Startseite Sine power Burr X distribution with estimation and applications in physics and other fields
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Sine power Burr X distribution with estimation and applications in physics and other fields

  • Ibrahim Elbatal , Ehab M. Almetwally , Mohamed Kayid , Ahmed W. Shawki , Oluwafemi Samson Balogun und Mohammed Elgarhy EMAIL logo
Veröffentlicht/Copyright: 7. November 2025

Abstract

This article aims to introduce a new three-parameter lifetime distribution called sine power Burr X (SPB-X) distribution. The proposed distribution is obtained by the sine-G class of distributions and the power Burr X distribution. Various properties of the proposed distribution, including explicit expressions for the quantile function, Bowley skewness, Moors kurtosis, ordinary moments, generating function, incomplete and conditional moments, and some numerical and graphical illustrations, are provided. Some various significant reliability metrics for the SPB-X model, including common reliability functions, mean residual life function, mean waiting time function, residual moment, and reversed residual life. Several essential risk measures for the SPB-X distribution. These risk measures include the value at risk, the expected shortfall, the tail value at risk, the tail variance, and the tail variance premium. Four estimation methods were employed to estimate the model’s parameters such as maximum likelihood, least squares, maximum product spacing, and Bayesian. A simulation study is conducted to assess the performance of the estimation methods. Finally, five real data are considered to analyze the usefulness and flexibility of the proposed model.

1 Introduction

Recent years in the field of applied sciences have been characterized by the need and magnitude of data that require analysis. Recently, most statisticians have focused on developing new families that are a generalization of existing distributions to obtain a better fit for data modeling. These families of distributions are derived by compounding multiple distributions or incorporating additional parameters into the baseline model. Recent research has focused on the generation of families of distributions by authors. The beta-G family [1], Kumaraswamy-G [2], T-X family [3], Type II half logistic-G [4], and Topp-Leone odd Fréchet-G [5] are included in this classification. The families described by trigonometric transformations have garnered significant interest due to their applicability and effectiveness in various contexts. These families offer versatility and flexibility as the parameters fluctuate with changes in their values, while the periodic function governs the behavior of the distribution curve. The combination of diverse functions exhibiting distinct behaviors enhances the modeling of real-world phenomena, addressing the limitations of previously established generalized statistical distributions. The sine-G family of distributions, introduced in 2015, is recognized as the pioneering trigonometric family of distributions.

Another method of creating new life distributions by modifying trigonometric functions to produce new statistical distributions was introduced by Kumar et al. [6]. This generated family is called the sine G family and has the following cumulative distribution function (cdf) and probability density function (pdf) as follows:

(1) F ( x ; ζ ) = sin π 2 G ( x , ζ ) , x R

and

(2) f ( x ; ζ ) = π 2 g ( x ; ζ ) cos π 2 G ( x ; ζ ) , x R ,

respectively, where G ( x , ζ ) and g ( x ; ζ ) represent the cdf and pdf of the parent distribution, which has the parameter vector symbolized by ζ . This family offers several advantages, including the following. (1) It is simple. (2) The two cdfs F ( x ) and G ( x ) have the same number of parameters; there are no additional parameters, avoiding the problem of excessive parameterization. (3) The trigonometric function allows F ( x ) to extend the flexibility of G ( x ) , resulting in new flexible models. Among the trigonometric families of distributions, a few of them, including Cos-G [7], sine Kumaraswamy-G [8], sine Topp-Leone-G [9], and Tan-G [10], arcsine exponentiated-X family [11], among others.

The Burr type X (B-X) distribution was first presented and examined by Burr [12]. The B-X distribution has widespread use in dependability research, agriculture, biology, and medicine. In addition, it can accurately depict mechanical strength data and overall lifespan statistics. Several researchers have examined the B-X distribution, starting with [13], which explored several features of the two-parameter B-X distribution and their relationship with other distributions. The beta B-X was examined by Surles and Padgett [14]. Algarni et al. [15] proposed the family of distributions formed by type I half-logistic B-X, whereas Abonongo et al. [16] discussed cosine Fréchet loss distribution, whereas Bantan et al. [17] presented the family of distributions generated by the truncated B-X. Suleiman et al. [18] studied new odd beta prime-B-X distribution, new truncated Zubair-generalized family studied by Soliman et al. [19] transmuted B-X distribution studied by Khan et al. [20], Topp-Leone Weibull generated family studied by Elbatal et al. [21] odd Burr-B-X distribution studied by Butt and Khalil [23], odd log-logistic B-X distribution studied by Usman et al. [24], type I half-logistic B-X distribution proposed by Shrahili et al. [25], Marshall-Olkin exponentiated B-X distribution investigated by Abdullah et al. [26], exponentiated generalized B-X distribution introduced by Khaleel et al. [27], beta Kumaraswamy B-X distribution presented by Madaki et al. [28], Weibull B-X distribution studied by Ishaq et al. [29], Marshall-Olkin extended B-X distribution investigated by Al-Saiari et al. [30], gamma B-X distribution introduced by Khaleel et al. [31], beta B-X distribution discussed by Merovci et al. [32], and Kavya-Manoharan-B-X distribution studied by Hassan et al. [33]. The cdf and pdf of the B-X distribution are provided via

G ( x ; θ , α ) = [ 1 e ( θ x ) 2 ] α , x > 0

and

g ( x ; θ , α ) = 2 α θ 2 x e ( θ x ) 2 [ 1 e ( θ x ) 2 ] α 1 ,

where α > 0 and θ > 0 are the shape and scale parameters, respectively. By including a new parameter, the power transformation of a random variable can provide a more adaptable distribution model. The power B-X (PB-X) distribution was constructed in Ref. [22], with an additional shape parameter λ depending on the transformation procedure. The cdf and pdf of the PB-X distribution are provided and presented by

(3) G ( x ; θ , λ , α ) = [ 1 e ( θ x λ ) 2 ] α , x > 0

and

(4) g ( x ; θ , λ , α ) = 2 α λ θ 2 x 2 λ 1 e ( θ x λ ) 2 [ 1 e ( θ x λ ) 2 ] α 1 .

Often, the PB-X distribution is not flexible enough to represent a variety of lifetime data well. To address this limitation, we propose a novel extension of the PB-X distribution. Inspired by the sine-G family, the new suggested distribution is called the sine PB-X (SPB-X) distribution, and it has the same number of parameters as for the PB-X distribution. In this study, the following objectives will be the main focus:

  1. Create a flexible distribution that can represent ft-skewed, right-skewed, decreased, unimodal, heavy-tailed, and closely to symmetric can be seen in its pdf. A variety of shapes, such as increasing, J-shaped, and decreasing patterns, can be seen in its hrf.

  2. Compute some important statistical properties of the suggested distribution, including its quantile function (QF), Bowley skewness, Moors kurtosis, ordinary moments, generating function, incomplete and conditional moments, and some numerical and graphical illustrations.

  3. Some significant reliability metrics are calculated for the SPB-X model, including common reliability functions, mean residual life function, mean waiting time function, residual moment, and reversed residual life.

  4. Several essential risk measures include the value at risk, the expected shortfall (ES), the tail value at risk (TVaR), the tail variance (TV), and the tail variance premium (TVP).

  5. Estimate the unknown parameters of the SPB-X distribution using four estimation methods, including maximum likelihood, least squares, maximum product spacing (MPS), and Bayesian. To evaluate the efficacy of these estimators in varying scenarios, perform a detailed simulation study.

  6. As a result of its adaptability, the SPB-X distribution appears to be a good contender for modeling five datasets taken from the real world in contrast to other alternatives that are currently available. To illustrate its superiority, this present article examines a variety of modern statistical models, such as the PB-X, shifting exponential Weibull exponential (SEWHE), Weibull, gamma, exponentiated Weibull, sine exponentiated Weibull exponential (SEWE) and Burr III (BIII) distributions.

In this study, an idea for an extension of the PB-X model is presented. The sine-G family serves as a framework for its construction, and the distribution is referred to as the sine power Burr X (SPB-X) distribution. The subsequent sections of this work are structured as follows. In Section 2, we present the SPB-X distribution and give visual representations of its density function. Section 3 examines the many statistical and mathematical features. Multiple reliability metrics are established in Section 4. Some theoretical and numerical actuarial measures are discussed in Section 5. Several different methods of estimation for the unknown parameters are derived in Section 6. A comprehensive Monte Carlo simulation investigation is conducted in Section 7. The utility of the SPB-X distribution is shown through the analysis of five actual datasets in Section 8. Ultimately, the conclusions are presented in Section 9.

2 Construction of the SPB-X model

In this article, we combine the sine G family and the PB-X distribution by inserting (3) in (1) to obtain the cdf of the SPB-X distribution as follows:

(5) F SPB-X ( x ; θ , λ , α ) = sin π 2 [ 1 e ( θ x λ ) 2 ] α ,

where x > 0 , θ , λ , α > 0 . The corresponding pdf of the SPB-X distribution can be constructed by inserting (3) and (4) into (2) as follows:

(6) f SPB-X ( x ; θ , λ , α ) = π 2 2 α λ θ 2 x 2 λ 1 e ( θ x λ ) 2 [ 1 e ( θ x λ ) 2 ] α 1 cos × π 2 [ 1 e ( θ x λ ) 2 ] α .

Figure 1 illustrates some pdf curves for the SPB-X distribution at θ = 0.5 (left panel) and θ = 1.5 (right panel) and for different numerical values of α and λ . From Figure 1, we can note that the pdf for the SPB-X distribution can be left-skewed, right-skewed, decreased, unimodal, and closely symmetric shapes.

Figure 1 
               Plots of the pdf for the SPB-X distribution at 
                     
                        
                        
                           θ
                           =
                           0.5
                        
                        \theta =0.5
                     
                   (left panel) and 
                     
                        
                        
                           θ
                           =
                           1.5
                        
                        \theta =1.5
                     
                   (right panel).
Figure 1

Plots of the pdf for the SPB-X distribution at θ = 0.5 (left panel) and θ = 1.5 (right panel).

To obtain the explicit expression of the distribution, we use the generalized binomial theorem and the Taylor series expansion of the cosine function,

(7) cos π 2 G ( x ) = i = 0 ( 1 ) i ( 2 i ) ! π 2 G ( x ) 2 i

and

(8) ( 1 z ) b 1 = i = 0 ( 1 ) i b 1 i z i .

By using (7) and (8), we have

cos π 2 [ 1 e ( θ x λ ) 2 ] α = i = 0 ( 1 ) i ( 2 i ) ! π 2 2 i [ 1 e ( θ x λ ) 2 ] 2 α i .

One possible way to express the expansion of pdf in Eq. (6) is as follows:

(9) f SPB-X ( x ; θ , λ , α ) = 2 α λ θ 2 i , j = 0 φ ( i , j ) x 2 λ 1 e ( j + 1 ) ( θ x λ ) 2 ,

where

φ ( i , j ) = ( 1 ) i + j ( 2 i ) ! π 2 2 i + 1 ( 2 i + 1 ) α 1 j .

3 Statistical and mathematical properties of SPB-X model

Several significant statistical and mathematical metrics for the SPB-X model are presented in this section.

3.1 Quantile function

There are several uses for the QF, including statistical applications, Monte Carlo techniques, and theoretical parts. The QF algorithm is used in Monte Carlo simulations to generate simulated random variables for classical and novel continuous distributions. It is possible to derive the p th QF of the SPB-X distribution by inverting the Eq. (5) as follows:

(10) x p = Q ( p ) = 1 θ 2 log 1 2 π arcsin ( p ) 1 α 1 2 λ , p ( 0 , 1 ) .

Bowley skewness, which was defined in [34], is considered one of the early skewness measurements that was offered as

SK = Q 3 4 + Q 1 4 2 Q 1 2 Q 3 4 Q 1 4 .

As an alternative, Moors kurtosis [35], which is derived from quantiles, is presented by the following equation:

KU = Q 7 8 Q 5 8 + Q 3 8 Q 1 8 Q 6 8 Q 2 8 .

where Q ( ) represents the QF.

Table 1 displays the values of Q 1 4 , Q 1 2 , and Q 3 4 , which represent the first, second (median), and third percentiles, respectively, offering valuable information on the distribution characteristics of the SPB-X model. The skewness (SK) coefficient quantifies the asymmetry of the distribution, while the kurtosis (KU) coefficient describes its peakedness relative to a normal distribution. These measures are provided for different values of the shape parameters λ and α , with θ fixed at 1.5. Table 1 illustrates how variations in α and λ influence the distribution. Increasing these parameters results in a broader data spread, as reflected in higher percentile values. The skewness and kurtosis values highlight the model’s flexibility in capturing different distributional shapes, making it adaptable to diverse real-world applications. These findings suggest that by adjusting λ and α , the SPB-X distribution can be tailored to exhibit varying degrees of skewness and symmetry, depending on the specific requirements of the dataset.

