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Article

Extropy and Some of Its More Recent Related Measures for Concomitants of K-Record Values in an Extended FGM Family

by
Mohamed A. Abd Elgawad
1,2,*,
Haroon M. Barakat
3,
Metwally A. Alawady
3,
Doaa A. Abd El-Rahman
4,
Islam A. Husseiny
3,
Atef F. Hashem
1,5 and
Naif Alotaibi
1
1
Department of Mathematics and Statistics, Faculty of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), Riyadh 11432, Saudi Arabia
2
Department of Mathematics, Faculty of Science, Benha University, Benha 13518, Egypt
3
Department of Mathematics, Faculty of Science, Zagazig University, Zagazig 44519, Egypt
4
Department of Basic Science, Faculty of Computers and Informatics, Suez Canal University, Ismailia 41522, Egypt
5
Mathematics and Computer Science Department, Faculty of Science, Beni-Suef University, Beni-Suef 62511, Egypt
*
Author to whom correspondence should be addressed.
Mathematics 2023, 11(24), 4934; https://doi.org/10.3390/math11244934
Submission received: 27 October 2023 / Revised: 24 November 2023 / Accepted: 10 December 2023 / Published: 12 December 2023
(This article belongs to the Special Issue Probability, Statistics & Symmetry)

Abstract

:
This study uses an effective, recently extended Farlie–Gumbel–Morgenstern (EFGM) family to derive the distribution of concomitants of K-record upper values (CKRV). For this CKRV, the negative cumulative residual extropy (NCREX), weighted NCREX (WNCREX), negative cumulative extropy (NCEX), and weighted NCEX (WNCEX) are theoretically and numerically examined. This study presents several beautiful symmetrical and asymmetric relationships that these inaccuracy measurements satisfy. Additionally, empirical estimations are provided for these measures, and their visualizations enable users to verify their accuracy.

1. Introduction

One of the most fundamental techniques in stochastic multivariate analysis is the concept of a family of multivariate distributions. Families of bivariate distributions with known marginals have drawn attention for many years. The Farlie–Gumbel–Morgenstern (FGM) family is regarded as one of the world’s first bivariate distribution families. When the FGM family turns into a copula (i.e., when the marginals are uniform), the correlation coefficient between the FGM family’s marginals reaches its minimum value of −0.33 and highest value of 0.33. The FGM distribution is, therefore, best suited for data with low correlation coefficients. Despite this constraining restriction, the FGM family has increasingly replaced conventional multivariate normal models in various applications and is now extensively used in several different fields. In a study by Ghosh et al. [1], the FGM family was applied to model the interdependence between environmental and biological variables. In another study by Shrahili and Alotaibi [2], variants of this copula were employed to simulate real-world datasets with symmetric characteristics.
Numerous modifications to the FGM copula that have been discussed in the literature aim to improve the correlation between the inner marginals. Ebaid et al. [3] presented the symmetric generalization of the FGM copula, and Barakat et al. [4] have since considered it. They discovered that the admissible range and correlation claims made by Ebaid et al. [3] were false. Barakat et al. [4] revised the copula’s allowable range. The symbol for this extension is EFGM, and it has a more straightforward function than many known generalizations of the FGM family, such as Bairamov–Kotz–Becki–FGM, Huang–Kotz FGM (see [5,6]), and iterated FGM (see Barakat and Husseiny, [7]). Recently, Abd Elgawad et al. [8] revealed and discussed some distributional traits of concomitants of order statistics (OSs) arising from the EFGM family. The work by Abd Elgawad et al. [8] is expanded upon in this research to include K record values in the perspective of some recent information measures. The cumulative distribution function (CDF) and probability density function (PDF) of the EFGM family, denoted by EFGM ( c , d ) , are given, respectively, by (cf. [4])
H T , W ( t , w ) = H T ( t ) H W ( w ) 1 + c H ¯ T ( t ) H ¯ W ( w ) ( 1 + d H T ( t ) ) ( 1 + d H W ( w ) )
and
h T , W ( t , w ) = h T ( t ) h W ( w ) 1 + c 1 + 2 d 1 H T ( t ) 3 d H T 2 ( t ) 1 + 2 d 1 H W ( w ) 3 d H W 2 ( w ) ,
where the marginals H T ( t ) and H W ( w ) are continuous, and H ¯ X ( . ) = 1 H X ( . ) . Barakat et al. [4] clarified that the natural parameter space Λ (the admissible set of parameters c and d that ensure H T , W ( t , w ) is a bonafide CDF) is convex. The set Λ is given by Λ = Λ + Λ , where
Λ + = ( c , d ) : 0 d 1 , 1 ( 1 + d ) 2 c 1 ( 1 + d ) ; or d > 1 , 1 ( 1 + d ) 2 c 1 ( 1 + d ) 2 , Λ = ( c , d ) : 2 d 0 , 1 c 0 ; or d < 2 , 1 ( 1 + d ) 2 c 1 ( 1 + d ) 2 .
Let { T i , i 1 } be a set of independent random variables (RVs) with the same continuous CDF H T ( . ) and PDF h T ( . ) . The observation T j is called an upper record value when T j > T i for every i < j . A similar definition can be given for lower record values. Due to the rarity of upper record values, which restricts their use in various applications, we can switch to a more flexible model, which is K record upper values (KRVs), where we can always expect the occurrence of KRVs more frequently than upper record values. Considering the KRV model, refer to Dziubdziela and Kopociński [9]. For a fixed K 1 , the PDF of the Nth KRV is given by
g T N , k ( t ) = K N Γ ( N ) ln H ¯ T ( t ) N 1 H ¯ T K 1 ( t ) h T ( t ) , N 1 ,
where Γ ( . ) is the gamma function. For more details about this model and its applications, refer to [10,11,12,13].
Let a random bivariate sample ( T i , W i ) , i = 1 , 2 , , have a common continuous CDF H T , W ( t , w ) = P ( T t , W w ) . When the investigator is just interested in studying the sequence of K records, T N , K , of the first component T , the second component associated with the KRV of the first one is termed as the concomitant of that KRV, denoted by W [ N , K ] . Several papers, including [14,15,16,17], discussed the PDF of CKRV W [ N , K ] . This concomitant’s PDF is provided by
h [ N , K ] ( w ) = h W | T ( w | t ) g T N , K ( t ) d t ,
where h W | T ( w | t ) is the conditional PDF of W, given T.
The extropy (EX) was proposed by Lad et al. [18]. Earlier in academic literature, EX was used to contrast with entropy. The EX refers to an organism’s intelligence, functional order, vitality, energy, life, experience, and capacity for growth and improvement. The EX of an RV T with PDF h T ( t ) is defined as (see [18,19])
E X ( T ) = 1 2 0 h T 2 ( t ) d t = 1 2 0 1 h T ( H T 1 ( u ) ) d u 0 .
Qiu [20] reviewed several characterizations, as well as the EX-lower bounds for OSs and record values. Qiu and Jia [21] examined residual EX using OSs. Irshad et al. [22] refined the concept of past EX for concomitants of OSs from the FGM family. In addition, they studied the cumulative past EX and dynamic cumulative past EX for the concomitant of rth OS. There have been many studies of EX measures in conjunction with generalized OSs, such as Almaspoor et al. [23], Husseiny and Syam [24], and Husseiny et al. [25]. Additionally, Jahanshahi et al. [26] proposed a measure of uncertainty for RVs, known as cumulative residual extropy, abbreviated by CREX, which is given by
C R E X ( T ) = 1 2 0 H ¯ T 2 ( t ) d t = 1 2 0 1 ( 1 u ) 2 h T ( H T 1 ( u ) ) d u ,
which is always negative. Consequently, the negative CREX (NCREX) shall be
ζ R ( T ) = 1 2 0 H ¯ T 2 ( t ) d t = 1 2 0 1 ( 1 u ) 2 h T ( H T 1 ( u ) ) d u .
Recently, Hashempour et al. [27] proposed a new information measure called weighted CREX (WCREX), which assigns more importance to large values of the considered RV, as well as EX and CREX; this measure is permanently negative and is defined by
C R E X w ( T ) = 1 2 0 t H ¯ T 2 ( t ) d t = 1 2 0 1 H T 1 ( u ) ( 1 u ) 2 h T ( H T 1 ( u ) ) d u .
Thus, the positive one would be called weighted negative cumulative residual extropy (WNCREX) and is expressed as
ζ R w ( T ) = 1 2 0 t H ¯ T 2 ( t ) d t = 1 2 0 1 H T 1 ( u ) ( 1 u ) 2 h T ( H T 1 ( u ) ) d u .
Also, a negative cumulative extropy (NCEX) has been introduced, similar to (7), by Tahmasebi and Toomaj [28]; that is,
ζ ( T ) = 1 2 0 ( 1 H T 2 ( t ) ) d t = 1 2 0 1 1 u 2 h T ( H T 1 ( u ) ) d u .
Furthermore, Chaudhary et al. [29] investigated another new information measure called weighted negative cumulative extropy (WNCEX), which is defined by
ζ w ( T ) = 1 2 0 t ( 1 H T 2 ( t ) ) d t = 1 2 0 1 H T 1 ( u ) ( 1 u 2 ) h T ( H T 1 ( u ) ) d u .

