by Arefi and Taheri [1] and Zendehdel et al. [22]. It consists of the lifetimes (1000 km) of front disk brake pads of 40 cars. Note that, the lifetimes may not be measured accurately since a disk may work perfectly over a period but be braking for some time. Similar to [1, 22], we use fuzzy numbers
The fuzzy data of the lifetimes (in 1000 km)
The fuzzy data of the lifetimes (in 1000 km)
Since n = 40, we choose the least conservative window size m = 6 from Table 1. Then, we obtain that KL mn = 0.4285 based on Equation (3.3), which is less than 0.7932, the empirical critical value for n = 40 at 5% significance level (see Table 2). Hence, we conclude that the null hypothesis H0 is rejected, that is, the fuzzy data we considered do not follow a fuzzy exponential distribution, which is consistent with the result in [22].
The exponential distribution has been widely used in engineering, social and biological sciences. In this paper, we proposed a new goodness-of-fit test for fuzzy exponentiality using the α-pessimistic value introduced by Peng and Liu [20]. The test statistic is established based on Kullback-Leibler information. Although the test statistic KL mn is easy to compute, it’s difficult to get its distribution function. We employ Monte Carlo simulations to compute the empirical critical points of KL mn . For comparison, we select four commonly used goodness-of-fit tests for fuzzy exponentiality: CVM, AD, KS and U test. Simulation results show that KL mn behaves better than CVM, AD, KS and U in most cases. Moreover, for the uniform and linear failure rate alternatives, KL mn test has the best performance. Finally, we illustrate the application of the test we proposed by a lifetime data in Lawless [16].
It is noted that the goodness-of-fit test we proposed can be only used for fuzzy numbers. Therefore, constructing the goodness-of-fit tests for exponentiality for intuitionistic fuzzy data and type 2 fuzzy data is an interesting problem and we will investigate it in the future. Recently, Choi et al. [5] constructed a new goodness-of-fit test for exponentiality based on Kullback-Leibler information, which is more powerful than the test of Ebrahimi et al. [6]. Extending the test of Choi et al. [5] to fuzzy environment is another future research direction.
Footnotes
Acknowledgments
The author would like to thank editor-in-chief and two anonymous referees for their valuable comments and suggestions which lead to improve this paper significantly. The author was supported by the National Natural Science Foundation of China (No. 11801317), the Project of Shandong Provincial Higher Educational Science and Technology Program (No. J17KA163).
Appendix
k<-10000 #repeated times
n<-20 #sample size
m<-4 #window size
alpha=seq(0.01,1,by=0.01)#α
kl<-rep(0,k)
for(s in 1:k)
{ x<-rexp(n,1) #center points
u1<-runif(n,0.15,0.2)
u2<-runif(n,0.15,0.2)
l<-x*u1 # left spread
r<-x*u2 # right spread
KL<-rep(0,100)# KL mn (α)
for(j in 1:100)
{ x_alp<-T_alp<-rep(0,n)
if(alpha[j]< =0.5)x_alp<-x-l*(1-2*alpha[j])
if(alpha[j]>0.5)x_alp<-x-r*(1-2*alpha[j])#alpha-pessimistic value
z<-rep(0,n)
x_alp<-sort(x_alp)
for(i in 1:n)
{if(i-m<1)z[i]<-x_alp[i+m]-x_alp[1]
if(i+m>n)z[i]<-x_alp[n]-x_alp[i-m]
if(i+m< = n&i-m> =1)z[i]<-x_alp[i+m]-x_alp[i-m] }
H<-mean(log(n*z/(2*m)))#H_mn
KL[j]<-exp(H)/exp(log(mean(x))+1)#KL_mn
} kl[s]<-mean(KL) }
quantile(kl,γ)