Table 1

Results of Q 1 4 , Q 1 2 , Q 3 4 , SK, and KU associated with the SPB-X distribution when θ = 1.5

λ α Q 1 4 Q 1 2 Q 3 4 SK KU
0.5 1.5 0.1559 0.2913 0.4835 0.1733 1.2573
1.8 0.2000 0.3482 0.5502 0.1537 1.2532
2.0 0.2278 0.3828 0.5899 0.1441 1.2517
2.2 0.2544 0.4150 0.6263 0.1363 1.2507
2.4 0.2797 0.4451 0.6600 0.1300 1.2504
2.6 0.3038 0.4734 0.6914 0.1246 1.2498
2.8 0.3268 0.5002 0.7207 0.1198 1.2497
3.0 0.3489 0.5254 0.7482 0.1160 1.2497
3.2 0.3699 0.5492 0.7741 0.1126 1.2496
3.4 0.3901 0.5720 0.7987 0.1096 1.2496
3.6 0.4094 0.5936 0.8219 0.1069 1.2497
3.8 0.4280 0.6142 0.8440 0.1045 1.2497
4.0 0.4459 0.6340 0.8650 0.1024 1.2498
1.6 1.5 0.5594 0.6801 0.7968 0.0171 1.2289
1.8 0.6047 0.7191 0.8297 0.0172 1.2325
2.0 0.6299 0.7407 0.8479 0.0168 1.2340
2.2 0.6520 0.7597 0.8640 0.0165 1.2355
2.4 0.6716 0.7765 0.8782 0.0157 1.2364
2.6 0.6891 0.7916 0.8911 0.0151 1.2373
2.8 0.7051 0.8053 0.9027 0.0142 1.2380
3.0 0.7196 0.8178 0.9133 0.0140 1.2383
3.2 0.7329 0.8293 0.9231 0.0132 1.2391
3.4 0.7451 0.8398 0.9321 0.0126 1.2391
3.6 0.7565 0.8496 0.9406 0.0117 1.2393
3.8 0.7670 0.8587 0.9484 0.0112 1.2395
4.0 0.7769 0.8673 0.9557 0.0107 1.2399
2.5 1.5 0.6895 0.7814 0.8647 0.0488 1.2418
1.8 0.7248 0.8098 0.8874 0.0454 1.2429
2.0 0.7439 0.8252 0.8998 0.0434 1.2437
2.2 0.7605 0.8387 0.9107 0.0415 1.2442
2.4 0.7751 0.8505 0.9203 0.0398 1.2442
2.6 0.7880 0.8611 0.9288 0.0382 1.2443
2.8 0.7996 0.8706 0.9366 0.0365 1.2446
3.0 0.8101 0.8792 0.9436 0.0353 1.2442
3.2 0.8196 0.8871 0.9501 0.0338 1.2444
3.4 0.8284 0.8943 0.9560 0.0327 1.2451
3.6 0.8364 0.9009 0.9615 0.0309 1.2441
3.8 0.8439 0.9071 0.9667 0.0302 1.2438
4.0 0.8508 0.9129 0.9714 0.0291 1.2441

3.2 Moments and generating functions

The r th moment of the SPB-X model is calculated as follows:

μ r = 0 x r f ( x ) d x = 2 α λ θ 2 i , j = 0 φ ( i , j ) 0 x r + 2 λ 1 e ( j + 1 ) ( θ x λ ) 2 d x .

By letting y = ( j + 1 ) ( θ x λ ) 2 , after some algebra, the r th moment is provided via

(11) μ r = α θ r λ i , j = 0 φ ( i , j ) Γ ( 1 + r 2 λ ) ( j + 1 ) 1 + r 2 λ .

The moment generating function of the SPB-X distribution may be defined as follows:

M X ( t ) = α θ r λ i , j = 0 φ ( i , j ) t r r ! Γ ( 1 + r 2 λ ) ( j + 1 ) 1 + r 2 λ .

Table 2 presents the numerical values of the first four moments ( μ 1 , μ 2 , μ 3 , and μ 4 ), along with variance ( σ 2 ), standard deviation ( σ ), skewness (SK), kurtosis (KU), and coefficient of variation (CV) for the SPB-X distribution when θ = 1.5 . Table 2 illustrates the effect of varying the shape parameters λ and α on the distribution characteristics. As α increases for a fixed λ , both the mean and variance increase, indicating a wider spread of the distribution. SK values reveal how the distribution deviates from symmetry, transitioning between positive and negative values, demonstrating the model’s ability to represent different distribution shapes, symmetric or skewed to the left or right.

Table 2

Numerical outcomes for the first four moments, σ 2 , σ , SK, KU, and CV for the SPB-X distribution when θ = 1.5

λ α μ 1 μ 2 μ 3 μ 4 σ 2 σ SK KU CV
0.5 1.5 0.3538 0.1973 0.1494 0.1432 0.0721 0.2685 1.4774 6.3418 0.7590
1.8 0.4080 0.2462 0.1958 0.1939 0.0797 0.2823 1.3496 5.8230 0.6919
2.0 0.4410 0.2784 0.2280 0.2301 0.0839 0.2897 1.2846 5.5792 0.6568
2.2 0.4719 0.3102 0.2609 0.2681 0.0876 0.2959 1.2308 5.3877 0.6272
2.4 0.5008 0.3416 0.2944 0.3077 0.0908 0.3013 1.1855 5.2339 0.6018
2.6 0.5280 0.3724 0.3284 0.3486 0.0937 0.3061 1.1469 5.1080 0.5797
2.8 0.5536 0.4027 0.3628 0.3908 0.0962 0.3102 1.1136 5.0031 0.5603
3.0 0.5779 0.4325 0.3974 0.4342 0.0985 0.3139 1.0845 4.9147 0.5431
3.2 0.6010 0.4618 0.4322 0.4786 0.1006 0.3171 1.0589 4.8391 0.5277
3.4 0.6230 0.4905 0.4672 0.5239 0.1024 0.3201 1.0362 4.7739 0.5138
3.6 0.6439 0.5187 0.5023 0.5701 0.1041 0.3227 1.0160 4.7172 0.5012
3.8 0.6639 0.5465 0.5374 0.6170 0.1057 0.3251 0.9978 4.6673 0.4897
4.0 0.6831 0.5737 0.5726 0.6646 0.1071 0.3273 0.9813 4.6233 0.4791
1.6 1.5 0.6771 0.4888 0.3716 0.2953 0.0302 0.1739 0.0526 2.8624 0.2568
1.8 0.7161 0.5402 0.4259 0.3488 0.0275 0.1658 0.0674 2.9135 0.2315
2.0 0.7377 0.5702 0.4587 0.3821 0.0260 0.1611 0.0715 2.9387 0.2184
2.2 0.7568 0.5974 0.4892 0.4137 0.0246 0.1570 0.0726 2.9587 0.2074
2.4 0.7738 0.6223 0.5176 0.4438 0.0235 0.1533 0.0719 2.9748 0.1981
2.6 0.7891 0.6451 0.5443 0.4725 0.0225 0.1499 0.0700 2.9879 0.1900
2.8 0.8029 0.6663 0.5694 0.4998 0.0216 0.1469 0.0671 2.9987 0.1830
3.0 0.8156 0.6859 0.5931 0.5261 0.0208 0.1442 0.0637 3.0077 0.1768
3.2 0.8272 0.7043 0.6156 0.5512 0.0201 0.1417 0.0599 3.0153 0.1713
3.4 0.8379 0.7215 0.6369 0.5753 0.0194 0.1394 0.0559 3.0218 0.1663
3.6 0.8478 0.7376 0.6572 0.5985 0.0188 0.1372 0.0532 3.0391 0.1619
3.8 0.8571 0.7529 0.6765 0.6209 0.0183 0.1352 0.0475 3.0322 0.1578
4.0 0.8657 0.7673 0.6950 0.6424 0.0178 0.1334 0.0432 3.0364 0.1541
2.5 1.5 0.7728 0.6145 0.5007 0.4168 0.0172 0.1310 0.3461 3.1244 0.1695
1.8 0.8023 0.6585 0.5516 0.4705 0.0149 0.1220 0.3347 3.1557 0.1520
2.0 0.8184 0.6834 0.5812 0.5025 0.0137 0.1171 0.3245 3.1657 0.1431
2.2 0.8323 0.7055 0.6080 0.5319 0.0127 0.1128 0.3135 3.1704 0.1356
2.4 0.8446 0.7253 0.6324 0.5591 0.0119 0.1092 0.3021 3.1719 0.1292
2.6 0.8556 0.7433 0.6548 0.5844 0.0112 0.1059 0.2908 3.1712 0.1238
2.8 0.8655 0.7597 0.6755 0.6081 0.0106 0.1030 0.2797 3.1691 0.1191
3.0 0.8744 0.7747 0.6948 0.6303 0.0101 0.1005 0.2690 3.1663 0.1149
3.2 0.8826 0.7885 0.7127 0.6511 0.0096 0.0981 0.2586 3.1630 0.1112
3.4 0.8900 0.8014 0.7295 0.6708 0.0092 0.0960 0.2486 3.1594 0.1079
3.6 0.8969 0.8134 0.7452 0.6895 0.0089 0.0941 0.2391 3.1557 0.1049
3.8 0.9033 0.8246 0.7601 0.7072 0.0085 0.0923 0.2300 3.1520 0.1022
4.0 0.9093 0.8351 0.7741 0.7241 0.0082 0.0907 0.2212 3.1484 0.0997

Furthermore, the values of KU indicate the degree of peakness in the distribution. Higher values correspond to a leptokurtic distribution (more peaked), whereas lower values suggest a platykurtic distribution (flatter). CV reflects the relative dispersion of the data around the mean, with lower values indicating greater homogeneity and higher values suggesting greater variability.

In general, these results highlight the flexibility of the SPB-X distribution and its ability to be customized for different applications by adjusting the shape parameters λ and α to fit the characteristics of the data under analysis. Figure 2 shows 3D plots of the moments measurements for the SPB-X distribution at θ = 2.5 .

Figure 2 
                  3D plots of the moments measurements for the SPB-X distribution at 
                        
                           
                           
                              θ
                              =
                              2.5
                           
                           \theta =2.5
                        
                     .
Figure 2

3D plots of the moments measurements for the SPB-X distribution at θ = 2.5 .

3.3 Incomplete moments

The s th incomplete moment of the SPB-X distribution is given by

(12) m s ( t ) = E ( X s X < t ) = 0 t x s f ( x ) d x = 2 α λ θ 2 i , j = 0 φ ( i , j ) 0 t x s + 2 λ 1 e ( j + 1 ) ( θ x λ ) 2 d x = α θ s λ i , j = 0 φ ( i , j ) γ ( 1 + s 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + s 2 λ ,

where γ ( s , t ) = 0 t x s 1 e x d x is the lower incomplete gamma function.

3.4 Conditional moments

For the SPB-X model, the conditional moments defined by E ( X s X > t ) . It can be written as follows:

E ( X s X > t ) = 1 F ¯ ( t ) κ s ( t ) ,

where

(13) κ s ( t ) = t x s f ( x ) d x = 2 α λ θ 2 i , j = 0 φ ( i , j ) t x s + 2 λ 1 e ( j + 1 ) ( θ x λ ) 2 d x = α θ s λ i , j = 0 φ ( i , j ) Γ ( 1 + s 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + s 2 λ ,

and Γ ( s , t ) = t x s 1 e x d x is the upper incomplete gamma function.

4 Reliability measures

In this section, we suggested various significant reliability metrics for the SPB-X model, including common reliability functions, mean residual life function, mean waiting time function, residual moment, and reversed residual life.

4.1 Common reliability functions

The common reliability functions of SPB-X distribution are survival, hazard rate function (hrf), and reversed hrf, where the survival or reliability function is given by

F ¯ ( x ) = 1 sin π 2 [ 1 e ( θ x λ ) 2 ] α .

The hrf is provided via

τ ( x ) = f ( x ) F ¯ ( x ) = π 2 2 α λ θ 2 x 2 λ 1 e ( θ x λ ) 2 [ 1 e ( θ x λ ) 2 ] α 1 × cos π 2 [ 1 e ( θ x λ ) 2 ] α 1 sin π 2 [ 1 e ( θ x λ ) 2 ] α ,

and reversed hrf is provided via

ς ( x ) = f ( x ) F ( x ) = π 2 2 α λ θ 2 x 2 λ 1 e ( θ x λ ) 2 [ 1 e ( θ x λ ) 2 ] α 1 × cot π 2 [ 1 e ( θ x λ ) 2 ] α .

Figure 3 illustrates some hrf curves for the SPB-X distribution at θ = 0.5 (left panel) and θ = 1.5 (right panel) and for different numerical values of α and λ . From Figure 3, we can note that the hrf for the SPB-X distribution can be decreased, increased, and J-shaped.

Figure 3 
                  Plots of the hrf for the SPB-X distribution at 
                        
                           
                           
                              θ
                              =
                              0.5
                           
                           \theta =0.5
                        
                      (left panel) and 
                        
                           
                           
                              θ
                              =
                              1.5
                           
                           \theta =1.5
                        
                      (right panel).
Figure 3

Plots of the hrf for the SPB-X distribution at θ = 0.5 (left panel) and θ = 1.5 (right panel).

4.2 Mean residual life function

To characterize lifespan distributions, the mean residual life (MRL) function is of critical significance in the fields of dependability, survival analysis, actuarial sciences, economics, and social sciences. In addition, it is an essential component in the repair and replacement methods and provides a comprehensive summary of the residual life function. The MRL function may be derived for the SPB-X distribution from the following:

μ ( t ) = E ( ( X t ) X > t ) = 1 F ¯ ( t ) t x f ( x ) d x t = α F ¯ ( t ) θ 1 λ i , j = 0 φ ( i , j ) Γ ( 1 + 1 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + 1 2 λ t .

4.3 Mean inactivity time function

Given that T i t , the mean waiting time indicates the meantime that has passed since the T i hazard. This is also known as the mean past lifetime (MPL). The random variable of interest in this case is ( t T i T i t ) , where i = 1 , 2 , , n . Given that T i failed before t , this conditional random variable displays the time that has passed since the hazard. The average previous lifespan is provided by

υ ( t ) = E ( t X X t ) = t 1 F ( t ) 0 t x f ( x ) d x = t α F ( t ) θ 1 λ i , j = 0 φ ( i , j ) γ ( 1 + 1 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + 1 2 λ .

4.4 Moment of residual and reversed residual lifes

The residual life is the duration beyond t before failure occurs, specified by the conditional random variable X t X > t . The n th -order moment of the residual life of the random variable X is expressed as follows:

φ n ( t ) = E ( ( X t ) n X > t ) = 1 F ¯ ( t ) t ( x t ) n f ( x ) d x , n 1 .

Employing (8) and utilizing the binomial expansion of ( x t ) n in the aforementioned calculation yields

φ n ( t ) = 1 F ¯ ( t ) d = 0 n ( t ) n d n d t x n f ( x ) d x = α F ¯ ( t ) θ s λ i , j = 0 d = 0 n φ ( i , j ) ( t ) n d n d Γ ( 1 + s 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + s 2 λ .

On the other hand, the r th moment of the reversed residual life can be obtained by the following formula:

ξ r ( t ) = E ( ( t X ) r X t ) = 1 F ( t ) 0 t ( t x ) r f ( x ) d x .

By utilizing (8) and employing the binomial expansion of ( t x ) r in the aforementioned formula, we obtain

ξ r ( t ) = 1 F ( t ) d = 0 r ( t ) r d r d 0 t x r f ( x ) d x = α F ( t ) θ s λ × i , j = 0 d = 0 n φ ( i , j ) ( t ) n d n d γ ( 1 + s 2 λ , ( j + 1 ) ( θ t λ ) 2 ) ( j + 1 ) 1 + s 2 λ .