Motivations of the Work

This study builds upon the work of Abd Elgawad et al. [8] regarding the OSs model, developing a significant parallel model about record values. Numerous real-world experiments lead to the concomitants of record values. These concomitants offer a practical and effective method for organizing and analyzing bivariate record data. One of the main motivations for this work is the practicality and realism of the KRV model, especially considering the rarity of record values. Another driving factor is the application of recent uncertainty measures to our model, which have broad implications across various scientific fields.
This paper is organized as follows: In Section 2, we derive the marginal distribution of CKRV based on the EFGM family and obtain the EX, NCREX, WNCREX, NCEX, and WNCEX for CKRV. In addition, in Section 3, numerical studies based on some well-known distributions are carried out. Moreover, Section 4 introduces the issue of non-parametric estimation of the mentioned measures through simulation studies. Finally, Section 5 presents the study’s conclusion.

2. CKRV Based on EFGM(c,d) and EX, with Some of Its Associated Measures

In this section, we derive the marginal distribution of CKRV based on the EFGM family. Moreover, the EX, NCREX, WNCREX, NCEX, and WNCEX for CKRV are obtained.

2.1. The Marginal Distribution of CKRV Based on EFGM(c,d)

In the next theorem, we obtain a useful representation for the PDF of W [ N , K ] . We use the notation T H T to signify that T is distributed as H T .
Theorem 1. 
Let V 1 H W 2 and V 2 H W 3 . Then
h [ N , K ] ( w ) = h W ( w ) 1 + η [ 1 + 2 ( d 1 ) H W ( w ) 3 d H W 2 ( w ) ] = ( 1 + η ) h W ( w ) + ( d 1 ) η h V 1 ( w ) d η h V 2 ( w ) ,
where
η = c ( d + 1 ) + 2 c ( 2 d + 1 ) K K + 1 N 3 c d K K + 2 N .
Proof. 
The PDF of CKRV is derived, starting with (4) as follows:
h [ N , K ] ( w ) = h W | T ( w | t ) g T N , K ( t ) d t = h W ( w ) 1 + c [ 1 + 2 ( d 1 ) H T ( t ) 3 d H T 2 ( t ) ] × [ 1 + 2 ( d 1 ) H W ( w ) 3 d H W 2 ( w ) ] g T N , K ( t ) d t = h W ( w ) 1 + η [ 1 + 2 ( d 1 ) H W ( w ) 3 d H W 2 ( w ) ] ,
where
η = c 1 + 2 ( d 1 ) H T ( t ) 3 d H T 2 ( t ) g T N , K ( t ) d t .
Using H T ( t ) = 1 H ¯ T ( t ) and simple algebra, we have
η = c ( d + 1 ) + 2 c ( 2 d + 1 ) I 1 3 c d I 2 ,
such that, for p = 1 , 2
I p = H ¯ T p ( t ) g T N , K ( t ) d t .
Taking the transformation H ¯ T ( t ) = e z , we have
I p = K N Γ ( N ) 0 z N 1 e z ( K + p ) d z = K K + p N .
Finally, by using (13) with (14). The proof is completed. □
Remark 1. 
If K = 1 in Theorem 1, we obtain the case of upper record values.
Remark 2. 
When the value of K is large, we can use the approximation η c . Moreover, when the value of N is large, we can use the approximation η c ( d + 1 ) . Finally, when both K and N are large, such that K N , we have η c ( d + 1 ) + 2 c ( 2 d + 1 ) e 1 3 c d e 2 .
Corollary 1. 
By using Theorem 1, the marginal CDF of CKRV and its survival function satisfy the following two elegant symmetry relationships:
H [ N , K ] ( w ) = ( 1 + η ) H W ( w ) + ( d 1 ) η H V 1 ( w ) d η H V 2 ( w )
and
H ¯ [ N , K ] ( w ) = ( 1 + η ) H ¯ W ( w ) + ( d 1 ) η H ¯ V 1 ( w ) d η H ¯ V 2 ( w ) .

2.2. EX and Some of Its More Recent Related Measures

In this section, the measures EX, NCREX, WNCREX, NCEX, and WNCEX for CKRV W [ N , K ] based on EFGM ( c , d ) are derived.

2.2.1. EX of CKRV for EFGM(c,d)

Using (5) and (12), the EX of W [ N , K ] is given by
E X [ N , K ] ( W ) = 1 2 0 h [ N , K ] 2 ( w ) d w = 1 2 0 h W 2 ( w ) A 1 2 + A 2 2 H W 2 ( w ) + A 3 2 H W 4 ( w ) + 2 A 1 A 2 H W ( w ) + 2 A 1 A 3 H W 2 ( w ) + 2 A 2 A 3 H W 3 ( w ) d w = A 1 2 E X ( W ) A 1 A 2 E [ h W ( w ) H W ( w ) ] 1 2 A 2 2 + A 1 A 3 E [ h W ( w ) H W 2 ( w ) ] A 2 A 3 E [ h W ( w ) H W 3 ( w ) ] 1 2 A 3 2 E [ h W ( w ) H W 4 ( w ) ] ,
where A 1 = 1 + η , A 2 = 2 ( d 1 ) η , and A 3 = 3 d η .
We can write E X [ N , K ] ( W ) in terms of the quantile function (QF). Let the QF be Q ( u ) = H W 1 ( u ) , then the quantile density function is given by q ( u ) = 1 / h W ( Q ( u ) ) , where the derivative of Q ( u ) is respect to u and is denoted by q ( u ) (i.e., Q ( u ) = q ( u ) ). Thus, E X [ N , K ] ( W ) is given by
E X [ N , K ] ( W ) = A 1 2 E X ( W ) A 1 A 2 E U q ( u ) 1 2 A 2 2 + A 1 A 3 E U 2 q ( u ) A 2 A 3 E U 3 q ( u ) 1 2 A 3 2 E U 4 q ( u ) ,
where E X ( W ) is the EX of W , and U is a uniformly distributed RV on ( 0 , 1 ) .
Example 1. 
Assume that the random vector ( T , W ) follows the extended Weibull family (denoted by EWF). As mentioned in [30], the EWF has its CDF and PDF described as follows
H T ( t ) = 1 e ϱ G ( t ; τ ) , h T ( t ) = ϱ g ( t ; τ ) e ϱ G ( t ; τ ) ,
respectively, where ϱ > 0 , τ is a vector of parameters, and G ( t , τ ) is a non-negative, continuous, monotonically increasing, differentiable function of t, dependent on the parameter vector τ, such that G ( t , τ ) 0 + as t 0 + and G ( t , τ ) + as t + . g ( t ; τ ) is the derivative of G ( t ; τ ) . Using (18) in (1), the CDF of EFGM with EWF (denoted by EFGM-EWF) is given by
H T , W ( t , w ) = 1 e ϱ 1 G ( t ; τ 1 ) 1 e ϱ 2 G ( w ; τ 2 ) 1 + c e ϱ 1 G ( t ; τ 1 ) ϱ 2 G ( w ; τ 2 ) × 1 + d 1 e ϱ 1 G ( t ; τ 1 ) 1 + d 1 e ϱ 2 G ( w ; τ 2 ) .
According to (17), the EX of W [ N , K ] is
E X [ N , K ] ( W ) = A 1 2 E X ( W ) A 1 A 2 E ϱ 2 g ( w ; τ 2 ) e ϱ 2 G ( w ; τ 2 ) 1 e ϱ 2 G ( w ; τ 2 ) 1 2 A 2 2 + A 1 A 3 E ϱ 2 g ( w ; τ 2 ) e ϱ 2 G ( w ; τ 2 ) 1 e ϱ 2 G ( w ; τ 2 ) 2 A 2 A 3 E ϱ 2 g ( w ; τ 2 ) e ϱ 2 G ( w ; τ 2 ) 1 e ϱ 2 G ( w ; τ 2 ) 3 1 2 A 3 2 E ϱ 2 g ( w ; τ 2 ) e ϱ 2 G ( w ; τ 2 ) 1 e ϱ 2 G ( w ; τ 2 ) 4 .
Example 2. 
Based on Example 1, by using ϱ i G ( x , τ i ) = l o g ( 1 x ) (i.e., ϱ i = 1 ) and ϱ i g ( x , τ i ) = 1 1 x for x = t , w and i = 1 , 2 , respectively, with (19), we obtain the joint uniform distribution with parameters 0 and 1 as EFGM (denoted by EFGM-UD), which is given by
H T , W ( t , w ) = t w [ 1 + c ( 1 t ) ( 1 w ) ( 1 + d t ) ( 1 + d w ) ] .
According to (20), the EX of W [ N , K ] is
E X [ N , K ] ( W ) = 1 2 A 1 2 1 6 A 2 2 1 10 A 3 2 1 2 A 1 A 2 1 3 A 1 A 3 1 4 A 2 A 3 = 1 2 1 6 + 1 6 d + 1 15 d 2 η 2 .
Example 3. 
Based on Example (1), by putting ϱ i G ( x , τ i ) = x λ i (i.e., ϱ i = 1 λ i ) for x = t , w and i = 1 , 2 , respectively, and ϱ i g ( x , τ ) = 1 λ i , in (19), we obtain the joint exponential distribution with parameters λ i > 0 as the EFGM family (denoted by EFGM-ED), which is given as
H T , W ( t , w ) = 1 e t λ 1 1 e w λ 2 1 + c e t λ 1 + w λ 2 1 + d 1 e t λ 1 1 + d 1 e w λ 2 .
Moreover, in view of (20), we have
E X [ N , K ] ( W ) = λ 2 1 4 A 1 2 + 1 24 A 2 2 + 1 60 A 3 2 1 6 A 1 A 2 + 1 12 A 1 A 3 + 1 20 A 2 A 3 = λ 2 1 4 + 1 6 + 1 12 d η + 1 12 + 1 20 d + 1 60 d 2 η 2 .