5 Actuarial measures

In actuarial practice, evaluating risk exposures is essential for companies. One of the primary goals of actuarial science institutes is to forecast market risks within a portfolio of instruments. Consequently, assessing risk measures is crucial in purchasing and selling products. In this section, we will explore many essential risk measures for the SPB-X distribution. These risk measures include the value at risk (VaR), the ES, the TVaR, the TV, and the TVP [47].

5.1 VaR measure

Risk managers often focus on the likelihood of an unfavorable result, which can be quantified using VaR at a certain probability level. The VaR [36] is used to assess risk exposure, thereby determining the capital required to endure undesirable outcomes. The VaR of the SPB-X distribution is specified as follows:

(14) VaR q = 1 θ 2 log 1 2 π arcsin ( q ) 1 α 1 2 λ .

5.2 ES measure

Another significant financial metric is the ES, first articulated by [37,38]. The ES is a metric that provides superior justification for trading relative to VaR.

ES = 1 q 0 q VaR q d x

for 0 < q < 1 and VaR q define in Eq. (4.1).

5.3 TVaR measure

The TVaR is a crucial risk metric. When an event occurs over a set probability threshold, TVaR is used to assess the expected value of the incurred loss. The TVaR of the SPB-X distribution is explicitly specified as follows:

(15) TVaR q ( x ) = 1 1 q VaR q x f ( x ) d x = 1 1 q α θ 1 λ i , j = 0 φ ( i , j ) × Γ ( 1 + 1 2 λ , ( j + 1 ) ( θ ( VaR q ) ) λ ) 2 ( j + 1 ) 1 + 1 2 λ .

5.4 TV measure

The TV risk measure, as put up by Landsman [39], is summarized as the variance of the loss distribution above a certain critical threshold. The TV of the SPB-X distribution may be characterized as follows:

(16) TV q ( x ) = E ( X 2 X > x q ) ( TVaR q ) 2 ,

where

(17) E ( X 2 X > x q ) = 1 1 q VaR q x 2 f ( x ) d x = 1 1 q α θ 2 λ i , j = 0 φ ( i , j ) × Γ ( 1 + 1 λ , ( j + 1 ) ( θ ( VaR q ) ) λ ) 2 ( j + 1 ) 1 + 1 λ .

5.5 TVP measure

The TVP is another important measure that plays an essential role in insurance sciences and is the mixture of central tendency and dispersion statistics. The TVP of SPB-X distribution takes the following form:

(18) TV P q ( x ) = TVaR q + ω TV q ( x ) ,

where 0 < ω < 1 .

Key actuarial metrics, such as VaR, ES, Tail TVaR, TV, and TVP, are summarized in Table 3 for various combinations of λ and α at a fixed θ = 1.5 . Both VaR and ES increase when the quantile level ( q ) increases from 0.650 to 0.995, indicating higher risks at higher confidence levels. TVaR captures more risk in the tail by also following this increasing trend. Meanwhile, TV exhibits constancy in severe loss distributions and stays constant across circumstances. As q and ω grow, TVP measurements reveal increasing contributions from the tail, with ω = 0.9 indicating the largest influence.

Table 3

Actuarial measures for θ = 1.5

λ α q VaR ES TVaR TV TVP
ω = 0.5 ω = 0.75 ω = 0.9
0.5 0.5 0.650 0.1008 0.0298 0.2774 0.0375 0.2961 0.3055 0.3112
0.700 0.1241 0.0357 0.3049 0.0385 0.3242 0.3338 0.3395
0.750 0.1531 0.0425 0.3383 0.0395 0.3580 0.3679 0.3738
0.800 0.1904 0.0505 0.3801 0.0405 0.4004 0.4105 0.4166
0.850 0.2408 0.0601 0.4354 0.0417 0.4563 0.4668 0.4730
0.900 0.3154 0.0721 0.5155 0.0432 0.5371 0.5479 0.5544
0.950 0.4498 0.0880 0.6567 0.0450 0.6792 0.6904 0.6972
0.975 0.5903 0.0989 0.8018 0.0463 0.8250 0.8365 0.8435
0.990 0.7821 0.1075 0.9976 0.0474 1.0213 1.0332 1.0403
0.995 0.9302 0.1113 1.1476 0.0481 1.1717 1.1837 1.1909
1.2 0.650 0.3211 0.1485 0.5605 0.0536 0.5873 0.6008 0.6088
0.700 0.3601 0.1622 0.5972 0.0531 0.6238 0.6371 0.6450
0.750 0.4054 0.1768 0.6403 0.0526 0.6666 0.6797 0.6876
0.800 0.4597 0.1928 0.6924 0.0521 0.7185 0.7315 0.7393
0.850 0.5285 0.2104 0.7590 0.0516 0.7848 0.7977 0.8055
0.900 0.6237 0.2305 0.8521 0.0510 0.8776 0.8903 0.8980
0.950 0.7835 0.2550 1.0094 0.0504 1.0346 1.0472 1.0548
0.975 0.9409 0.2703 1.1656 0.0499 1.1906 1.2031 1.2106
0.990 1.1473 0.2818 1.3708 0.0498 1.3957 1.4082 1.4156
0.995 1.3025 0.2865 1.5257 0.0496 1.5505 1.5629 1.5703
1.6 0.5 0.650 0.4882 0.2854 0.6440 0.0146 0.6513 0.6549 0.6571
0.700 0.5210 0.3010 0.6672 0.0133 0.6738 0.6772 0.6792
0.750 0.5564 0.3169 0.6929 0.0120 0.6989 0.7019 0.7037
0.800 0.5956 0.3330 0.7223 0.0107 0.7276 0.7303 0.7319
0.850 0.6409 0.3498 0.7571 0.0093 0.7618 0.7641 0.7655
0.900 0.6973 0.3674 0.8018 0.0078 0.8057 0.8077 0.8089
0.950 0.7791 0.3868 0.8689 0.0060 0.8719 0.8735 0.8744
0.975 0.8482 0.3976 0.9272 0.0050 0.9297 0.9309 0.9317
0.990 0.9261 0.4050 0.9946 0.0042 0.9967 0.9977 0.9983
0.995 0.9776 0.4077 1.0409 0.0028 1.0423 1.0430 1.0434
1.2 0.650 0.7012 0.5220 0.8222 0.0089 0.8266 0.8289 0.8302
0.700 0.7268 0.5357 0.8402 0.0082 0.8443 0.8463 0.8475
0.750 0.7541 0.5493 0.8601 0.0074 0.8638 0.8657 0.8668
0.800 0.7844 0.5631 0.8830 0.0066 0.8863 0.8879 0.8889
0.850 0.8193 0.5771 0.9102 0.0058 0.9131 0.9145 0.9154
0.900 0.8629 0.5917 0.9451 0.0051 0.9476 0.9489 0.9497
0.950 0.9266 0.6075 0.9985 0.0039 1.0004 1.0014 1.0020
0.975 0.9812 0.6163 1.0455 0.0032 1.0471 1.0480 1.0484
0.990 1.0439 0.6222 1.1008 0.0027 1.1022 1.1028 1.1033
0.995 1.0861 0.6245 1.1384 0.0028 1.1398 1.1405 1.1409

6 Estimation methods

6.1 Maximum likelihood estimation (MLE)

The MLEs [45,58] is the most widely used method of parameter estimation. Let x 1 , x 2 , , x n be a random sample (RS) of size n from the SPB-X distribution; then the log-likelihood function without constant term is given by

(19) L = n log ( α ) + n log ( λ ) + 2 n log ( θ ) + ( 2 λ 1 ) i = 1 n log ( x i ) θ 2 i = 1 n x i 2 λ + ( α 1 ) i = 1 n log ( 1 e ( θ x λ ) 2 ) + i = 1 n log cos π 2 [ 1 e ( θ x λ ) 2 ] α .

To obtain the MLEs of parameters, we differentiate (19) partially with respect to θ , λ , and α and equating them to zero, we obtain the following three equations:

(20) L θ = 2 n θ + 2 i = 1 n log ( x i ) 2 θ i = 1 n x i 2 λ + 2 θ ( α 1 ) i = 1 n x i 2 λ e ( θ x i λ ) 2 1 e ( θ x λ ) 2 + i = 1 n π θ α x i 2 λ e ( θ x i λ ) 2 tan π 2 [ 1 e ( θ x λ ) 2 ] α [ 1 e ( θ x λ ) 2 ] 1 α ,

(21) L λ = n λ + 2 i = 1 n log ( x i ) 2 θ 2 i = 1 n log ( x i ) x i 2 λ + ( α 1 ) i = 1 n log ( x i ) x i 2 λ e ( θ x λ ) 2 1 e ( θ x λ ) 2 + θ 2 i = 1 n π x i 2 λ log ( x i ) tan π 2 [ 1 e ( θ x λ ) 2 ] α e ( θ x i λ ) 2 [ 1 e ( θ x λ ) 2 ] 1 α ,

and

(22) L α = n α + i = 1 n log ( 1 e ( θ x λ ) 2 ) + i = 1 n π log ( 1 e ( θ x λ ) 2 ) tan π 2 [ 1 e ( θ x λ ) 2 ] α 2 [ 1 e ( θ x λ ) 2 ] α .

Then the maximum likelihood estimates of the parameters θ , λ , and α denoted by θ ^ , λ ^ , and α ^ , respectively, are obtained by solving the aforementioned three equations simultaneously.

6.2 Least squares estimators (LSEs)

The LSEs [46,48,49] are key in regression and estimation analysis, with the aim of minimizing the squared differences between observed and predicted values. In linear regression, LSE finds the coefficients that best fit the data. For a RS x ( 1 ) < x ( 2 ) < < x ( n ) from the SPB-X distribution, the LSE for α , θ , and λ minimizes an objective function to achieve the best data fit.More precisely, the LSE minimizes the following objective function:

LSE = i = 1 n i n sin π 2 [ 1 e ( θ x λ ) 2 ] α 2 .

This minimization aims to identify the optimal values of α , θ , and λ , yielding estimates that align the empirical cumulative distribution function with the theoretical one based on the ordered sample, resulting in the best possible fit to the data.

6.3 MPS

MPS estimators are vital in statistical inference, offering efficient parameter estimates for probability distributions, especially useful in survival analysis and reliability modeling with censored data. In survival analysis, where not all failure times in a sample are fully observed, MPS estimators effectively manage such censoring. The method involves MPS between observed failure times to estimate distribution parameters. These estimators are recognized for their robustness against outliers and their strong performance across various distributional assumptions. MPS estimators are widely used in different fields. Further discussions on MPS can be found in papers by previous studies [43,44, 50,51].

The MPS estimators for θ and λ are derived by minimizing the following expression:

D i = F ( x i ; θ , λ , α ) F ( x i 1 ; θ , λ , α ) ; i = 1 , , n + 1 ,

where D i = 1 , then the natural logarithm of product spacing function of SPB-X distribution is

MPS = 1 n + 1 i = 1 n + 1 ln sin π 2 [ 1 e ( θ x ( i ) λ ) 2 ] α sin π 2 [ 1 e ( θ x ( i 1 ) λ ) 2 ] α .

6.4 Bayesian estimation

In this subsection, we utilize the Bayesian estimation method to estimate the unknown parameters of the SPB-X distribution. The core concept of the Bayesian approach is that the model’s parameters are treated as random variables with a predefined distribution, known as the prior distribution. When prior knowledge is available, selecting an appropriate prior is essential. We choose the gamma conjugate prior for the parameters due to several reasons, such as its flexibility, noninformative nature, and the simplicity, it offers in analytical or computational updates to the posterior. In addition, its positive domain makes it well suited for modeling parameters. We implement the Bayesian inference method to estimate the unknown parameters Θ = ( θ , λ , α ) . We assume independent gamma priors for θ , λ , and α . Specifically, θ , λ , and α follow a Gamma distribution Γ ( c i , d i ) , where c i and d i are positive hyperparameters for i = 1 , 2, 3.

The estimates have been derived using the square error loss function. Therefore, the joint prior density of the independent parameters is expressed as follows:

π ( Θ ) = π ( θ ) π ( λ ) π ( α )

and

(23) π ( Θ ) = θ c 1 1 e d 1 θ λ c 2 1 e d 2 λ α c 3 1 e d 3 α ,

where θ > 0 , λ > 0 , α > 0 . The joint posterior for the parameters can be obtained by incorporating the observed censored samples along with the prior distributions of these parameters, as shown below:

(24) π ( Θ , x ) = π ( Θ ) L ( Θ x ) θ 2 n + c 1 1 e d 1 θ λ n + c 2 1 × e d 2 λ α n + c 3 1 e d 3 α e i = 1 n ( θ x i λ ) 2 × i = 1 r x i 2 λ 1 cos π 2 [ 1 e ( θ x i λ ) 2 ] α [ 1 e ( θ x i λ ) 2 ] 1 α .

Since Eq. (24) cannot be solved explicitly, numerical methods are used. One of the most effective numerical approaches in Bayesian estimation is the Monte Carlo Markov chain method. In this case, we propose using the Metropolis–Hastings algorithm, see the study by Tierney [59].

7 Simulation

The simulation of four estimation methods deepens our understanding of statistical techniques, assists in choosing the most appropriate method, and reveals the strengths and weaknesses of various approaches in different contexts. This section utilizes simulation analysis to compare the results of three different parameter estimates for the SPB-X distribution. We carried out simulations by generating 10,000 RS with sizes of n = 25, 70, 100, and 200 from the SPB-X distribution, applying various parameter values ( α , θ , λ ) = (0.5, 0.5, 0.75), (1.5, 0.5, 0.75), (0.5, 0.5, 2), (1.5, 0.5, 2), (1.5, 2, 2), (3, 1.5, 1.5), (3, 1.5, 3), and (1.5, 4, 2). We computed the root mean square error (RMSE) and relative absolute bias (RAB) for all estimates, which are essential metrics to evaluate the performance of different estimators. The simulations were performed using the R programming language, and the results, including the RAB and RMSE values, are summarized in Tables 4, 5, 6, and 7 for the MLE, least squares (LS), MPS, and Bayesian estimation methods. Simulating these four estimation techniques for the SPB-X distribution’s parameters plays a crucial role in statistical research and analysis for several key reasons:

  • Simulations allow researchers to assess the performance of various estimation methods under different conditions. By generating synthetic datasets with known properties, they can evaluate the accuracy, rank, RMSE, and RAB of each technique.

  • Simulations serve as a tool to optimize estimation techniques for the parameters of the SPB-X distribution. Researchers can adjust the algorithm parameters or experiment with alternative methodologies to determine the most efficient and accurate approach for specific scenarios.

  • Through simulation studies, researchers can systematically compare multiple estimators for the SPB-X distribution parameters within a controlled setting. This facilitates an objective assessment of each method’s advantages and limitations, guiding the selection of the most suitable estimator for practical use.

Tables 4, 5, 6, and 7 contain RMSE and RAB values, which are standard metrics used to assess the precision and bias of the different estimation methods. Lower RMSE values suggest more accurate estimates, while lower RAB values suggest less bias. You can see in the tables how the performance of each method changes as the sample size increases. Typically, as sample sizes increase ( n = 200 ), the RMSE and RAB values are expected to decrease, reflecting improved estimation performance. The ranking system (1st, 2nd, 3rd, 4rd) shows which method is best suited for a particular condition. For example, a method ranked “1st” consistently across different parameter settings and sample sizes would indicate it is the most reliable estimator in that situation. The total rank column provides an overall assessment of each method across all conditions. This helps summarize which estimation method is generally superior in terms of various sample sizes and parameter values. A method with consistently low total ranks (closer to 1) is likely the most robust estimator overall.

Table 4

RAB, RMSE, and ranked of estimation methods for parameters of SPB-X distribution

θ = 0.5 , λ = 0.75 MLE LS MPS Bayeaisan
α n RAB RMSE RAB RMSE RAB RMSE RAB RMSE
1.5 25 α 0.098349 1 0.535404 1 0.008759 4 0.16359 4 0.028028 3 0.525338 2 0.096516 2 0.497735 3
θ 0.087211 1 0.159227 1 0.05332 4 0.083594 4 0.086144 2 0.14988 2 0.03257 3 0.12008 3
λ 0.014938 3 0.212967 1 0.006078 4 0.130798 4 0.018591 2 0.186292 2 0.063172 1 0.142277 3
Rank 5 3 12 12 7 6 6 9
70 α 0.064606 2 0.517576 1 0.004599 4 0.099651 4 0.01644 3 0.325084 3 0.085276 1 0.398442 2
θ 0.082028 1 0.140715 1 0.006724 4 0.042627 4 0.010017 3 0.090501 3 0.026713 2 0.099203 2
λ 0.01474 3 0.084148 1 0.00541 4 0.075748 2 0.01495 4 0.081042 3 0.024655 1 0.081247 2
Rank 6 3 12 10 10 9 4 6
100 α 0.016829 2 0.453821 1 0.00126 4 0.085145 4 0.015741 3 0.301315 3 0.059674 1 0.389176 2
θ 0.016211 1 0.124052 1 0.003828 4 0.036019 4 0.009168 3 0.084335 3 0.015022 2 0.091723 2
λ 0.01387 3 0.080529 1 0.00248 4 0.065027 2 0.0149 4 0.079522 2 0.008973 1 0.071036 3
Rank 6 3 12 10 10 8 4 7
200 α 0.014146 2 0.241456 1 0.00114 4 0.031091 4 0.014128 3 0.166741 2 0.030725 1 0.128756 3
θ 0.002011 3 0.066863 1 0.000717 4 0.02494 4 0.0082 1 0.051008 3 0.005046 2 0.052854 2
λ 0.0022 3 0.076778 1 0.00137 4 0.047154 2 0.00922 4 0.06048 3 0.008912 1 0.068712 2
Rank 8 3 12 10 8 8 4 7
Total rank 11 22 16 11
0.5 25 α 0.337683 1 0.50644 1 0.090933 4 0.146 4 0.336589 2 0.45835 2 0.217261 3 0.258538 3
θ 0.111395 1 0.297497 1 0.036013 4 0.166826 4 0.110824 2 0.265625 2 0.100963 3 0.179842 3
λ 0.05131 4 0.395424 1 0.03217 4 0.143998 2 0.05129 3 0.313146 2 0.00881 1 0.20029 3
Rank 6 3 12 10 7 6 7 9
70 α 0.207274 1 0.26776 2 0.05815 4 0.109132 4 0.206881 2 0.301125 1 0.124303 3 0.1626 3
θ 0.090973 1 0.194696 1 0.034912 4 0.095431 4 0.090931 2 0.192916 2 0.076127 3 0.118987 3
λ 0.045 3 0.284272 1 0.01976 4 0.120023 2 0.0452 4 0.220632 2 0.001959 1 0.150957 3
Rank 5 4 12 10 8 5 7 9
100 α 0.192792 2 0.247364 2 0.01696 4 0.066954 4 0.193514 1 0.261325 1 0.100436 3 0.156027 3
θ 0.089484 2 0.176863 1 0.03058 4 0.090415 4 0.089562 1 0.176665 2 0.046063 3 0.109306 3
λ 0.04356 4 0.229272 1 0.018205 4 0.072571 1 0.04056 3 0.202952 2 0.001209 2 0.134832 3
Rank 8 4 12 9 5 5 8 9
200 α 0.149399 1 0.185062 2 0.00283 4 0.024367 4 0.148784 2 0.188903 1 0.043033 3 0.092727 3
θ 0.080922 1 0.148105 1 0.0102 4 0.030511 4 0.07918 2 0.13829 2 0.018522 3 0.077706 3
λ 0.03657 4 0.202376 1 0.00198 4 0.030395 2 0.03465 3 0.157082 2 0.001143 1 0.10759 3
Rank 6 4 12 10 7 5 7 9
Total rank 10 22 12 16
Total rank 21 44 28 27
Table 5

RAB, RMSE, and ranked of estimation methods for parameters of SPB-X distribution

θ = 0.5 , λ = 2 MLE LS MPS Bayeaisan
α n RAB RMSE RAB RMSE RAB RMSE RAB RMSE
0.5 25 α 0.237293 1 0.481939 1 0.031422 4 0.140239 4 0.236122 2 0.369424 2 0.148007 3 0.178753 3
θ 0.094034 1 0.313662 1 0.02126 3 0.159829 4 0.079784 2 0.249774 2 0.069063 3 0.122545 4
λ 0.08233 3 0.56169 1 0.09085 4 0.191695 4 0.08216 2 0.487931 2 0.00937 1 0.246092 3
Rank 5 3 11 12 6 6 7 10
70 α 0.135257 2 0.290683 1 0.030646 4 0.086505 4 0.135534 1 0.230553 2 0.071858 3 0.10814 3
θ 0.065682 2 0.188634 1 0.010859 3 0.083362 4 0.065696 1 0.154763 2 0.035749 3 0.081059 4
λ 0.05906 4 0.463898 1 0.01577 4 0.166698 2 0.05888 3 0.392399 2 0.00845 1 0.215204 3
Rank 8 3 11 10 5 6 7 10
100 α 0.108458 1 0.191718 1 0.02193 4 0.068469 4 0.108304 2 0.181584 2 0.059705 3 0.097331 3
θ 0.059619 1 0.129028 1 0.00774 4 0.068863 4 0.059537 2 0.126247 2 0.033491 3 0.078193 3
λ 0.05741 4 0.373276 1 0.004215 4 0.0915 1 0.05714 3 0.345385 2 0.0071 2 0.204391 3
Rank 6 3 12 9 7 6 8 9
200 α 0.080716 1 0.065794 2 0.002218 4 0.038939 4 0.080353 2 0.12508 1 0.043635 3 0.060712 3
θ 0.053007 1 0.058535 2 0.00176 4 0.038808 4 0.052625 2 0.096398 1 0.028389 3 0.050202 3
λ 0.04536 4 0.184168 2 0.00109 4 0.040365 1 0.04513 3 0.292117 1 0.0061 2 0.179928 3
Rank 6 6 12 9 7 3 8 9
Total rank 12 21 10 17
1.5 25 α 0.05385 4 0.533336 1 0.02125 4 0.214276 2 0.03524 3 0.434168 2 0.041754 1 0.420127 3
θ 0.08557 3 0.225968 1 0.0937 3 0.200131 4 0.08501 2 0.203626 2 0.005053 1 0.082185 4
λ 0.08693 4 0.416789 1 0.058698 3 0.228875 1 0.07017 3 0.355903 2 0.002684 2 0.208831 4
Rank 11 3 10 7 8 6 4 11
70 α 0.036452 1 0.153281 2 0.0086 4 0.115467 4 0.00494 3 0.385402 1 0.034544 2 0.131382 3
θ 0.02989 4 0.151305 2 0.02655 3 0.12475 2 0.02898 3 0.163303 1 0.004341 1 0.065997 4
λ 0.01584 2 0.143572 2 0.01689 4 0.123425 4 0.01638 3 0.292842 1 0.002335 1 0.129063 3
Rank 7 6 11 10 9 3 4 10
100 α 0.019642 2 0.125253 2 0.00629 4 0.08095 4 0.00382 3 0.344566 1 0.031589 1 0.123064 3
θ 0.00937 3 0.137042 1 0.01914 3 0.093568 4 0.00932 2 0.136492 2 0.003622 1 0.060676 4
λ 0.01138 3 0.12584 2 0.001803 3 0.109926 1 0.01141 4 0.271943 1 0.00214 2 0.108031 4
Rank 8 5 10 9 9 4 4 11
200 α 0.017144 2 0.123611 2 0.00254 4 0.070877 4 0.00276 3 0.300586 1 0.023573 1 0.092434 3
θ 0.008163 2 0.105762 1 0.01064 3 0.081686 4 0.008167 1 0.089414 2 0.001453 3 0.055692 4
λ 0.01047 3 0.112907 2 0.00149 4 0.086068 2 0.01068 4 0.222332 1 0.0013 1 0.091578 3
Rank 7 5 11 10 8 4 5 10
Total rank 12 21 12 15
Total rank 24 42 22 32
Table 6

RAB, RMSE, and ranked of estimation methods for parameters of SPB-X distribution

α = 1.5 , λ = 2 MLE LS MPS Bayeaisan
θ n RAB RMSE RAB RMSE RAB RMSE RAB RMSE
2 25 α 0.0417 4 0.784902 1 0.0408 4 0.186499 3 0.0312 2 0.618933 2 0.0798 1 0.452759 3
θ 0.0379 4 0.36032 1 0.0102 2 0.286095 2 0.0377 3 0.274264 3 0.0082 1 0.191702 4
λ 0.038 2 0.756547 1 0.0094 4 0.203331 4 0.0385 1 0.599379 2 0.0039 3 0.249373 3
Rank 10 3 10 9 6 7 5 10
70 α 0.0159 4 0.675556 1 0.006 4 0.178961 2 0.0156 3 0.402374 2 0.052 1 0.323463 3
θ 0.0258 3 0.203099 1 0.0056 2 0.19451 2 0.026 4 0.163596 3 0.0068 1 0.110154 4
λ 0.0093 1 0.711175 1 0.0084 4 0.169255 4 0.0088 2 0.353533 2 0.0037 3 0.213583 3
Rank 8 3 10 8 9 7 5 10
100 α 0.0069 2 0.466559 1 0.0054 4 0.13176 4 0.0069 2 0.361317 2 0.044 1 0.295145 3
θ 0.0165 4 0.172465 1 0.0039 2 0.168627 2 0.0163 3 0.135038 3 0.0055 1 0.084145 4
λ 0.0084 1 0.553203 1 0.002 4 0.142907 4 0.0075 2 0.314431 2 0.0035 3 0.204128 3
Rank 7 3 10 10 7 7 5 10
200 α 0.006 3 0.452244 1 0.0043 4 0.128513 2 0.006 3 0.26335 3 0.0434 1 0.26658 2
θ 0.0094 3 0.109653 1 0.0027 2 0.107198 2 0.0095 4 0.093364 3 0.0055 1 0.058806 4
λ 0.0025 1 0.499037 1 0.0015 4 0.134906 4 0.0021 3 0.237421 2 0.0025 1 0.191229 3
Rank 7 3 10 8 10 8 3 9
Total rank 10 18 18 12
4 25 α 0.0987 1 0.807114 1 0.0536 3 0.480387 4 0.0206 3 0.603981 2 0.056 2 0.442574 4
θ 0.0464 3 0.90611 1 0.0071 4 0.443569 1 0.0467 4 0.68943 2 0.0088 2 0.46061 3
λ 0.0096 2 0.416854 1 0.0241 4 0.1636 1 0.0057 3 0.402546 2 0.0028 4 0.210831 3
Rank 6 3 11 6 10 6 8 10
70 α 0.015 2 0.405756 2 0.027 4 0.253711 4 0.0145 3 0.429374 1 0.0523 1 0.359802 3
θ 0.029 4 0.725479 1 0.0065 4 0.243816 2 0.0284 3 0.462748 2 0.0019 1 0.380727 3
λ 0.0079 4 0.396709 1 0.0134 4 0.123397 1 0.0048 3 0.284519 2 0.0009 2 0.185777 3
Rank 10 4 12 7 9 5 4 9
100 α 0.014 2 0.327157 2 0.007 4 0.212561 4 0.0136 3 0.382202 1 0.0466 1 0.314589 3
θ 0.0229 4 0.306385 2 0.0022 4 0.18737 2 0.0227 3 0.385213 1 0.0014 1 0.306162 3
λ 0.0074 4 0.155957 2 0.0061 4 0.058291 1 0.0037 3 0.227913 1 0.0008 2 0.149529 3
Rank 10 6 12 7 9 3 4 9
200 α 0.0141 2 0.323692 1 0.0062 4 0.187806 4 0.0124 3 0.28776 2 0.0426 1 0.266214 3
θ 0.0205 4 0.290651 2 0.0012 4 0.175217 1 0.0125 3 0.302992 1 0.0013 2 0.229806 3
λ 0.0013 3 0.13804 2 0.0051 4 0.046913 1 0.0037 4 0.189102 1 0.0003 2 0.126885 3
Rank 9 5 12 6 10 4 5 9
Total rank 14 18 14 14
Total rank 24 36 32 26
Table 7