2.2.2. NCREX of CKRV for EFGM(c,d)

We can obtain ζ R [ N , K ] ( W ) by using (7) and (16) as
ζ R [ N , K ] ( W ) = 1 2 0 H ¯ [ N , K ] 2 ( w ) d w = 1 2 0 ( 1 + η ) 2 H ¯ W 2 ( w ) + ( d 1 ) 2 η 2 H ¯ V 1 2 ( w ) + d 2 η 2 H ¯ V 2 2 ( w ) + 2 ( d 1 ) ( 1 + η ) η H ¯ W ( w ) H ¯ V 1 ( w ) 2 d ( 1 + η ) η H ¯ W ( w ) H ¯ V 2 ( w ) 2 d ( d 1 ) η 2 H ¯ V 1 ( w ) H ¯ V 2 ( w ) d w .
Then,
ζ R [ N , K ] ( W ) = ( 1 + η ) 2 ζ R ( W ) + ( d 1 ) 2 η 2 ζ R ( V 1 ) + d 2 η 2 ζ R ( V 2 ) + ( d 1 ) ( 1 + η ) η E H ¯ W ( w ) H ¯ V 1 ( w ) h W ( w ) d ( 1 + η ) η E H ¯ W ( w ) H ¯ V 2 ( w ) h W ( w ) d ( d 1 ) η 2 E H ¯ V 1 ( w ) H ¯ V 2 ( w ) h W ( w ) .
Also, it can be expressed in another form using QF as
ζ R [ N , K ] ( W ) = 1 2 ( 1 + η ) 2 E ( 1 U ) 2 q ( u ) + 1 2 ( d 1 ) 2 η 2 E 1 U 2 2 q ( u ) + 1 2 d 2 η 2 E 1 U 3 2 q ( u ) + ( d 1 ) ( 1 + η ) η E ( 1 U ) 1 U 2 q ( u ) d ( 1 + η ) η E ( 1 U ) 1 U 3 q ( u ) d ( d 1 ) η 2 E 1 U 2 1 U 3 q ( u ) .
Example 4. 
Let ( T , W ) follow EFGM.
  • According to EFGM-EWF, which is defined by (19), using (23), the NCREX of W [ N , K ] is given by
    ζ R [ N , K ] ( W ) = 1 2 ( 1 + η ) 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) + 1 2 ( d 1 ) 2 η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 2 + 1 2 d 2 η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 2 + ( d 1 ) ( 1 + η ) η E 1 ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 d ( 1 + η ) η E 1 ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 d ( d 1 ) η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 1 1 e ϱ 2 G ( w ; τ 2 ) 3 .
  • For EFGM-UD, which is given by (21), using (24), NCREX of W [ N , K ] is given by
    ζ R [ N , K ] ( W ) = 1 6 1 12 + 1 30 d η + 1 60 + 1 60 d + 1 210 d 2 η 2 .
  • By choosing ϱ i G ( x , τ i ) = l o g 1 w β i (i.e., ϱ i = 1 ) in EFGM-EWF, we obtain the EFGM with power function distribution marginals (denoted by EFGM-PFD), which is given by
    H T , W ( t , w ) = t β 1 w β 2 [ 1 + c 1 t β 1 1 w β 2 ( 1 + d t β 1 ) ( 1 + d w β 2 ) ] , β i > 0 , i = 1 , 2 .
    Also, by using ϱ i G ( x , τ i ) and ϱ i g ( x , τ i ) into (24), we have
    ζ R [ N , K ] ( W ) = β 2 2 1 1 + 3 β 2 + 2 β 2 2 + 2 1 + 6 β 2 + 11 β 2 2 + 6 β 2 3 2 1 + 9 β 2 + 26 β 2 2 + 24 β 2 2 d η + 1 1 + 9 β 2 + 26 β 2 2 + 24 β 2 3 + 1 1 + 12 β 2 + 47 β 2 2 + 60 β 2 3 d + 1 1 + 15 β 2 + 74 β 2 2 + 120 β 2 3 d 2 η 2 .
  • For EFGM-ED with parameters λ i , i = 1 , 2 , whose CDF is (22), the ζ R [ N , K ] ( W ) is given by
    ζ R [ N , K ] ( W ) = 1 λ 2 1 4 1 6 + 1 12 d η + 1 24 + 1 20 d + 1 60 d 2 η 2 .

2.2.3. WNCREX of CKRV for EFGM(c,d)

Using (9) and (16), the WNCREX of W [ N , K ] can be simply obtained as follows:
ζ R [ N , K ] w ( W ) = 1 2 0 w H ¯ [ N , K ] 2 ( w ) d w = 1 2 0 w [ ( 1 + η ) 2 H ¯ W 2 ( w ) + ( d 1 ) 2 η 2 H ¯ V 1 2 ( w ) + d 2 η 2 H ¯ V 2 2 ( w ) + 2 ( d 1 ) ( 1 + η ) η H ¯ W ( w ) H ¯ V 1 ( w ) 2 d ( 1 + η ) η H ¯ W ( w ) H ¯ V 2 ( w ) 2 d ( d 1 ) η 2 H ¯ V 1 ( w ) H ¯ V 2 ( w ) ] d w .
Then,
ζ R [ N , K ] w ( W ) = ( 1 + η ) 2 ζ R w ( W ) + ( d 1 ) 2 η 2 ζ R w ( V 1 ) + d 2 η 2 ζ R w ( V 2 ) + ( d 1 ) ( 1 + η ) η E W H ¯ W ( w ) H ¯ V 1 ( w ) h W ( w ) d ( 1 + η ) η E W H ¯ W ( w ) H ¯ V 2 ( w ) h W ( w ) d ( d 1 ) η 2 E W H ¯ V 1 ( w ) H ¯ V 2 ( w ) h W ( w ) .
In addition, it can be written in terms of QF. Thus, the corresponding ζ R [ N , K ] w ( W ) based on the QF is given by
ζ R [ N , K ] w ( W ) = ( 1 + η ) 2 2 E ( 1 U ) 2 q ( u ) Q ( u ) + ( d 1 ) 2 η 2 2 E 1 U 2 2 q ( u ) Q ( u ) + d 2 η 2 2 E 1 U 3 2 q ( u ) Q ( u ) + ( d 1 ) ( 1 + η ) η E ( 1 U ) 1 U 2 q ( u ) Q ( u ) d ( 1 + η ) η E ( 1 U ) 1 U 3 q ( u ) Q ( u ) d ( d 1 ) η 2 E 1 U 2 1 U 3 q ( u ) Q ( u ) .
Example 5. 
Let T and W follow EFGM.
  • According to EFGM-EWF, which is defined by (19), and by using (26), the WNCREX of W [ N , K ] is
    ζ R [ N , K ] w ( W ) = 1 2 ( 1 + η ) 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) + 1 2 ( d 1 ) 2 η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 2 + 1 2 d 2 η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 2 + ( d 1 ) ( 1 + η ) η E W ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 d ( 1 + η ) η E W ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 d ( d 1 ) η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 1 1 e ϱ 2 G ( w ; τ 2 ) 3 .
  • For EFGM-UD, which is defined by (21), and by using (27), the WNCREX of W [ N , K ] is
    ζ R [ N , K ] w ( W ) = 1 24 1 30 + 1 60 d η + 1 120 + 1 105 d + 1 336 d 2 η 2 .
  • For EFGM-PFD, which is defined in (25), and by using (27), the WNCREX of W [ N , K ] would be
    ζ R [ N , K ] w ( W ) = β 2 2 1 8 + 12 β 2 + 4 β 2 2 + 1 4 + 12 β 2 + 11 β 2 2 + 3 β 2 3 1 4 + 18 β 2 + 26 β 2 2 + 12 β 2 2 d η + 1 8 + 36 β 2 + 52 β 2 2 + 24 β 2 3 + 1 4 + 24 β 2 + 47 β 2 2 + 30 β 2 3 d + 1 8 + 60 β 2 + 148 β 2 2 + 120 β 2 3 d 2 η 2 .
  • According to EFGM-ED, which is described in (22), and by using (27), the WNCREX of W [ N , K ] is given by
    ζ R [ N , K ] w ( W ) = 1 λ 2 2 1 8 5 36 + 13 144 d η + 13 288 + 77 1200 d + 29 1200 d 2 η 2 .
  • Putting ϱ i G ( x , τ i ) = x 2 2 λ i (i.e., ϱ i = 1 2 λ i ) in EFGM-EWF, we obtain EFGM with Rayleigh distribution marginals (denoted by EFGM-RD), which is given by
    H T , W ( t , w ) = 1 e t 2 2 λ 1 1 e w 2 2 λ 2 1 + c e t 2 2 λ 1 + w 2 2 λ 2 1 + d 1 e t 2 2 λ 1 1 + d 1 e w 2 2 λ 2 .
    Therefore, the WNCREX of W [ N , K ] would be
    ζ R [ N , K ] w ( W ) = λ 2 2 1 4 + 1 6 1 12 d η + 1 24 + 1 20 d + 1 60 d 2 η 2 .
  • Choosing ϱ i G ( x , τ i ) = α i l o g σ i x (i.e., ϱ i = α i ), in EFGM- EWF, we obtain EFGM with Pareto type-I distribution marginals (denoted by EFGM-PID), as follows
    H T , W ( t , w ) = 1 σ 1 t α 1 1 σ 2 w α 2 1 + c σ 1 α 1 σ 2 α 2 t α 1 w α 2 1 + d 1 σ 1 t α 1 1 + d 1 σ 2 w α 2 ,
    Further, by using (27), we have
    ζ R [ N , K ] w ( W ) = σ 2 2 1 4 + 4 α 2 + 4 α 2 4 10 α 2 + 6 α 2 2 α 2 2 4 + 18 α 2 26 α 2 2 + 12 α 3 d η + α 2 2 8 + 36 α 2 52 α 2 2 + 24 α 3 + 3 α 2 3 8 56 α 2 + 142 α 2 2 154 α 3 + 60 α 2 4 d + 3 α 2 4 8 + 80 α 2 310 α 2 2 + 580 α 3 522 α 2 4 + 180 α 2 5 d 2 η 2 .
Figure 1a,b depicts the WNCREX of W [ N , K ] from EFGM-PFD for various values of N and K at d = 3 . The following properties can be extracted from Figure 1.
1.
With fixed N, c , and β , the value of ζ R [ N , K ] w ( W ) increases as K decreases (see Figure 1a) and stability occurs for large N .
2.
For the fixed large K , the value of ζ R [ N , K ] w ( W ) increases with the increasing N; see Figure 1b.
Figure 2a,b depicts the WNCREX of W [ N , K ] from EFGM-RD for various values of N and K at d = 2 . The following properties can be extracted from Figure 2.
1.
Stability occurs for large N and K , see Figure 2a,b.
2.
With fixed c and σ , the values of ζ R [ N , K ] w ( W ) are very near to each other as N and K rise.

2.2.4. NCEX of CKRV for EFGM(c,d)

We can calculate the NCEX of CKRV W [ N , K ] as follows:
ζ [ N , K ] ( W ) = 1 2 0 1 H [ N , K ] 2 ( w ) d t = 0 H ¯ [ N , K ] ( w ) d w ζ R [ N , K ] ( W ) = 0 [ ( 1 + η ) H ¯ W ( w ) + ( d 1 ) η H ¯ V 1 ( w ) d η H ¯ V 2 ( w ) ] d w ζ R [ N , K ] ( W ) .
Using (23) and simple algebra, we have
ζ [ N , K ] ( W ) = ( 1 + η ) E H ¯ W ( w ) h W ( w ) + ( d 1 ) η E H ¯ V 1 ( w ) h W ( w ) d η E H ¯ V 2 ( w ) h W ( w ) ( 1 + η ) 2 ζ R ( W ) ( d 1 ) 2 η 2 ζ R ( V 1 ) d 2 η 2 ζ R ( V 2 ) ( d 1 ) ( 1 + η ) η E H ¯ W ( w ) H ¯ V 1 ( w ) h W ( w ) + d ( 1 + η ) η E H ¯ W ( w ) H ¯ V 2 ( w ) h W ( w ) + d ( d 1 ) η 2 E H ¯ V 1 ( w ) H ¯ V 2 ( w ) h W ( w ) .
According to QF, ζ [ N , K ] ( W ) is given by
ζ [ N , K ] ( W ) = ( 1 + η ) E ( 1 U ) q ( u ) + ( d 1 ) η E 1 U 2 q ( u ) d η E 1 U 3 q ( u ) 1 2 ( 1 + η ) 2 E ( 1 U ) 2 q ( u ) 1 2 ( d 1 ) 2 η 2 E 1 U 2 2 q ( u ) 1 2 d 2 η 2 E 1 U 3 2 q ( u ) ( d 1 ) ( 1 + η ) η E ( 1 U ) 1 U 2 q ( u ) + d ( 1 + η ) η E ( 1 U ) 1 U 3 q ( u ) + d ( d 1 ) η 2 E 1 U 2 1 U 3 q ( u ) .
Example 6. 
Let T and W follow the EFGM family
  • For EFGM-EWF, which is defined by (19), and by using (29), the NCEX of W [ N , K ] is
    ζ [ N , K ] ( W ) = ( 1 + η ) E 1 ϱ 2 g ( w ; τ 2 ) + ( d 1 ) η E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 d η E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 1 2 ( 1 + η ) 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 2 ( d 1 ) 2 η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 2 1 2 d 2 η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 2 ( d 1 ) ( 1 + η ) η E 1 ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 + d ( 1 + η ) η E 1 ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 + d ( d 1 ) η 2 E e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 1 1 e ϱ 2 G ( w ; τ 2 ) 3 .
  • For EFGM-UD, as clarified in (21), the following equation is derived using (30):
    ζ [ N , K ] ( W ) = 1 3 1 12 + 1 20 d η 1 60 + 1 60 d + 1 210 d 2 η 2 .
  • For EFGM-ED, with parameters as defined in (22), the equation using (30) is given by
    ζ [ N , K ] ( W ) = 1 λ 2 3 4 1 3 + 1 4 d η 1 24 + 1 20 d + 1 60 d 2 η 2 .
  • For EFGM-PID, with parameters as mentioned in (28), by using (30), then
    ζ [ N , K ] ( W ) = σ 2 1 + 3 α 2 2 6 α 2 + 4 α 2 2 2 α 2 2 1 + 6 α 2 11 α 2 2 + 6 α 2 3 + 6 α 2 3 1 10 α 2 + 35 α 2 2 50 α 3 + 24 α 2 4 d η α 2 2 1 + 9 α 2 26 α 2 2 + 24 α 3 + 6 α 2 3 1 14 α 2 + 71 α 2 2 154 α 3 + 120 α 2 4 d + 3 α 2 4 1 + 20 α 2 155 α 2 2 + 580 α 3 1044 α 2 4 + 720 α 2 5 d 2 η 2 .