RAB, RMSE, and ranked of estimation methods for parameters of SPB-X distribution

α = 3 , θ = 1.5 MLE LS MPS Bayeaisan
λ n RAB RMSE RAB RMSE RAB RMSE RAB RMSE
1.5 25 α 0.08714 4 0.00711 1 0.08685 3 0.0297 2 1.022988 1 0.247263 4 0.749682 2 0.65512 3
θ 0.0439 3 0.0164 2 0.0439 4 0.00941 1 0.171082 2 0.263046 1 0.142879 3 0.124047 4
λ 0.03102 1 0.0128 4 0.030965 2 0.011691 3 0.721195 1 0.274253 3 0.431103 2 0.210736 4
Rank 8 7 9 6 4 8 7 11
70 α 0.06098 4 0.00626 2 0.06064 3 0.021909 1 0.203063 3 0.164013 4 0.601484 2 0.617428 1
θ 0.03047 4 0.0035 1 0.03033 3 0.00523 2 0.063614 4 0.070686 3 0.099399 1 0.085748 2
λ 0.021379 1 0.00875 4 0.0211 2 0.005284 3 0.148033 4 0.165576 3 0.292466 1 0.175084 2
Rank 9 7 8 6 11 10 4 5
100 α 0.04945 4 0.00506 2 0.0494 3 0.005074 1 0.20064 3 0.153381 4 0.500061 2 0.567637 1
θ 0.02241 3 0.00337 1 0.02243 4 0.00504 2 0.061136 3 0.06013 4 0.078926 1 0.078552 2
λ 0.018067 1 0.001437 4 0.01782 2 0.004198 3 0.127727 4 0.139024 3 0.226073 1 0.167588 2
Rank 8 7 9 6 10 11 4 5
200 α 0.02843 4 0.00214 1 0.02818 3 0.00465 2 0.186027 3 0.148856 4 0.36416 2 0.522604 1
θ 0.01255 4 0.00153 1 0.01253 3 0.0036 2 0.060114 2 0.043521 4 0.055014 3 0.062995 1
λ 0.005953 1 0.00078 4 0.005789 2 0.004023 3 0.052092 4 0.100627 3 0.147558 2 0.153146 1
Rank 9 6 8 7 9 11 7 3
1.5 Total rank 15 15 20 10
3 25 α 0.05279 3 0.00454 1 0.05289 4 0.01405 2 1.01585 1 0.304876 4 0.685717 2 0.670245 3
θ 0.03089 3 0.02071 2 0.03092 4 0.00838 1 0.281515 2 0.322409 1 0.134832 3 0.123108 4
λ 0.00966 3 0.01596 4 0.00953 2 0.00603 1 0.954966 1 0.464819 3 0.569249 2 0.250907 4
Rank 9 7 10 4 4 8 7 11
70 α 0.03685 4 0.00304 2 0.03662 3 0.011103 1 0.206847 3 0.111765 4 0.553092 1 0.545158 2
θ 0.01952 4 0.00439 2 0.0195 3 0.00201 1 0.194985 1 0.152068 2 0.093001 3 0.088362 4
λ 0.002145 2 0.00756 4 0.001838 3 0.002758 1 0.247989 2 0.22598 3 0.397819 1 0.219657 4
Rank 10 8 9 3 6 9 5 10
100 α 0.02922 3 0.00237 2 0.02956 4 0.010222 1 0.189243 3 0.102759 4 0.481484 2 0.511498 1
θ 0.01546 4 0.00407 2 0.01544 3 0.001072 1 0.156499 1 0.148069 2 0.078632 3 0.075901 4
λ 0.001646 3 0.00279 4 0.001779 1 0.001779 2 0.142582 4 0.216851 3 0.344835 1 0.220094 2
Rank 10 8 8 4 8 9 6 7
200 α 0.02282 3 0.00218 2 0.02284 4 0.009103 1 0.146666 3 0.091199 4 0.367609 2 0.413775 1
θ 0.01258 3 0.00172 2 0.01261 4 0.00091 1 0.152245 1 0.043352 4 0.054523 3 0.055331 2
λ 0.000397 3 0.000944 2 0.000335 4 0.001427 1 0.137847 4 0.159341 3 0.251225 1 0.186038 2
Rank 9 6 12 3 8 11 6 5
Total rank 15 15 19 11
Total rank 30 30 39 21

The best-performing estimation method can be determined using the total rank column in the table. The method with the highest total rank is considered the most effective in different scenarios. Based on the ranked values provided in the table, it is clear which method consistently achieves better performance in terms of RMSE and RAB. In the case of θ = 0.5 , λ = 0.75 , we observe that the LS method performs the best, achieving a total rank of 201. This is the highest value compared to the other estimation methods, indicating its superior performance in this scenario. In the case of θ = 0.5 , λ = 2 , we observe that the Bayesian estimation method performs the best, achieving a total rank of 221. This is the highest value compared to the other estimation methods, indicating its superior performance in this scenario. In the case of α = 1.5 , λ = 2 , we observe that the LS method performs the best, achieving a total rank of 173. This is the highest value compared to the other estimation methods, indicating its superior performance in this scenario.

In all cases, the LS method achieved the highest total rank, reaching 546, indicating its superior performance. The Bayesian method followed with a total rank of 494. However, the MLE method had the lowest performance, with a total rank of 327, making it the least effective among the estimation methods compared.

7.1 Approximate confidence intervals (ACIs)

Determining the exact distribution of these estimates becomes problematic when closed-form MLEs and MPS for the unknown parameters cannot be obtained. Therefore, it is not feasible to obtain precise confidence intervals (CIs) for the parameters. Hence, ACIs are built using large sample approximation approaches for the parameters α , θ , and λ to overcome this constraint.

Using the asymptotic normality features of MLEs and MPS, one may compute the ACIs for Θ = ( α , θ , λ ) , which are generated from the observed Fisher information matrix. For the purpose of approximating the asymptotic variance–covariance of the MLEs and MPS, the observed information matrix is obtained by differentiating the log-likelihood function with respect to the unknown parameters.

(25) I ( Θ ˆ ) = 2 L Θ i Θ j Θ ˆ .

From there, we can obtain the approximate asymptotic variance–covariance matrix, which is:

(26) Cov ( ϑ ˆ ) = I 1 ( ϑ ˆ ) .

With a mean of Θ and a variance–covariance matrix of Cov ( Θ ˆ ) , Θ ˆ N ( Θ , Cov ( Θ ˆ ) ) , the MLEs and MPS parameters are roughly distributed according to a multivariate normal distribution. The ACIs for the unknown parameters can be expressed as 100 ( 1 ε ) % for any 0 < ε < 1 .

(27) Θ ˆ ρ ε 2 V ar ( Θ ˆ ) , Θ ˆ + ρ ε 2 V ar ( Θ ˆ ) .

The ( 1 ε ) quantile of the standard normal distribution N ( 0 , 1 ) is represented by ρ ε 2 .

Tables 8 and 9 present confidence intervals for the parameters ( α , θ , λ ) of the SPB-X distribution using the MLE and MPS methods for different sample sizes and parameter values. It shows that as the sample size increases, the confidence intervals become narrower, indicating better precision. The lower limits, upper limits, and the length average of confidence intervals (LACIs) are computed. The MPS method generally produces slightly narrower intervals than MLE, suggesting better accuracy in some cases. Furthermore, confidence intervals vary according to parameter values, with broader intervals observed for θ = 0.5 compared to θ = 2 . In general, the table highlights the comparative performance of the two estimation methods and the impact of sample size on the reliability of the estimation.

Table 8

Confidence intervals for parameters of SPB-X distribution

θ = 0.5 , λ = 0.75 θ = 2 , λ = 0.75
MLE MPS MLE MPS
α n Lower Upper LACI Lower Upper LACI α Lower Upper LACI Lower Upper LACI
1.5 25 α 0.6388 2.6563 2.0175 0.5157 2.5684 2.0527 0.5 0.0699 1.1674 1.0975 0.0416 1.3042 1.3722
θ 0.2435 0.8438 0.6003 0.2617 0.8244 0.5627 0.1030 0.9910 0.8880 0.0566 1.0232 0.9665
λ 0.3444 1.1780 0.8337 0.3998 1.1281 0.7282 0.7828 2.8879 2.1051 0.9352 2.7361 1.8010
70 α 0.6004 2.5934 1.9930 0.8893 2.1600 1.2707 0.0135 1.1217 1.1082 0.1358 0.9997 0.8638
θ 0.2772 0.8048 0.5277 0.3279 0.6821 0.3542 0.1688 0.8969 0.7282 0.2364 0.8293 0.5928
λ 0.5754 0.9024 0.3270 0.5815 0.8961 0.3146 1.0026 2.7611 1.7585 1.1486 2.6159 1.4673
100 α 0.6371 2.4134 1.7762 0.9349 2.1124 1.1775 0.1938 0.9147 0.7208 0.2144 0.8939 0.6794
θ 0.2655 0.7507 0.4852 0.3395 0.6696 0.3301 0.2838 0.7759 0.4921 0.2893 0.7702 0.4809
λ 0.5831 0.8961 0.3130 0.5845 0.8931 0.3086 1.1890 2.5813 1.3923 1.2469 2.5245 1.2776
200 α 1.0498 1.9926 0.9428 1.1970 1.8454 0.6483 0.4385 0.6422 0.2037 0.3080 0.7723 0.4643
θ 0.3700 0.6320 0.2621 0.4044 0.6038 0.1993 0.4242 0.6288 0.2046 0.3445 0.7081 0.3635
λ 0.5979 0.8988 0.3009 0.6253 0.8609 0.2355 1.5951 2.2234 0.6283 1.3652 2.4543 1.0891
0.5 25 α 0.0665 1.2712 1.2047 1.1693 2.8405 1.6712 1.5 0.3859 2.4525 2.0666 0.4039 2.4903 2.0864
θ 0.1593 0.9520 0.7927 0.0462 1.0646 1.0183 0.0223 0.8921 0.8698 0.0672 0.8478 0.7806
λ 0.1095 1.3135 1.2040 0.1024 1.3207 1.2182 1.0837 2.5686 1.4849 1.2186 2.5007 1.2821
70 α 0.1197 1.0875 0.9678 0.0492 1.1577 1.1086 1.2740 1.8353 0.5613 0.5488 2.4660 1.9172
θ 0.1744 0.9165 0.7421 0.1780 0.9129 0.7349 0.1899 0.7802 0.5902 0.1667 0.8043 0.6376
λ 0.1630 1.2695 1.1065 0.2888 1.1434 0.8546 1.6939 2.2428 0.5489 1.3969 2.5376 1.1407
100 α 0.1499 1.0429 0.8930 0.1210 1.0726 0.9516 1.2909 1.7681 0.4772 0.6243 2.3871 1.7628
θ 0.2094 0.8801 0.6708 0.2098 0.8797 0.6699 0.2269 0.7638 0.5369 0.2280 0.7627 0.5347
λ 0.2725 1.1621 0.8896 0.3263 1.1129 0.7866 1.7347 2.2198 0.4852 1.4460 2.5083 1.0623
200 α 0.2428 0.9066 0.6637 0.2341 0.9147 0.6807 1.2887 1.7627 0.4740 0.7085 2.2998 1.5913
θ 0.2612 0.8197 0.5585 0.2799 0.7993 0.5194 0.2969 0.7112 0.4143 0.3290 0.6792 0.3501
λ 0.3296 1.1156 0.7860 0.4204 1.0277 0.6073 1.7616 2.1965 0.4349 1.4875 2.4698 0.9823
Table 9

Confidence intervals for parameters of SPB-X distribution: α = 1.5 , λ = 2

α = 1.5 , λ = 2 MLE MPS
θ n Lower Upper LACI Lower Upper LACI
2 25 α 0.1006 2.7742 2.6736 0.2748 2.6940 2.4193
θ 1.2337 2.6145 1.3808 1.4078 2.4416 1.0338
λ 0.6007 3.5513 2.9507 0.9118 3.2420 2.3301
70 α 0.1529 2.7994 2.6465 0.7049 2.2795 1.5746
θ 1.5634 2.3334 0.7700 1.6439 2.2519 0.6079
λ 0.6251 3.4119 2.7869 1.3256 2.7097 1.3841
100 α 0.5962 2.4246 1.8285 0.7955 2.2113 1.4158
θ 1.6352 2.2989 0.6636 1.7105 2.2241 0.5136
λ 0.9330 3.1006 2.1676 1.3994 2.6305 1.2312
200 α 0.6048 2.3772 1.7724 0.9811 2.0129 1.0317
θ 1.7694 2.1929 0.4235 1.8019 2.1603 0.3584
λ 1.0269 2.9830 1.9561 1.5389 2.4695 0.9305
4 25 α 0.0929 3.2031 3.1102 0.3280 2.6925 2.3645
θ 2.0762 5.5530 3.4768 2.5125 5.1142 2.6016
λ 1.2031 2.8354 1.6323 1.2227 2.8000 1.5774
70 α 0.7285 2.3166 1.5881 0.6667 2.3477 1.6810
θ 2.4804 5.2877 2.8073 3.0071 4.7654 1.7583
λ 1.2073 2.7611 1.5539 1.4331 2.5478 1.1147
100 α 0.8811 2.1609 1.2798 0.7588 2.2549 1.4961
θ 3.3354 4.4815 1.1461 3.1756 4.6432 1.4677
λ 1.6810 2.2896 0.6086 1.5461 2.4390 0.8929
200 α 0.8880 2.1542 1.2662 0.9434 2.0690 1.1257
θ 3.3715 4.4646 1.0931 3.3643 4.5357 1.1715
λ 1.7269 2.2679 0.5410 1.6222 2.3629 0.7407

8 Applications

In this section, we present a comprehensive discussion of various statistical metrics used to evaluate the performance of different models [57]. Tables 10, 11, 12, 13, and 15 provide a detailed comparison of key metrics, including estimates, standard errors (StEr), Kolmogorov-Smirnov distance (KSD), p -value for the Kolmogorov-Smirnov test (PVKS), Cramer-von Mises statistic (CVM), p -value for CVM (PVCVM), Anderson–Darling (AD) statistic, and p -value for AD (PVAD).