2.2.5. WNCEX of CKRV for EFGM(c,d)

Similar to ζ , we can obtain ζ w of W [ N , K ] as
ζ [ N , K ] w ( W ) = ( 1 + η ) E ( 1 U ) q ( u ) Q ( u ) + ( d 1 ) η E 1 U 2 q ( u ) Q ( u ) d η E 1 U 3 q ( u ) Q ( u ) 1 2 ( 1 + η ) 2 E ( 1 U ) 2 q ( u ) Q ( u ) 1 2 ( d 1 ) 2 η 2 E 1 U 2 2 q ( u ) Q ( u ) 1 2 d 2 η 2 E 1 U 3 2 q ( u ) Q ( u ) ( d 1 ) ( 1 + η ) η E ( 1 U ) 1 U 2 q ( u ) Q ( u ) + d ( 1 + η ) η E ( 1 U ) 1 U 3 q ( u ) Q ( u ) + d ( d 1 ) η 2 E 1 U 2 1 U 3 q ( u ) Q ( u ) .
Example 7. 
Suppose that T and W follow the EFGM family
  • For EFGM-EWF, which is defined by (19), by using (31), the WNCEX of W [ N , K ] is
    ζ [ N , K ] w ( W ) = ( 1 + η ) E W ϱ 2 g ( w ; τ 2 ) + ( d 1 ) η E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 d η E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 1 2 ( 1 + η ) 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 2 ( d 1 ) 2 η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 2 1 2 d 2 η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 2 ( d 1 ) ( 1 + η ) η E W ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 + d ( 1 + η ) η E W ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 3 + d ( d 1 ) η 2 E W e ϱ 2 G ( w ; τ 2 ) ϱ 2 g ( w ; τ 2 ) 1 1 e ϱ 2 G ( w ; τ 2 ) 2 1 1 e ϱ 2 G ( w ; τ 2 ) 3 .
  • For EFGM-UD, we have
    ζ [ N , K ] w ( W ) = 1 8 1 20 + 1 30 d η 1 120 + 1 105 d + 1 336 d 2 η 2 .
  • For EFGM-ED, we have
    ζ [ N , K ] w ( W ) = 1 λ 2 2 7 8 11 18 + 25 48 d η 13 288 + 77 1200 d + 29 1200 d 2 η 2 .
  • For EFGM-RD, we have
    ζ R [ N , K ] w ( W ) = λ 2 2 3 4 1 3 + 1 4 d η 1 24 + 1 20 d + 1 60 d 2 η 2 .

3. Numerical Study for the EX, NCREX, WNCREX, NCEX, and WNCEX

Table 1, Table 2, Table 3, Table 4, Table 5 and Table 6 display the EX, NCREX, and WNCREX of W [ N , K ] from EFGM. The following properties can be extracted:
Table 1 displays the EX of W [ N , K ] from the EFGM copula.
  • The value of E X ( W [ N , K ] ; c ) = E X ( W [ N , K ] ; c ) , at d = 3 , 0.9 , 2 .
  • For N > 1 , large K ( K 40 ), and d = 3 , 1 , 0.9 , the value of E X ( W [ N , K ] ; | c | ) increases as the value of N increases.
  • For N > 1 , large K ( K 40 ), and d = 2 , the value of E X ( W [ N , K ] ; | c | ) decreases as the value of N increases.
Table 2 displays the EX of W [ N , K ] based on EFGM-UD.
  • For N > 1 and large K ( K 40 ), the value of E X ( W [ N , K ] ; c ) increases as the value of N increases along with the values of parameters ( c , d ) as ( 0.2 , 3 ) , ( 0.2 , 0.9 ) , and ( 0.1 , 2 ) .
  • For N > 1 and large K ( K 40 ), the value of E X ( W [ N , K ] ; c ) decreases as the value of N increases along with the values of parameters ( c , d ) as ( 0.2 , 3 ) , ( 0.75 , 1 ) , ( 0.25 , 1 ) , ( 0.9 , 0.2 ) , and ( 0.1 , 2 ) .
NCREX in W [ N , K ] based on EFGM copula, NCREX in W [ N , K ] based on EFGM-ED, WNCREX in W [ N , K ] based on EFGM copula, and WNCREX in W [ N , K ] based on EFGM-ED all satisfy the same asymmetry properties extracted for EX in W [ N , K ] from EFGM-ED (Table 2).
Moreover, in the earlier version of this paper, we presented an extra four tables for NCEX in W [ N , K ] based on EFGM copula, NCEX in W [ N , K ] based on EFGM-ED, WNCEX in W [ N , K ] based on EFGM copula, and WNCEX in W [ N , K ] based on EFGM-ED. Responding to the reviewers’ comments about the excessive number of tables, we removed these extra tables, knowing that the same asymmetry properties, as extracted for EX in W [ N , K ] from EFGM-ED, also hold for these removed tables.

4. Non-Parametric Estimation of NCREX, WNCREX, NCEX, and WNCEX

In this section, we study the non-parametric estimators of NCREX, WNCREX, NCEX, and WNCEX of the CKRV, W [ N , K ] . Furthermore, the mean and variance of the empirical measures (EMs) of the CKRV, W [ N , K ] , are deduced. Let W i , i = 1 , 2 , , n , be a random sample from an absolutely continuous CDF H W and W 1 : n W 2 : n W n : n display the OSs of W 1 , W 2 , , W n . Then the EM of H W ( w ) is given by
H ^ W ( w ) = 0 , w < W 1 : n , i n , W i : n w W i + 1 : n , 1 , w > W n : n .
From (33) into (15), we have the EM of H [ N , K ] ( w ) as
H ^ [ N , K ] ( w ) = ( 1 + η ) H ^ W ( w ) + ( d 1 ) η H ^ W 2 ( w ) d η H ^ W 3 ( w ) = ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 .

4.1. EM of NCREX in CKRV Based on EFGM(c,d)

According to (33), the EM of ζ R [ N , K ] ( W ) is given by
ζ R ^ [ N , K ] ( W ) = 1 2 0 1 H ^ [ N , K ] ( w ) 2 d w = 1 2 0 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 d w = 1 2 i = 1 n 1 W i : n W i + 1 : n 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2 d w = 1 2 i = 1 n 1 U i 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2 ,
where U i = W i + 1 : n W i : n , i = 1 , 2 , , n 1 , are sample spacings. Thus, the expectation and variance of the empirical NCREX are given by
E ζ R ^ [ N , K ] ( W ) = 1 2 i = 1 n 1 E [ U i ] 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2
and
V a r ζ R ^ [ N , K ] ( W ) = 1 4 i = 1 n 1 V a r [ U i ] 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 4 .
Example 8. 
Assume that T i , W i , i = 1 , 2 , , n , is a random sample from EFGM-UD with parameters 0 and 1 for each T i and W i . By using (35) and (36), we have
E ζ R ^ [ N , K ] ( W ) = 1 2 ( n + 1 ) i = 1 n 1 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2
and
V a r ζ R ^ [ N , K ] ( W ) = n 4 ( n + 1 ) 2 ( n + 2 ) i = 1 n 1 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 4 .
Example 9. 
Let T i , W i , i = 1 , 2 , , n , be a random sample from EFGM-ED with parameters λ 1 and λ 2 , respectively. Then, we have
E ζ R ^ [ N , K ] ( W ) = 1 2 λ 2 i = 1 n 1 1 n i 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2
and
V a r ζ R ^ [ N , K ] ( W ) = 1 4 λ 2 2 i = 1 n 1 1 ( n i ) 2 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 4 .
Figure 3 shows the relation between NCREX and the empirical NCREX in W [ N , K ] from EFGM-UD, at n = 100 . It can be extracted that, at any value of N, the values of NCREX are very close to the values of the empirical NCREX, as long as n is large.
Table 7 displays the values of E ζ R ^ [ N , K ] ( W ) and V a r ζ R ^ [ N , K ] ( W ) for the EFGM-ED model at K = 2 ,   n = 10 , and d = 0.5 . The following features can be extracted:
  • With fixed N and λ 2 ,   E ζ R ^ [ N , K ] ( W ) and V a r ζ R ^ [ N , K ] ( W ) increase as c increases.
  • With fixed N and c ,   E ζ R ^ [ N , K ] ( W ) and V a r ζ R ^ [ N , K ] ( W ) increase as λ 2 increases.
Table 7. E ζ R ^ [ N , K ] ( W ) and V a r ζ R ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
Table 7. E ζ R ^ [ N , K ] ( W ) and V a r ζ R ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
E ζ R ^ [ N , K ] ( W ) Var ζ R ^ [ N , K ] ( W )
N λ 2 c = 0.2 c = 0.1 c = 0.1 c = 0.2 c = 0.2 c = 0.1 c = 0.1 c = 0.2
30.50.1024920.1074080.1177680.1232130.0015510.0016620.0019110.002051
310.2049850.2148160.2355370.2464260.0062040.0066460.0076430.008204
320.4099700.4296320.4710730.4928520.0248180.0265850.0305740.032817
50.50.0929150.1023440.1233840.1349950.0013500.0015480.0020560.002377
510.1858290.2046870.2467670.2699900.0054000.0061910.0082220.009507
520.3716590.4093750.4935350.5399800.0215980.0247660.0328890.038028
80.50.0872080.0992170.1270560.1428860.0012380.0014800.0021540.002612
810.1744150.1984340.2541130.2857730.0049540.0059210.0086160.010449
820.3488310.3968680.5082260.5715450.0198150.0236840.0344630.041796
100.50.0858300.0984480.1279850.1449040.0012120.0014640.0021790.002675
1010.1716600.1968970.2559710.2898080.0048500.0058560.0087170.010699
1020.3433200.3937930.5119410.5796170.0193990.0234230.0348690.042796