Table 10

MLE for parameters of SPB-X and each competitive models: latitude for the Southwest of the rain gauge stations

Estimates StEr KSD PVKS CVM PVCVM AD PVAD
SPB-X α 14.5195 91.8156 0.1684 0.9141 0.0380 0.9417 0.3073 0.9254
θ 0.8207 2.1497
λ 1.0578 2.2285
PB-X α 5.2896 19.5810 0.1709 0.9049 0.0385 0.9391 0.3103 0.9207
θ 0.4440 1.1365
λ 1.8414 2.6215
SEWHE α 2.5621 7.9144 0.1740 0.8932 0.0506 0.9341 0.3817 0.9218
θ 3.1999 5.2423
λ 1.4554 4.0546
β 0.3341 0.1767
W α 8.0720 1.9099 0.1764 0.8834 0.0579 0.8369 0.4090 0.8368
θ 2.0251 0.0800
G α 51.0781 18.4243 0.1703 0.9042 0.03914 0.9352 0.3116 0.9179
θ 0.0374 0.0135
EW α 0.6437 0.4917 0.1709 0.9050 0.0404 0.9391 0.3204 0.9207
θ 3.6794 5.2306
λ 5.3017 19.6086
Table 11

MLE for parameters of SPB-X and each competitive models: latitude for West of rain gauge stations

Estimates StEr KSD PVKS CVM PVCVM AD PVAD
SPB-X α 2.7126 9.3506 0.1036 0.9978 0.0196 0.9960 0.1702 0.9949
θ 0.2305 0.9371
λ 1.0543 1.9056
PB-X α 1.8090 4.3094 0.1038 0.9976 0.0197 0.9952 0.1703 0.9940
θ 0.1305 0.4589
λ 1.4638 1.7972
SEWHE α 0.7708 2.8499 0.1417 0.9422 0.0329 0.9927 0.2473 0.9913
θ 3.1580 9.7527
λ 0.1476 0.6489
β 0.1821 0.2501
W α 4.0489 0.9208 0.1201 0.9866 0.02484 0.9926 0.1920 0.9928
θ 4.6803 0.3525
G α 12.5199 5.0407 0.1129 0.9932 0.0220 0.9954 0.1884 0.9936
θ 0.3383 0.1390
EW α 0.2487 0.1808 0.1038 0.9968 0.0223 0.9962 0.1817 0.9920
θ 2.9275 3.7318
λ 1.8087 4.4687
Table 12

MLE for parameters of SPB-X and each competitive models: dataset of carbon fibers stress

Estimates StEr KSD PVKS CVM PVCVM AD PVAD
SPB-X α 0.8472 0.4571 0.0784 0.8124 0.0809 0.8604 0.4809 0.8972
θ 0.0878 0.0994
λ 1.8287 0.6911
PB-X α 0.8006 0.3533 0.0809 0.7801 0.0858 0.6861 0.5084 0.7619
θ 0.1009 0.0829
λ 1.9554 0.5340
SEWHE α 4.6250 2.6478 0.0862 0.7112 0.0868 0.8398 0.4921 0.8694
θ 0.4987 0.1811
λ 0.4402 0.2756
β 0.9296 0.2869
SEWE α 0.9319 0.2743 0.0812 0.7771 0.0821 0.7176 0.4811 0.7918
θ 3.3898 0.5825
λ 0.0121 0.0107
BIII α 2.2416 0.1688 0.1941 0.0138 0.7133 0.0076 3.9874 0.0050
θ 5.8443 0.8339
W α 3.4412 0.3309 0.0822 0.7630 0.0836 0.6727 0.4857 0.7607
θ 3.0623 0.1149
G α 7.4880 1.2757 0.1328 0.1947 0.2461 0.1935 1.3107 0.2288
θ 0.3685 0.0649
EW α 0.3094 0.0331 0.0809 0.7795 0.0813 0.6859 0.4847 0.7618
θ 3.9118 1.0682
λ 0.8000 0.3528
Table 13

MLE for parameters of SPB-X and each competitive models: dataset of carbon fibers strength

Estimates StEr KSD PVKS CVM PVCVM AD PVAD
SPB-X α 0.8548 0.5113 0.0470 0.9980 0.0238 0.9995 0.2087 0.9981
θ 0.2995 0.2240
λ 1.7155 0.7232
PB-X α 0.8131 0.3847 0.0479 0.9974 0.0259 0.9932 0.2236 0.9870
θ 0.3759 0.1884
λ 1.8324 0.5392
SEWHE α 1.6525 2.5956 0.0477 0.9978 0.0239 0.9990 0.2093 0.9978
θ 1.5192 2.5144
λ 0.5202 1.5503
β 0.5532 1.1950
SEWE α 0.8961 0.4053 0.0478 0.9978 0.0240 0.9959 0.2098 0.9912
θ 3.2901 0.9324
λ 0.1064 0.0914
BIII α 3.2367 0.2923 0.1407 0.1304 0.3344 0.0782 2.1634 0.0588
θ 2.0133 0.2424
W α 3.2489 0.3065 0.1201 0.9866 0.02484 0.9926 0.2920 0.9928
θ 1.6171 0.0629
G α 6.9960 1.1629 0.0884 0.6535 0.1235 0.4824 0.8539 0.4432
θ 0.2074 0.0357
EW α 0.5862 0.0712 0.0479 0.9973 0.0232 0.9932 0.2112 0.9870
θ 3.6666 1.0799
λ 0.8124 0.3846
Table 15

MLE for parameters of SPB-X and each competitive models: insurance dataset

Estimates StEr KSD PVKS CVM PVCVM AD PVAD
SPB-X α 16.8042 0.9714 0.0881 0.9463 0.0505 0.8767 0.3508 0.8949
θ 0.2799 0.2559
λ 1.0771 47.5307
PBX α 0.7679 0.5972 0.0910 0.9319 0.0518 0.8687 0.3551 0.8910
θ 0.4524 0.2740
λ 7.1741 12.1309
SEWE α 0.8713 0.5111 0.0915 0.9291 0.0525 0.8642 0.3583 0.8880
θ 0.3280 0.4747
λ 6.7275 10.9735
BIII α 15.3663 4.8010 0.1442 0.4749 0.1413 0.4190 0.8172 0.4677
θ 2.1054 0.2600
W α 2.0483 0.2612 0.0940 0.8939 0.0534 0.8657 0.3771 0.8701
θ 5.9411 0.5431
G α 4.0985 0.9865 0.0988 0.8954 0.0532 0.8666 0.3898 0.8452
θ 1.2798 0.3277
EW α 0.5570 0.7609 0.0909 0.9319 0.0517 0.8688 0.3549 0.8911
θ 0.9054 0.5482
λ 7.1603 12.0956

The performance of each model is presented in a detailed perspective, focusing on various distribution models, such as the power Burr X (PB-X) proposed by [22], the SEWHE by [42], Weibull (W) [52], gamma (G) [53], exponentiated Weibull (EW) [54], SEWE [42], and BIII [55] distributions.

8.1 Rainfall data analysis across Peninsular Malaysia

This study analyzed daily rainfall data collected from 50 rain gauge stations in Peninsular Malaysia during the period 1975–2004. Data were sourced from the Malaysian Meteorological Department and the Drainage and Irrigation Department. Following the regional classification by Dale (1959), the area was divided into five distinct rainfall zones: northwest, west, the Port Dickson–Muar coast, southwest, and east (Lim and Azizan [56]). Due to limited data availability, the ports on the port Dickson–Muar coast were grouped with the southwest region.

To ensure data reliability, the dataset was meticulously examined for missing values and homogeneity. Interestingly, less than 10% of the data was missing. The missing values were estimated using enhanced spatial weighting techniques [60], while homogeneity was verified through four robust statistical tests [61]: the standard normal homogeneity test, the Buishand range test, the Pettitt test, and the Von Neumann ratio test, as documented in [62].

Our analysis focused on the latitude data from two key regions, the Southwest and East. The latitude values for the Southwest region are: 1.47, 1.63, 1.63, 1.76, 1.87, 1.88, 1.92, 2.02, 2.25, 2.27, 2.29, and for the east region: 2.45, 2.59, 3.17, 3.56, 3.78, 3.90, 4.23, 4.76, 4.94, 5.32, 5.97, 6.17. In Tables 10 and 11, we provide an in-depth comparison of various models using MLE with StEr, KSD, PVKS, CVM, PVCVM, AD, and PVAD. Among the tested distributions, the SPB-X distribution consistently outperformed others across multiple metrics, including KSD, PVKS, CVM, PVCVM, AD, and PVAD, making it the most suitable model for this rainfall dataset.

Figures 4 and 5 includes the histogram, violin plot, QQ (quantile-quantile) plot, box plot with stripchart, and TTT (total time in test) plot of dataset of rain gauge stations datasets. The estimated PDFs of competing models for the datasets of rain gauge stations datasets are shown in Figures 6 and 9, while Figures 7 and 10 display the estimated CDFs of the competitive models. Furthermore, Figures 8 and 11 illustrate the PP plots of the competing models. Figures 611 demonstrate the fit of our distribution to the actual data.

Figure 4 
                  Some basic nonparametric plots for latitude for southwest of rain gauge stations.
Figure 4

Some basic nonparametric plots for latitude for southwest of rain gauge stations.

Figure 5 
                  Some basic nonparametric plots for latitude for west of rain gauge stations.
Figure 5

Some basic nonparametric plots for latitude for west of rain gauge stations.

Figure 6 
                  Estimated PDFs for the competing models for latitude for southwest of rain gauge stations.
Figure 6

Estimated PDFs for the competing models for latitude for southwest of rain gauge stations.

Figure 7 
                  Estimated CDFs for the competing models for latitude for southwest of rain gauge stations.
Figure 7

Estimated CDFs for the competing models for latitude for southwest of rain gauge stations.

Figure 8 
                  The PP plot for the competing models for latitude for southwest of rain gauge stations.
Figure 8

The PP plot for the competing models for latitude for southwest of rain gauge stations.

Figure 9 
                  Estimated PDFs for the competing models for latitude for west of rain gauge stations.
Figure 9

Estimated PDFs for the competing models for latitude for west of rain gauge stations.

Figure 10 
                  Estimated CDFs for the competing models for latitude for west of rain gauge stations.
Figure 10

Estimated CDFs for the competing models for latitude for west of rain gauge stations.

Figure 11 
                  The PP plot for the competing models for latitude for west of rain gauge stations.
Figure 11

The PP plot for the competing models for latitude for west of rain gauge stations.

8.2 Breaking stress of carbon fibers dataset

The breaking stress of carbon fibers dataset contains crucial measurements of the maximum stress that carbon fibers can endure before fracturing. This dataset is indispensable for researchers and engineers in the fields of materials science and engineering. It plays a key role in investigating the mechanical properties and performance of carbon fiber-reinforced composites, widely used in industries such as aerospace and automotive manufacturing.

As mentioned by Cordeiro and Lemonte [40], this specific dataset offers valuable insights into the behavior of carbon fibers under stress. Below is the dataset:

{3.15, 1.25, 2.95, 4.38, 2.12, 1.47, 0.39, 2.79, 2.59, 2.05, 2.56, 3.65, 2.74, 1.87, 3.56, 4.42, 3.31, 2.55, 2.03, 3.19, 2.67, 3.22, 2.48, 2.43, 4.70, 3.09, 4.90, 1.61, 3.22, 2.50, 2.93, 3.68, 1.57, 1.80, 2.53, 2.81, 1.84, 2.87, 1.61, 3.11, 2.41, 3.60, 3.75, 3.27, 2.82, 2.35, 2.96, 3.39, 2.55, 0.85, 3.28, 3.11, 2.03, 1.08, 3.27, 2.03, 1.69, 3.39, 2.73, 3.31, 2.88, 4.20, 3.33}.

This dataset allows for deeper analysis into the variability and resilience of carbon fibers under extreme stress conditions. Researchers can apply these data to optimize material performance and design more efficient and durable composites, which are integral to high-stress environments.

In Table 12, we provide an in-depth comparison of various models using MLE with StEr, KSD, PVKS, CVM, PVCVM, AD, and PVAD. Among the tested distributions, the SPB-X distribution consistently outperformed others across multiple metrics, including KSD, PVKS, CVM, PVCVM, AD, and PVAD, making it the most suitable model for breaking stress of carbon fibers dataset.

Figure 12 includes the histogram, violin plot, QQ plot, box plot with stripchart, and TTT plot of dataset of breaking stress of carbon fibers datasets. The estimated PDFs of competing models for the of dataset of breaking stress of carbon fibers datasets are shown in Figure 13, while Figure 14 displays the estimated CDFs of the competitive models. In addition, Figure 15 illustrates the PP plots of the competing models. Figures 1315 demonstrate the fit of our distribution to the actual data.

Figure 12 
                  Some basic nonparametric plots for dataset of carbon fibers stress.
Figure 12

Some basic nonparametric plots for dataset of carbon fibers stress.

Figure 13 
                  Estimated PDFs for the competing models for dataset of carbon fibers stress.
Figure 13

Estimated PDFs for the competing models for dataset of carbon fibers stress.

Figure 14 
                  Estimated CDFs for the competing models for dataset of carbon fibers stress.
Figure 14

Estimated CDFs for the competing models for dataset of carbon fibers stress.

Figure 15 
                  The PP plot for the competing models for dataset of carbon fibers stress.
Figure 15

The PP plot for the competing models for dataset of carbon fibers stress.

8.3 Tensile strength of carbon fibers dataset

Tensile strength, typically expressed in Gigapascals (GPa), measures the maximum stress a single carbon fiber can withstand before fracturing under tension. This property is essential in evaluating the performance and reliability of carbon fiber-reinforced materials, widely applied across industries such as aerospace, automotive, and sports equipment manufacturing. An in-depth understanding of the tensile strength of carbon fibers directly influences the design and development of more durable and resilient composite structures.

The dataset used in this study, sourced from Kundu and Raqab [41], contains tensile strength measurements for individual carbon fibers, expressed in GPa. The following is the dataset:

{1.098, 1.253, 0.944, 1.055, 1.586, 1.773, 1.554, 2.012, 1.301, 1.179, 1.884, 0.966, 0.552, 1.179, 1.642, 0.312, 1.426, 1.726, 0.865, 1.063, 0.803, 1.514, 1.270, 2.233, 1.301, 1.240, 1.627, 2.096, 1.533, 1.534, 1.321, 1.801, 1.559, 0.865, 0.979, 2.094, 1.300, 0.865, 1.434, 1.235, 2.585, 1.684, 2.012, 1.048, 1.373, 1.633, 1.697, 0.753, 1.726, 1.754}.

This dataset provides critical insights into the variability of tensile strength between individual fibers, allowing engineers and materials scientists to optimize the use of carbon fibers in high-performance applications. Using such data, industries can create composites that push the boundaries of durability and functionality in demanding environments.

In Table 13, we provide an in-depth comparison of various models using MLE with StEr, KSD, PVKS, CVM, PVCVM, AD, and PVAD. Among the tested distributions, the SPB-X distribution consistently outperformed others across multiple metrics, including KSD, PVKS, CVM, PVCVM, AD, and PVAD, making it the most suitable model for the tensile strength of the carbon fibers dataset.

Figure 16 includes the histogram, violin plot, QQ plot, box plot with stripchart, and TTT plot of dataset of tensile stress of carbon fibers datasets. The estimated PDFs of competing models for the of dataset of tensile stress of carbon fibers datasets are shown in Figure 17, while Figure 18 displays the estimated CDFs of the competitive models. In addition, Figure 19 illustrates the PP plots of the competing models. Figures 1719 demonstrate the fit of our distribution to the actual data.

Figure 16 
                  Some basic nonparametric plots for dataset of carbon fibers strength.
Figure 16

Some basic nonparametric plots for dataset of carbon fibers strength.

Figure 17 
                  The PDF plot of SPB-X distribution for dataset of carbon fibers strength.
Figure 17

The PDF plot of SPB-X distribution for dataset of carbon fibers strength.

Figure 18 
                  The CDF plot of SPB-X distribution for dataset of carbon fibers strength.
Figure 18

The CDF plot of SPB-X distribution for dataset of carbon fibers strength.

Figure 19 
                  The PP plot of SPB-X distribution for dataset of carbon fibers strength.
Figure 19

The PP plot of SPB-X distribution for dataset of carbon fibers strength.

8.4 Insurance dataset

The insurance dataset, which spans the years 1987–2017, displays the excess of assets over liabilities for investments made by insurance companies, pension funds, and trusts. The values are expressed in billions of pounds. The following is the electronic address that it was obtained from: The link https://www.ons.gov.uk/  references the aforementioned product. The dataset is reported in Table 14.

Table 14

Sed Excess of assets over liabilities for investment by insurance companies, and pension funds

Period Value Period Value Period Value
1986 2.151 1997 4.301 2008 15.264
1987 2.208 1998 8.421 2009 4.547
1988 2.170 1999 6.661 2010 3.261
1989 2.707 2000 6.548 2011 3.426
1990 2.014 2001 4.977 2012 6.418
1991 1.698 2002 4.202 2013 7.389
1992 2.512 2003 5.580 2014 6.136
1993 4.857 2004 8.856 2015 5.820
1994 3.509 2005 6.902 2016 3.094
1995 5.066 2006 5.442 2017 8.216
1996 5.413 2007 8.067

In Table 15, we provide an in-depth comparison of various models using MLE with StEr, KSD, PVKS, CVM, PVCVM, AD, and PVAD. Among the tested distributions, the SPB-X distribution consistently outperformed others across multiple metrics, including KSD, PVKS, CVM, PVCVM, AD, and PVAD, making it the most suitable model for insurance dataset.

Figure 20 includes the histogram, violin plot, QQ plot, box plot with stripchart, and TTT plot of dataset of insurance datasets. The estimated PDFs of competing models for the of dataset of insurance datasets are shown in Figure 21, while Figure 22 displays the estimated CDFs of the competitive models. In addition, Figure 23 illustrates the PP plots of the competing models. Figures 2123 demonstrate the fit of our distribution to the actual data.

Figure 20 
                  Some basic nonparametric plots for insurance dataset.
Figure 20

Some basic nonparametric plots for insurance dataset.

Figure 21 
                  Estimated PDFs for the competing models for insurance dataset.
Figure 21

Estimated PDFs for the competing models for insurance dataset.

Figure 22 
                  Estimated CDFs for the competing models for insurance dataset.
Figure 22

Estimated CDFs for the competing models for insurance dataset.

Figure 23 
                  Estimated CDFs for the competing models for insurance dataset.
Figure 23

Estimated CDFs for the competing models for insurance dataset.

The actuarial measures VaR, ES, TVaR, TV, and TVP of the SPB-X, PBX, and SEWE distributions are computed and compared using the actual dataset in the following. Tables 16 and 17 present the numerical findings.

Table 16

The actuarial metrics VaR, ES, TVaR, and TV values for the insurance dataset

Measure q SPB-X PBX SEWE Measure q SPB-X PBX SEWE
VaR 0.650 5.6930 5.6868 5.6815 TVaR 0.650 8.1786 8.1798 8.1864
0.700 6.0936 6.0942 6.0883 0.700 8.5602 8.5620 8.5707
0.750 6.5548 6.5636 6.5577 0.750 9.0087 9.0100 9.0215
0.800 7.1068 7.1253 7.1199 0.800 9.5554 9.5537 9.5695
0.850 7.8061 7.8351 7.8317 0.850 10.2603 10.2501 10.2728
0.900 8.7813 8.8196 8.8215 0.900 11.2598 11.2275 11.2621
0.910 9.0343 9.0736 9.0772 0.910 11.5214 11.4812 11.5193
0.920 9.3174 9.3569 9.3629 0.920 11.8150 11.7648 11.8070
0.930 9.6388 9.6776 9.6864 0.930 12.1493 12.0863 12.1336
0.940 10.0109 10.0474 10.0598 0.940 12.5376 12.4578 12.5112
0.950 10.4529 10.4843 10.5016 0.950 13.0001 12.8975 12.9586
0.960 10.9973 11.0190 11.0430 0.960 13.5715 13.4364 13.5076
0.970 11.7060 11.7088 11.7426 0.970 14.3173 14.1328 14.2184
0.975 12.1596 12.1465 12.1873 0.975 14.7957 14.5752 14.6705
0.980 12.7200 12.6832 12.7331 0.980 15.3873 15.1177 15.2255
0.985 13.4515 13.3766 13.4396 0.985 16.1607 15.8193 15.9443
0.990 14.5011 14.3577 14.4412 0.990 17.2715 16.8120 16.9634
0.995 16.3499 16.0457 16.1700 0.995 19.2293 18.5203 18.7222
0.999 20.9308 20.0204 20.2655 0.999 24.0749 22.5402 22.8827
ES 0.650 3.6882 3.6717 3.0239 TV 0.650 6.2552 5.9357 6.0739
0.700 3.8454 3.8299 3.1817 0.700 6.2759 5.9001 6.0496
0.750 4.0103 3.9961 3.3478 0.750 6.3207 5.8717 6.0364
0.800 4.1860 4.1735 3.5252 0.800 6.4003 5.8557 6.0379
0.850 4.3774 4.3671 3.7190 0.850 6.5323 5.8534 6.0582
0.900 4.5932 4.5853 3.9378 0.900 6.7623 5.8743 6.1107
0.910 4.6406 4.6332 3.9859 0.910 6.8288 5.8828 6.1274
0.920 4.6898 4.6830 4.0359 0.920 6.9061 5.8936 6.1473
0.930 4.7413 4.7350 4.0881 0.930 6.9969 5.9070 6.1710
0.940 4.7953 4.7895 4.1429 0.940 7.1061 5.9239 6.1998
0.950 4.8525 4.8470 4.2009 0.950 7.2404 5.9453 6.2352
0.960 4.9135 4.9084 4.2628 0.960 7.4118 5.9739 6.2815
0.970 4.9797 4.9748 4.3299 0.970 7.6437 6.0116 6.3398
0.975 5.0153 5.0104 4.3660 0.975 7.7954 6.0358 6.3776
0.980 5.0532 5.0482 4.4043 0.980 8.1037 6.0678 6.4260
0.985 5.0938 5.0886 4.4454 0.985 8.2437 6.1081 6.4876
0.990 5.1385 5.1328 4.4906 0.990 8.6181 6.1666 6.5745
0.995 5.1897 5.1829 4.5421 0.995 9.2927 6.2645 6.7159
0.999 5.2410 5.2322 4.5935 0.999 10.9996 6.4753 7.0392
Table 17

The actuarial metrics TVP values for the insurance dataset

ω q SPB-X PBX SEWE ω q SPB-X PBX SEWE
0.50 0.650 11.3062 11.1476 11.2233 0.90 0.650 13.8083 13.5219 13.6528
0.700 11.6982 11.5121 11.5955 0.700 14.2085 13.8721 14.0153
0.750 12.1690 11.9459 12.0397 0.750 14.6973 14.2946 14.4543
0.800 12.7555 12.4815 12.5884 0.800 15.3156 14.8238 15.0036
0.850 13.5265 13.1768 13.3019 0.850 16.1395 15.5182 15.7251
0.900 14.6410 14.1646 14.3174 0.900 17.3459 16.5143 16.7617
0.910 14.9358 14.4226 14.5830 0.910 17.6674 16.7757 17.0340
0.920 15.2680 14.7116 14.8807 0.920 18.0304 17.0690 17.3396
0.930 15.6478 15.0398 15.2191 0.930 18.4466 17.4026 17.6875
0.940 16.0906 15.4197 15.6110 0.940 18.9331 17.7893 18.0910
0.950 16.6203 15.8702 16.0762 0.950 19.5165 18.2483 18.5702
0.960 17.2774 16.4234 16.6484 0.960 20.2421 18.8129 19.1610
0.970 18.1391 17.1386 17.3882 0.970 21.1966 19.5432 19.9242
0.975 18.6934 17.5931 17.8593 0.975 21.8115 20.0074 20.4103
0.980 19.4391 18.1517 18.4385 0.980 22.6806 20.5788 21.0089
0.985 20.2825 18.8733 19.1881 0.985 23.5800 21.3166 21.7831
0.990 21.5805 19.8953 20.2507 0.990 25.0278 22.3620 22.8805
0.995 23.8756 21.6525 22.0802 0.995 27.5927 24.1583 24.7666
0.999 29.5747 25.7779 26.4023 0.999 33.9745 28.3680 29.2180
0.75 0.650 12.8700 12.6316 12.7418 0.99 0.650 14.3712 14.0561 14.1995
0.700 13.2672 12.9871 13.1079 0.700 14.7734 14.4031 14.5598
0.750 13.7492 13.4138 13.5488 0.750 15.2661 14.8230 14.9976
0.800 14.3556 13.9454 14.0979 0.800 15.8916 15.3508 15.5470
0.850 15.1596 14.6402 14.8164 0.850 16.7274 16.0450 16.2704
0.900 16.3316 15.6332 15.8451 0.900 17.9545 17.0430 17.3116
0.910 16.6431 15.8933 16.1149 0.910 18.2820 17.3052 17.5855
0.920 16.9945 16.1850 16.4175 0.920 18.6520 17.5994 17.8929
0.930 17.3970 16.5166 16.7619 0.930 19.0763 17.9343 18.2429
0.940 17.8672 16.9007 17.1610 0.940 19.5726 18.3224 18.6489
0.950 18.4304 17.3565 17.6350 0.950 20.1681 18.7834 19.1314
0.960 19.1304 17.9168 18.2187 0.960 20.9092 19.3506 19.7263
0.970 20.0500 18.6415 18.9732 0.970 21.8845 20.0843 20.4947
0.975 20.6422 19.1020 19.4537 0.975 22.5131 20.5506 20.9843
0.980 21.4650 19.6686 20.0450 0.980 23.4099 21.1249 21.5873
0.985 22.3434 20.4004 20.8100 0.985 24.3219 21.8663 22.3670
0.990 23.7351 21.4370 21.8943 0.990 25.8034 22.9170 23.4722
0.995 26.1988 23.2187 23.7592 0.995 28.4290 24.7221 25.3710
0.999 32.3246 27.3967 28.1621 0.999 34.9645 28.9508 29.8515

Figure 24 includes the competing model VaR, ES, TVaR, and TV plots for the insurance dataset. the competing model TVP plots for the insurance dataset shown in Figure 25.

Figure 24 
                  Competing model VaR, ES, TVaR, and TV plots for the insurance dataset.
Figure 24

Competing model VaR, ES, TVaR, and TV plots for the insurance dataset.

Figure 25 
                  Competing model TVP plots for the insurance dataset.
Figure 25

Competing model TVP plots for the insurance dataset.

We find that for different significance levels q and different values of ω , the SPB-X model has higher values for the risk measures VaR, ES, TVaR, TV, and TVP from Tables 16 and 17 and Figures 24 and 25. This suggests that compared to the PBX and SEWE distributions, the SPB-X model has a heavier tail.

From Table 18, it is observed that both estimation methods produce consistent results with only minor differences in the estimated parameters. In several datasets (Data1, Data3, Data4, and Data5), LSE achieves slightly smaller KS values and higher p -values compared to MLE, confirming its robustness in certain contexts. However, in other cases (Data2), MLE and LSE results are very close. These findings indicate that while LSE may have some advantages in terms of goodness-of-fit, both methods lead to the same empirical conclusion: the proposed SPB-X distribution provides the best overall fit to the datasets. Thus, the choice of estimation method does not alter the validity of the application results reported in Section 8.

Table 18

Parameter estimates of the SPB-X distribution using MLE and LSE for the five datasets, along with KSD and PVKS

Data Method α θ λ KSD PVKS
Data1 MLE 14.5195 0.8207 1.0578 0.1684 0.9141
LSE 19.8840 1.0673 0.7378 0.1415 0.9803
Data2 MLE 2.7126 0.2305 1.0543 0.1036 0.9978
LSE 1.7772 0.1973 1.0428 0.1088 0.9957
Data3 MLE 0.8472 0.0878 1.8287 0.0784 0.8124
LSE 0.5967 0.0255 2.7033 0.0616 0.9635
Data4 MLE 0.8548 0.2995 1.7155 0.0470 0.9980
LSE 1.0035 0.3514 1.5885 0.0386 0.9999
Data5 MLE 16.8042 1.0771 0.2799 0.0881 0.9463
LSE 0.6613 0.0505 1.3798 0.0791 0.9787

9 Concluding remarks

In this article, we discuss a novel three-parameter lifespan distribution known as the sine power Burr X (SPB-X) distribution. The suggested distribution is derived from the sine-G class of distributions and the power Burr-X distribution. The suggested distribution encompasses several features, including explicit formulations for the quantile function, Bowley skewness, Moors kurtosis, ordinary moments, generating function, and incomplete and conditional moments, with several numerical and graphical representations. Several notable reliability measures for the SPB-X model include standard reliability functions, mean residual life function, mean waiting time function, residual moment, and inverted residual life. Several critical risk metrics for the SPB-X distribution. Risk measurements include the value at risk, projected shortfall, TVaR, TV, and TVP. Four estimation strategies were used to determine the model parameters: maximum likelihood, least squares, MPS, and Bayesian. A simulation study is conducted to evaluate the efficacy of estimating techniques. Ultimately, five actual datasets are examined to assess the utility and adaptability of the suggested approach. The limitation of this article lies in estimating the parameters of the SPB-X model using the complete samples only. This reason opens the door for future studies to study the estimation of the parameters of the new distribution using different censored schemes for the censored data.