4.2. EM of WNCREX in CKRV Based on EFGM(c,d)

Using (9) and (34), the EM of ζ R [ N , K ] w ( W ) is given by
ζ R w ^ [ N , K ] ( W ) = 1 2 0 w 1 H ^ [ N , K ] ( w ) 2 d w = 1 2 i = 1 n 1 Z i 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2 ,
where Z i = W i + 1 : n 2 W i : n 2 2 , i = 1 , 2 , , n 1 .
Example 10. 
Let T i , W i , i = 1 , 2 , , n , be a random sample from the EFGM family. Furthermore, let W i have a distribution with PDF h W ( w ) = 2 w , 0 < w < 1 . According to Chakraborty et al. [31], W i 2 has a standard UD. Furthermore, the RVs Z i = W i + 1 : n 2 W i : n 2 2 , i = 1 , 2 , , n 1 , follow beta distribution with a mean 1 2 ( n + 1 ) and variance n 4 ( n + 1 ) 2 ( n + 2 ) . Thus,
E ζ R w ^ [ N , K ] ( W ) = 1 4 ( n + 1 ) i = 1 n 1 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2
and
V a r ζ R w ^ [ N , K ] ( W ) = n 16 ( n + 1 ) 2 ( n + 2 ) i = 1 n 1 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 4 .
Example 11. 
Suppose T i , W i , i = 1 , 2 , , n , is a random sample from the EFGM family. If W i has RD with PDF h W ( w ) = 2 λ w e λ w 2 ; w , λ > 0 . Then, the RVs Z i = W i + 1 : n 2 W i : n 2 2 , i = 1 , 2 , , n 1 , follow the exponential distribution with a mean 1 2 λ ( n i ) and variance 1 4 λ 2 ( n i ) 2 . Moreover, the mean and variance of ζ R w ^ [ N , K ] ( W ) are, respectively, given by
E ζ R w ^ [ N , K ] ( W ) = 1 4 λ i = 1 n i 1 n i 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 2
and
V a r ζ R w ^ [ N , K ] ( W ) = 1 16 λ 2 i = 1 n 1 1 ( n i ) 2 1 ( 1 + η ) i n ( d 1 ) η i n 2 + d η i n 3 4 .
Table 8 presents E ζ R w ^ [ N , K ] ( W ) and V a r ζ R w ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .  Table 8 shows the following features:
  • Generally, with fixed N and λ 2 ,   E ζ R w ^ [ N , K ] ( W ) and V a r ζ R w ^ [ N , K ] ( W ) increase with increasing c .
  • Generally, with fixed N and c ,   E ζ R w ^ [ N , K ] ( W ) and V a r ζ R w ^ [ N , K ] ( W ) increase with increasing λ 2 .
Table 8. E ζ R w ^ [ N , K ] ( W ) and V a r ζ R w ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
Table 8. E ζ R w ^ [ N , K ] ( W ) and V a r ζ R w ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
E ζ R w ^ [ N , K ] ( W ) Var ζ R w ^ [ N , K ] ( W )
N λ 2 c = 0.2 c = 0.1 c = 0.1 c = 0.2 c = 0.2 c = 0.1 c = 0.1 c = 0.2
30.50.0512460.0537040.0588840.0616070.0003880.0004150.0004780.000513
310.1024920.1074080.1177680.1232130.0015510.0016620.0019110.002051
320.2049850.2148160.2355370.2464260.0062040.0066460.0076430.008204
50.50.0464570.0511720.0616920.0674970.0003370.0003870.0005140.000594
510.0929150.1023440.1233840.1349950.0013500.0015480.0020560.002377
520.1858290.2046870.2467670.2699900.0054000.0061910.0082220.009507
80.50.0436040.0496090.0635280.0714430.0003100.0003700.0005380.000653
810.0872080.0992170.1270560.1428860.0012380.0014800.0021540.002612
820.1744150.1984340.2541130.2857730.0049540.0059210.0086160.010449
100.50.0429150.0492240.0639930.0724520.0003030.0003660.0005450.000669
1010.0858300.0984480.1279850.1449040.0012120.0014640.0021790.002675
1020.1716600.1968970.2559710.2898080.0048500.0058560.0087170.010699

4.3. EM of NCEX in CKRV Based on EFGM(c,d)

From (34) and (10), we obtain the EM of ζ [ N , K ] as
ζ ^ [ N , K ] ( W ) = 1 2 0 1 H ^ [ N , K ] 2 ( w ) d w = 1 2 i = 1 n 1 U i 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 .
Example 12. 
Suppose that T i , W i , i = 1 , 2 , , n , is a random sample from EFGM-UD with parameters 0 and 1. Thus,
E ζ ^ [ N , K ] ( W ) = 1 2 ( n + 1 ) i = 1 n 1 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2
and
V a r ζ ^ [ N , K ] ( W ) = n 4 ( n + 1 ) 2 ( n + 2 ) i = 1 n 1 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 2 .
Example 13. 
Let T i , W i , i = 1 , 2 , , n , be a random sample from EFGM-ED. Then, we have
E ζ ^ [ N , K ] ( W ) = 1 2 λ 2 i = 1 n 1 1 n i 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2
and
V a r ζ ^ [ N , K ] ( W ) = 1 4 λ 2 2 i = 1 n 1 1 ( n i ) 2 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 2 .
Figure 4 shows the relation between NCREX and the empirical NCEX in W [ N , K ] from EFGM-UD, at n = 100 . It can be concluded that NCREX and empirical NCREX have very similar values.
Table 9 shows E ζ ^ [ N , K ] ( W ) and V a r ζ ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 . It is observed that:
  • At fixed N and λ 2 ,   E ζ ^ [ N , K ] ( W ) and V a r ζ ^ [ N , K ] ( W ) increase as the value of c increases.
  • At fixed N and c ,   E ζ ^ [ N , K ] ( W ) and V a r ζ ^ [ N , K ] ( W ) increase as the value of λ 2 increases.
Table 9. E ζ ^ [ N , K ] ( W ) and V a r ζ ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
Table 9. E ζ ^ [ N , K ] ( W ) and V a r ζ ^ [ N , K ] ( W ) for EFGM-ED at K = 2 ,   n = 10 , and d = 0.5 .
E ζ ^ [ N , K ] ( W ) Var ζ ^ [ N , K ] ( W )
N λ 2 c = 0.2 c = 0.1 c = 0.1 c = 0.2 c = 0.2 c = 0.1 c = 0.1 c = 0.2
30.50.3177450.3277110.3471130.3565490.0114090.0122080.0138780.014747
310.6354910.6554220.6942260.7130980.0456350.0488300.0555130.058989
321.2709801.3108401.3884501.4262000.1825400.1953210.2220530.235954
50.50.2966430.3174350.3568370.3754480.0098470.0113850.0147740.016601
510.5932860.6348700.7136750.7508950.0393890.0455380.0590970.066403
521.1865701.2697401.4273501.5017900.1575570.1821530.2363880.265614
80.50.2828180.3107960.3629310.3870880.0089180.0108750.0153560.017820
810.5656350.6215910.7258620.7741770.0356740.0435010.0614240.071280
821.1312701.2431801.4517201.5483500.1426960.1740030.2456960.285121
100.50.2793180.3091260.3644410.3899480.0086950.0107500.0155030.018129
1010.5586360.6182520.7288810.7798950.0347800.0429990.0620100.072515
1021.1172701.2365001.4577601.5597900.1391200.1719970.2480410.290061

4.4. EM of WNCEX in CKRV Based on EFGM(c,d)

Based on (11), the EM of ζ [ N , K ] w ( W ) is given by
ζ w ^ [ N , K ] ( W ) = 1 2 0 w 1 H ^ [ N , K ] 2 ( w ) d w .
Using the CDF representation of CKRV that is established in (15) and substituting into (37), the empirical measure of ζ [ N , K ] w ( W ) can be calculated as
ζ w ^ [ N , K ] ( W ) = 1 2 0 w 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 d w = 1 2 i = 1 n 1 Z i 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 .
Example 14. 
Assume T i , W i , i = 1 , 2 , , n , is a random sample from the EFGM family and the RV W i follows a distribution with the PDF h W ( w ) = 2 w , 0 < w < 1 . Therefore, we obtain
E ζ w ^ [ N , K ] ( W ) = 1 4 ( n + 1 ) i = 1 n 1 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2
and
V a r ζ w ^ [ N , K ] ( W ) = n 16 ( n + 1 ) 2 ( n + 2 ) i = 1 n 1 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 2 .
Example 15. 
Suppose T i , W i , i = 1 , 2 , , n , is a random sample from the EFGM family. If the RV W i follows the Rayleigh distribution with the PDF h W ( w ) = 2 λ w e λ w 2 ; w , λ > 0 , then, we have
E ζ w ^ [ N , K ] ( W ) = 1 4 λ i = 1 n i 1 n i 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2
and
V a r ζ w ^ [ N , K ] ( W ) = 1 16 λ 2 i = 1 n 1 1 ( n i ) 2 1 ( 1 + η ) i n + ( d 1 ) η i n 2 d η i n 3 2 2 .
Table 10 clarifies a numerical application of Example 15 at K = 2 ,   n = 10 , and d = 0.5 and some distinct values of the parameters c ,   λ 2 , and N . It is apparent that
  • For fixed N and λ 2 ,   E ζ w ^ [ N , K ] ( W ) and V a r ζ w ^ [ N , K ] ( W ) increase as c increases.
  • For fixed N and c ,   E ζ w ^ [ N , K ] ( W ) and V a r ζ w ^ [ N , K ] ( W ) increase as λ 2 increases.
Table 10. E ζ w ^ [ N , K ] ( W ) and V a r ζ w ^ [ N , K ] ( W ) for EFGM-ED at K = 2 , n = 10 , and d = 0.5 .
Table 10. E ζ w ^ [ N , K ] ( W ) and V a r ζ w ^ [ N , K ] ( W ) for EFGM-ED at K = 2 , n = 10 , and d = 0.5 .
E ζ w ^ [ N , K ] ( W ) Var ζ w ^ [ N , K ] ( W )
N λ 2 c = 0.2 c = 0.1 c = 0.1 c = 0.2 c = 0.2 c = 0.1 c = 0.1 c = 0.2
30.50.1588730.1638550.1735560.1782750.0028520.0030520.0034700.003687
310.3177450.3277110.3471130.3565490.0114090.0122080.0138780.014747
320.6354910.6554220.6942260.7130980.0456350.0488300.0555130.058989
50.50.1483210.1587180.1784190.1877240.0024620.0028460.0036940.004150
510.2966430.3174350.3568370.3754480.0098470.0113850.0147740.016601
520.5932860.6348700.7136750.7508950.0393890.0455380.0590970.066403
80.50.1414090.1553980.1814650.1935440.0022300.0027190.0038390.004455
810.2828180.3107960.3629310.3870880.0089180.0108750.0153560.017820
820.5656350.6215910.7258620.7741770.0356740.0435010.0614240.071280
100.50.1396590.1545630.1822200.1949740.0021740.0026870.0038760.004532
1010.2793180.3091260.3644410.3899480.0086950.0107500.0155030.018129
1020.5586360.6182520.7288810.7798950.0347800.0429990.0620100.072515

5. Conclusions

Despite the fact that the EFGM family is as efficient as many other generalizations of the FGM family in terms of correlation level, its flexibility, and usability render it superior to many of these generalizations. Owing to this advantage, most PDFs in this paper are linear functions of other simpler distributions. This study has yielded useful representations of the PDF, CDF, and survival function of CKRV, along with some elegant symmetry relationships between them.
EX and its more recent related measures for CKRV were derived from the EFGM family, where a numerical study was carried out to reveal some features of these measures. Also, the QF based on these measures was derived. In addition, we derived non-parametric estimators of NCREX, WNCREX, NCEX, and WNCEX. An empirical analysis of the NCREX and NCEX has produced distinct results.

Author Contributions

Conceptualization, M.A.A.E., H.M.B., M.A.A., I.A.H., A.F.H. and N.A.; Methodology, M.A.A.E., H.M.B., M.A.A., D.A.A.E.-R., I.A.H., A.F.H. and N.A.; Software, M.A.A.E., D.A.A.E.-R., I.A.H., A.F.H. and N.A.; Validation, M.A.A.E., H.M.B., M.A.A., D.A.A.E.-R., I.A.H., A.F.H. and N.A.; Formal analysis, H.M.B., M.A.A., D.A.A.E.-R., I.A.H., A.F.H. and N.A.; Investigation, M.A.A.E., H.M.B., M.A.A., I.A.H., A.F.H. and N.A.; Resources, M.A.A.E., H.M.B., M.A.A., D.A.A.E.-R., I.A.H., A.F.H. and N.A.; Data curation, M.A.A.E., H.M.B., M.A.A., I.A.H., A.F.H. and N.A.; Writing—original draft, M.A.A.E., D.A.A.E.-R. and A.F.H.; Writing—review & editing, M.A.A.E., M.A.A., D.A.A.E.-R., I.A.H. and N.A.; Visualization, H.M.B. All authors have read and agreed to the published version of this manuscript.

Funding

This work was supported and funded by the Deanship of Scientific Research at Imam Mohammad Ibn Saud Islamic University (IMSIU) (grant number IMSIU-RG23114).

Data Availability Statement

The data used to support the findings of this study are available within the article.

Acknowledgments

The authors would like to express their sincere gratitude to the anonymous reviewers for their insightful comments and recommendations that raised the caliber of this paper.

Conflicts of Interest

The authors declare that they have no competing interests.

Abbreviations

RVsrandom variables
CDFcumulative distribution function
PDFprobability density function
QFquantile function
FGMFarlie–Gumbel–Morgenstern
EFGMextended Farlie–Gumbel–Morgenstern
OSsorder statistics
KRVsK-record upper values
EXextropy
CREXcumulative residual extropy
CKRVK-record upper values
NCREXnegative cumulative residual extropy
WNCREXweighted negative cumulative residual extropy
NCEXnegative cumulative extropy
WNCEXweighted negative cumulative extropy
EFGM-UDEFGM family with uniform marginals
EFGM-EDEFGM family with exponential marginals
EFGM-PFDEFGM family with power function distribution marginals
EFGM-PIDEFGM family with Pareto type-I distribution marginals

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Figure 1. WNCREX of W [ N , K ] from EFGM-PFD.
Figure 1. WNCREX of W [ N , K ] from EFGM-PFD.
Mathematics 11 04934 g001
Figure 2. WNCREX of W [ N , K ] from EFGM-RD.
Figure 2. WNCREX of W [ N , K ] from EFGM-RD.
Mathematics 11 04934 g002
Figure 3. Representation of NCREX and empirical NCREX based on W [ N , K = 1 ] from EFGM-UD.
Figure 3. Representation of NCREX and empirical NCREX based on W [ N , K = 1 ] from EFGM-UD.
Mathematics 11 04934 g003
Figure 4. Representation of NCEX and empirical NCEX based on W [ N , K = 1 ] from EFGM-UD.
Figure 4. Representation of NCEX and empirical NCEX based on W [ N , K = 1 ] from EFGM-UD.
Mathematics 11 04934 g004
Table 1. EX in W [ N , K ] from the EFGM copula.
Table 1. EX in W [ N , K ] from the EFGM copula.
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
21−0.500296−0.500296−0.501042−0.500116−0.503464−0.503464−0.503407−0.503407
23−0.500280−0.500280−0.501775−0.500197−0.504957−0.504957−0.504749−0.504749
25−0.509920−0.509920−0.501079−0.500120−0.523053−0.523053−0.526828−0.526828
27−0.523524−0.523524−0.500329−0.500037−0.537641−0.537641−0.546456−0.546456
61−0.500340−0.500340−0.510762−0.501196−0.511352−0.511352−0.508801−0.508801
63−0.502672−0.502672−0.500001−0.500000−0.503523−0.503523−0.504500−0.504500
65−0.502570−0.502570−0.501708−0.500190−0.500037−0.500037−0.500315−0.500315
67−0.500417−0.500417−0.502927−0.500325−0.501888−0.501888−0.501237−0.501237
401−0.507091−0.507091−0.530776−0.503420−0.514590−0.514590−0.508321−0.508321
403−0.502546−0.502546−0.520221−0.502247−0.513887−0.513887−0.509327−0.509327
405−0.500485−0.500485−0.512740−0.501416−0.512936−0.512936−0.509918−0.509918
407−0.500003−0.500003−0.507577−0.500842−0.511804−0.511804−0.510114−0.510114
1001−0.509078−0.509078−0.534630−0.503848−0.514752−0.514752−0.507955−0.507955
1003−0.506407−0.506407−0.529423−0.503269−0.514562−0.514562−0.508484−0.508484
1005−0.504327−0.504327−0.524863−0.502763−0.514319−0.514319−0.508947−0.508947
1007−0.502751−0.502751−0.520883−0.502320−0.514028−0.514028−0.509341−0.509341
Table 2. EX in W [ N , K ] from EFGM-ED at λ 2 = 0.5 .
Table 2. EX in W [ N , K ] from EFGM-ED at λ 2 = 0.5 .
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
21−0.123657−0.126435−0.120182−0.123307−0.113982−0.137343−0.114444−0.136667
23−0.126394−0.123693−0.132466−0.127341−0.139923−0.111974−0.138892−0.112657
25−0.134587−0.118514−0.130705−0.126812−0.159545−0.099277−0.160551−0.098197
27−0.141051−0.116300−0.128049−0.125989−0.170707−0.093696−0.173601−0.091548
61−0.126541−0.123565−0.112295−0.119868−0.106026−0.148318−0.108578−0.144292
63−0.121247−0.129588−0.124808−0.124936−0.113894−0.137455−0.112965−0.138502
65−0.121311−0.129492−0.132310−0.127294−0.123794−0.126220−0.121671−0.128432
67−0.123417−0.126714−0.134828−0.128032−0.133986−0.116737−0.131897−0.118506
401−0.132902−0.119314−0.108231−0.116846−0.103818−0.151764−0.108993−0.143720
403−0.129469−0.121327−0.109635−0.118193−0.104269−0.151045−0.108138−0.144903
405−0.126852−0.123299−0.111563−0.119459−0.104902−0.150048−0.107661−0.145573
407−0.124863−0.125138−0.113794−0.120633−0.105696−0.148821−0.107506−0.145792
1001−0.134106−0.118731−0.107956−0.116433−0.103716−0.151929−0.109320−0.143274
1003−0.132459−0.119543−0.108353−0.116999−0.103836−0.151736−0.108851−0.143916
1005−0.130984−0.120368−0.108878−0.117554−0.103990−0.151489−0.108454−0.144463
1007−0.129662−0.121198−0.109511−0.118097−0.104177−0.151191−0.108126−0.144920
Table 3. NCREX in W [ N , K ] based on EFGM copula.
Table 3. NCREX in W [ N , K ] based on EFGM copula.
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
210.1672330.1661220.1729910.1687580.1779540.1560430.1769740.156974
230.1661370.1672170.1586340.1639610.1540350.1802490.1552890.178900
250.1638060.1702360.1603830.1645550.1406120.1971400.1410230.197142
270.1625570.1724570.1631790.1654990.1341580.2063900.1339270.207775
610.1660840.1672740.1875250.1734490.1875880.1479210.1835310.151388
630.1684300.1650940.1668970.1667440.1780540.1559550.1785640.155580
650.1683950.1651220.1587860.1640130.1678080.1655320.1697370.163653
670.1673410.1660220.1563990.1631980.1587590.1749370.1607520.172804
4010.1642020.1696380.2028370.1782350.1905500.1455800.1830430.151789
4030.1651290.1683860.1956480.1760060.1899340.1460610.1840510.150962
4050.1659730.1673950.1894340.1740540.1890790.1467340.1846210.150499
4070.1667220.1666120.1840650.1723460.1880220.1475740.1848060.150349
10010.1639160.1700660.2051770.1789540.1906900.1454710.1826630.152104
10030.1643120.1694790.2019850.1779730.1905260.1455990.1832100.151651
10050.1646980.1689440.1989770.1770420.1903140.1457640.1836770.151268
10070.1650720.1684580.1961420.1761600.1900590.1459630.1840650.150951
Table 4. NCREX in W [ N , K ] based on EFGM-ED at λ 2 = 0.5 .
Table 4. NCREX in W [ N , K ] based on EFGM-ED at λ 2 = 0.5 .
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
210.5056480.4945370.5210940.5069730.5485940.4551500.5462960.457407
230.4946860.5054890.4732450.4909830.4467830.5585760.4501120.555050
250.4709540.5352460.4790670.4929620.3919230.6329960.3898720.639289
270.4578500.5568520.4883800.4961080.3663210.6743660.3611410.689354
610.4941540.5060590.5696550.5226200.5907190.4215520.5762120.433355
630.5175180.4841520.5007690.5002560.5490260.4547820.5535210.451371
650.5171670.4844400.4737500.4911550.5048730.4951680.5136920.486650
670.5067240.4935370.4658090.4884400.4665230.5355180.4738900.527455
4010.4750380.5293940.6209340.5386020.6037770.4119930.5739770.435068
4030.4845110.5170800.5968440.5311580.6010590.4139520.5786000.431538
4050.4930450.5072580.5760440.5246400.5972840.4166990.5812160.429564
4070.5005520.4994500.5580840.5189400.5926300.4201290.5820680.428926
10010.4720860.5335880.6287800.5410030.6043980.4115490.5722330.436414
10030.4761690.5278350.6180790.5377250.6036700.4120700.5747420.434480
10050.4801220.5225830.6079980.5346180.6027370.4127410.5768810.432844
10070.4839310.5177880.5985010.5316740.6016100.4135530.5786650.431489
Table 5. WNCREX in W [ N , K ] based on EFGM copula.
Table 5. WNCREX in W [ N , K ] based on EFGM copula.
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
210.0422300.0411180.0437780.0423640.0465190.0371750.0462860.037397
230.0411330.0422140.0389940.0407650.0363350.0475150.0366630.047157
250.0386960.0451250.0395750.0409630.0308140.0549220.0305710.055512
270.0372940.0471940.0405050.0412780.0282260.0590300.0276370.060458
610.0410800.0422700.0486510.0439310.0507170.0338000.0492610.034975
630.0434010.0400640.0417440.0416920.0465630.0371380.0470050.036790
650.0433660.0400930.0390450.0407830.0421540.0411830.0430350.040331
670.0423360.0410180.0382530.0405110.0383150.0452150.0390520.044408
4010.0391230.0445590.0538150.0455330.0520160.0328380.0490390.035148
4030.0401010.0433580.0513870.0447870.0517460.0330350.0494980.034792
4050.0409680.0423890.0492940.0441330.0513700.0333120.0497580.034592
4070.0417220.0416120.0474890.0435620.0509070.0336570.0498420.034528
10010.0388140.0449650.0546070.0457740.0520780.0327930.0488650.035283
10030.0392410.0444070.0535270.0454450.0520060.0328460.0491150.035088
10050.0396500.0438960.0525110.0451330.0519130.0329130.0493270.034923
10070.0400410.0434270.0515540.0448380.0518010.0329950.0495040.034787
Table 6. WNCREX in W [ N , K ] based on EFGM-ED at λ 2 = 0.5 .
Table 6. WNCREX in W [ N , K ] based on EFGM-ED at λ 2 = 0.5 .
d = 3 d = 1 d = 0.9 d = 2
K N c = 0.2 c = 0.2 c = 0.75 c = 0.25 c = 0.2 c = 0.2 c = 0.1 c = 0.1
210.5179040.4827190.5246270.5081380.5896980.4194570.5899880.419617
230.4831910.5173990.4688150.4894830.4047170.6083860.4061270.607259
250.4086420.6122320.4755960.4917910.3108680.7500630.2987870.776836
270.3679950.6815030.4864490.4954600.2691400.8303490.2509380.880013
610.4815090.5192070.5814430.5264100.6690990.3609050.6493090.375500
630.5556420.4499810.5008970.5002990.5905050.4188080.6042360.408448
650.5545220.4508870.4694040.4896840.5088900.4912090.5263600.474529
670.5213190.4795590.4601590.4865190.4396460.5653450.4504110.553077
4010.4213970.5935230.6416030.5450920.6939810.3445820.6448480.378608
4030.4511100.5542470.6133220.5363890.6887920.3479130.6540800.372211
4050.4780060.5230140.5889300.5287700.6815940.3525970.6593110.368646
4070.5017470.4982590.5678900.5221110.6727330.3584650.6610160.367494
10010.4121720.6069300.6508200.5479010.6951660.3438260.6413710.381053
10030.4249350.5885460.6382490.5440670.6937770.3447120.6463760.377540
10050.4373220.5717830.6264130.5404340.6919940.3458530.6506450.374575
10070.4492870.5565020.6152660.5369910.6898440.3472350.6542090.372122
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MDPI and ACS Style

Abd Elgawad, M.A.; Barakat, H.M.; Alawady, M.A.; Abd El-Rahman, D.A.; Husseiny, I.A.; Hashem, A.F.; Alotaibi, N. Extropy and Some of Its More Recent Related Measures for Concomitants of K-Record Values in an Extended FGM Family. Mathematics 2023, 11, 4934. https://doi.org/10.3390/math11244934

AMA Style

Abd Elgawad MA, Barakat HM, Alawady MA, Abd El-Rahman DA, Husseiny IA, Hashem AF, Alotaibi N. Extropy and Some of Its More Recent Related Measures for Concomitants of K-Record Values in an Extended FGM Family. Mathematics. 2023; 11(24):4934. https://doi.org/10.3390/math11244934

Chicago/Turabian Style

Abd Elgawad, Mohamed A., Haroon M. Barakat, Metwally A. Alawady, Doaa A. Abd El-Rahman, Islam A. Husseiny, Atef F. Hashem, and Naif Alotaibi. 2023. "Extropy and Some of Its More Recent Related Measures for Concomitants of K-Record Values in an Extended FGM Family" Mathematics 11, no. 24: 4934. https://doi.org/10.3390/math11244934

APA Style

Abd Elgawad, M. A., Barakat, H. M., Alawady, M. A., Abd El-Rahman, D. A., Husseiny, I. A., Hashem, A. F., & Alotaibi, N. (2023). Extropy and Some of Its More Recent Related Measures for Concomitants of K-Record Values in an Extended FGM Family. Mathematics, 11(24), 4934. https://doi.org/10.3390/math11244934

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