  1. Funding information: This work was supported and funded by the Deanship of Scientific Research at Imam Mohammad Ibn Saud Islamic University (IMSIU) (grant number IMSIU-DDRSP2502).

  2. Author contribution: All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Data availability statement: The data that support the findings of this study are available on request from the corresponding author. The data are not publicly available due to privacy or ethical restrictions.

References

[1] Eugene N, Lee C, Famoye F. Beta-normal distribution and its applications. Commun Stat Theory Methods. 2002;31(4):497–512. 10.1081/STA-120003130Suche in Google Scholar

[2] Cordeiro GM, de Castro M. A new family of generalized distributions. J Stat Comput Simulat. 2011;81(7):883–98. 10.1080/00949650903530745Suche in Google Scholar

[3] Alzaatreh A, Lee C, Famoye F. A new method for generating families of continuous distributions. Metron. 2013;71:63–79. 10.1007/s40300-013-0007-ySuche in Google Scholar

[4] Hassan AS, Elgarhy M, Shakil M. Type II half-Logistic family of distributions with applications. Pakistan J Stat Operat Res. 2017;13(2):245–64. 10.18187/pjsor.v13i2.1560Suche in Google Scholar

[5] Al-Marzouki S, Jamal F, Chesneau Ch, Elgarhy M. Topp-Leone odd Fréchet generated family of distributions with applications to COVID-19 data sets. Comput Model Eng Sci. 2020;125(1):437–58. 10.32604/cmes.2020.011521Suche in Google Scholar

[6] Kumar D, Singh U, Singh SK. A new distribution using sine function its application to bladder cancer patients data. J Stat Appl Pro. 2015;4(3):417–27. Suche in Google Scholar

[7] Souza L, Junior WRO, de Brito CCR, Chesneau C, Ferreira TAE, Soares L. Generalproperties for the Cos-G class of distributions with applications. Eurasian Bull Math. 2019;2:63–79. Suche in Google Scholar

[8] Chesneau C, Jamal F The sine Kumaraswamy-G family of distributions. J Math Ext. 2021;15:1–33. Suche in Google Scholar

[9] Al-Babtain AA, Elbatal I, Chesneau C, Elgarhy M. Sine Topp-Leone-G family of distributions: theory and applications. Open Phys. 2020;18:574–93. 10.1515/phys-2020-0180Suche in Google Scholar

[10] Souza L, Junior WRO, de Brito CCR, Chesneau C, Ferreira TAE, Fernandes LR. Tan-G class of trigonometric distributions and its applications. Cubo. 2021;23:1–20. 10.4067/S0719-06462021000100001Suche in Google Scholar

[11] Wenjing H, Afify Z, Goual H. The arcsine exponentiated-X family: validation andinsurance application. Complexity. 2020;2020:1–18. 10.1155/2020/8394815Suche in Google Scholar

[12] Burr IW. Cumulative frequency functions. Ann Math Stat. 1942;13(2):215–32. 10.1214/aoms/1177731607Suche in Google Scholar

[13] Raqab MZ, Kundu D. Burr type X distribution: Revisited. J Probabil Stat Sci. 2006;4:179–93. Suche in Google Scholar

[14] Surles JG, Padgett WJ. Inference for reliability and stress-strength for a scaled Burr type X distribution. Lifetime Data Anal. 2001;7:187–200. 10.1023/A:1011352923990Suche in Google Scholar PubMed

[15] Algarni A, Almarashi AM, Elbatal I, Hassan AS, Almetwally EM, Daghistani AM, et al. Type I half logistic Burr XG family: Properties, Bayesian, and non-Bayesian estimation under censored samples and applications to COVID-19 data. Math Problems Eng. 2021;2021:5461130. 10.1155/2021/5461130Suche in Google Scholar

[16] Abonongo J, Mwaniki IJ, Aduda JA. Cosine Fréchet loss distribution: properties, actuarial measures and insurance applications. Comput J Math Stat Sci. 2024;3(1):1–32. 10.21608/cjmss.2023.240185.1019Suche in Google Scholar

[17] Bantan RAR, Chesneau C, Jamal F, Elbatal I, Elgarhy M. The truncated Burr X-G family of distributions: Properties and applications to actuarial and financial data. Entropy 2021;23:1088. 10.3390/e23081088Suche in Google Scholar PubMed PubMed Central

[18] Suleiman AA, Daud H, Singh NSS, Ishaq AI, Othman M. A new odd beta prime-Burr X distribution with applications to petroleum rock sample data and COVID-19 mortality rate. Data. 2023;8:143. 10.3390/data8090143Suche in Google Scholar

[19] Soliman D, Hegazy MA, AL-Dayian GR, EL-Helbawy AA. Statistical properties and applications of a new truncated Zubair-generalized family of distributions. Comput J Math Stat Sci. 2025;4(1):222–57. 10.21608/cjmss.2024.322714.1073Suche in Google Scholar

[20] Khan MS, King R, Hudson IL. Transmuted Burr type X distribution with covariates regression modeling to analyze reliability data. Am J Math Manag Sci. 2020;39:99–121. 10.1080/01966324.2019.1605320Suche in Google Scholar

[21] Elbatal IA, Helal TS, Elsehetry AM, Elshaarawy RS. Topp-Leone Weibull generated family of distributions with applications. J Business Environ Sci. 2022;1(1):183–95. 10.21608/jcese.2022.270143. Suche in Google Scholar

[22] Usman RM, Ilyas M. The power Burr Type X distribution: Properties, regression modeling and applications. Punjab Univ J Math. 2020;52:27–44. Suche in Google Scholar

[23] Butt NS, Khalil MG. A new bimodal distribution for modeling asymmetric bimodal heavy- tail real lifetime data. Symmetry. 2020;12:2058. 10.3390/sym12122058Suche in Google Scholar

[24] Usman RM, Handique L, Chakraborty S. Some aspects of the odd log-logistic Burr X distribution with applications in reliability data modeling. Int J Appl Math Stat. 2019;58:127–47. Suche in Google Scholar

[25] Shrahili M, Elbatal M, Muhammad M. The type I half-logistic Burr X distribution: Theory and practice. J Nonlinear Sci Appl 2019;12:262–77. 10.22436/jnsa.012.05.01Suche in Google Scholar

[26] Abdullah ZM, Khaleel MA, Abdal-hameed MK, Oguntunde PE. Estimating parameters for extension of Burr type X distribution by using conjugate gradient in unconstrained optimization. Kirkuk Univ. 2019;14:33–49. 10.32894/kujss.2019.14.3.4Suche in Google Scholar

[27] Khaleel MA, Ibrahim NA, Shitan M, Merovci F. New extension of Burr type X distribution properties with application. J King Saud Univ Sci. 2018;30(4):450–7. 10.1016/j.jksus.2017.05.007Suche in Google Scholar

[28] Madaki UY, Abu Bakar MR, Handique L. Beta Kumaraswamy Burr type X distribution and its properties. Preprints 2018;2018080356. 10.20944/preprints201808.0356.v1Suche in Google Scholar

[29] Ishaq A, Usman A, Tasi’u M, Aliyu Y. Weibull-Burr type x distribution: Its properties and application. Niger. 2017;16:150–7. Suche in Google Scholar

[30] Al-Saiari AY, Baharith LA, Mousa SA. New extended burr type X distribution. Sri Lankan J Appl Stat. 2016;17:217–31. 10.4038/sljastats.v17i3.7904Suche in Google Scholar

[31] Khaleel MA, Ibrahim NA, Shitan M, Merovci F. Some properties of Gamma Burr type X distribution with application. In Proceedings of the AIP Conference Proceedings, Yogyakarta, Indonesia, 25–26 January 2016; p. 020087. 10.1063/1.4952567Suche in Google Scholar

[32] Merovci F, Khaleel MA, Ibrahim NA, Shitan M. The beta Burr type X distribution properties with application. SpringerPlus. 2016;5:697. 10.1186/s40064-016-2271-9Suche in Google Scholar PubMed PubMed Central

[33] Hassan OHM, Elbatal I, Al-Nefaie AH, Elgarhy M. On the Kavya-Manoharan-Burr X model: estimations under ranked set sampling and applications. J Risk Financial Manag. 2023;16:19. 10.3390/jrfm16010019Suche in Google Scholar

[34] Kenney FJ, Keeping SE. Mathematics of statistics. NJ: Princeton; 1962. Suche in Google Scholar

[35] Moors AJ. A quantile alternative for Kurtosis. J R Stat Soc D. 1998;37:25–32. 10.2307/2348376Suche in Google Scholar

[36] Artzner P. Application of coherent risk measures to capital requirements in insurance. North Am Actuarial J. 1999;3(2):11–25. 10.1080/10920277.1999.10595795Suche in Google Scholar

[37] Artzner P, Delbaen F, Eber J-M, Heath D. Thinking coherently. Risk. 1997;10(11):14. Suche in Google Scholar

[38] Artzner P, Delbaen F, Eber J-M, Heath D. Coherent measures of risk. Math Fin. 1999;9(3):203–28. 10.1111/1467-9965.00068Suche in Google Scholar

[39] Landsman Z. On the tail mean-variance optimal portfolio selection. Insur Math Econ. 2010;46:547–53. 10.1016/j.insmatheco.2010.02.001Suche in Google Scholar

[40] Cordeiro GM, Lemonte AJ. The β-Birnbaum-Saunders distribution: An improved distribution for fatigue life modeling. Comput Stat Data Anal. 2011;55(3):1445–61. 10.1016/j.csda.2010.10.007Suche in Google Scholar

[41] Kundu D, Raqab MZ. Estimation of R=P(Y<X) for three-parameter Weibull distribution. Stat Probab Lett. 2009;79(17):1839–46. 10.1016/j.spl.2009.05.026Suche in Google Scholar

[42] Alyami SA, Elbatal I, Alotaibi N, Almetwally EM, Elgarhy M. Modeling to factor productivity of the United Kingdom food Chain: using a new lifetime-generated family of distributions. Sustainability. 2022;14(14):8942. 10.3390/su14148942Suche in Google Scholar

[43] Shah A, Gokhale DV. On maximum product of spagings (mps) estimation for burr xii distributions: On maximum product of spagings. Commun Stat-Simulat Comput. 1993;22(3):615–41. 10.1080/03610919308813112Suche in Google Scholar

[44] Shao Y, Hahn MG. Maximum product of spacings method: A unified formulation with illustration of strong consistency. Illinois J Math. 1999;43(3):489–99. 10.1215/ijm/1255985105Suche in Google Scholar

[45] Husain QN, Qaddoori AS, Noori NA, Abdullah KN, Suleiman AA, Balogun OS. New expansion of Chen distribution according to the nitrosophic logic using the Gompertz family. Innovat Stat Probab. 2025;1(1):60–75. 10.64389/isp.2025.01105Suche in Google Scholar

[46] Noori NA, Khaleel MA, Khalaf SA, Dutta S. Analytical modeling of expansion for odd Lomax generalized exponential distribution in framework of neutrosophic logic: a theoretical and applied on neutrosophic data. Innovat Stat Probab. 2025;1(1):47–59. 10.64389/isp.2025.01104. Suche in Google Scholar

[47] Onyekwere CK, Aguwa OC, Obulezi OJ. An updated lindley distribution: properties, estimation, acceptance sampling, actuarial risk assessment and applications. Innovat Stat Probab. 2025;1(1):1–27. 10.64389/isp.2025.01103. Suche in Google Scholar

[48] Gemeay AM, Moakofi T, Balogun OS, Ozkan E, Hossain MM. Analyzing real data by a new heavy-tailed statistical model. Modern J Stat. 2025;1(1):1–24. 10.64389/mjs.2025.01108. Suche in Google Scholar

[49] Sapkota LP, Kumar V, Tekle G, Alrweili H, Mustafa MS, Yusuf M. Fitting real data sets by a new version of Gompertz distribution. Modern J Stat. 2025;1(1):25–48. 10.64389/mjs.2025.01109. Suche in Google Scholar

[50] El-Sherpieny ESA, Almetwally EM, Muhammed HZ. Progressive type-II hybrid censored schemes based on maximum product spacing with application to power Lomax distribution. Phys A Stat Mech Appl. 2020;553:124251. 10.1016/j.physa.2020.124251Suche in Google Scholar

[51] Alshenawy R, Sabry MA, Almetwally EM, Almongy HM. Product spacing of stress-strength under progressive hybrid censored for exponentiated-gumbel distribution. Comput Materials Continua. 2021;66(3):2973–95. 10.32604/cmc.2021.014289Suche in Google Scholar

[52] Weibull W. A: statistical distribution function of wide applicability. J Appl Mech. 1951;18:293–7. 10.1115/1.4010337. Suche in Google Scholar

[53] Thom HC. A note on the gamma distribution. Monthly Weather Rev. 1958;86(4):117–22. 10.1175/1520-0493(1958)086<0117:ANOTGD>2.0.CO;2Suche in Google Scholar

[54] Nadarajah S, Cordeiro GM, Ortega EM. The exponentiated Weibull distribution: a survey. Stat Papers. 2013;54:839–77. 10.1007/s00362-012-0466-xSuche in Google Scholar

[55] Cordeiro GM, Gomes AE, da-Silva CQ, Ortega EM. A useful extension of the Burr III distribution. J Stat Distributions Appl. 2017;4:1–15. 10.1186/s40488-017-0079-ySuche in Google Scholar

[56] Lim JT, Azizan AS. Weather and climate of Malaysia. Kuala Lumpur: University of Malaya Press; 2004. Suche in Google Scholar

[57] Ruzhansky M, Cho YJ, Agarwal P, Area I (Eds.). Advances in real and complex analysis with applications. Singapore: Springer; 2017. 10.1007/978-981-10-4337-6Suche in Google Scholar

[58] Butt SI, Sayyari Y, Agarwal P, Nieto JJ, Umar M. On some inequalities for uniformly convex mapping with estimations to normal distributions. J Inequal Appl. 2023;2023: 89. 10.1186/s13660-023-02997-z. Suche in Google Scholar

[59] Tierney L. Markov chains for exploring posterior distributions. Ann Stat. 1994;22(4):1701–28. 10.1214/aos/1176325750Suche in Google Scholar

[60] Suhaila J, Sayang MD, Jemain AA. Revised spatial weighting methods for estimation of missing rainfall data. Asia Pac J Atmos Sci. 2008;44:93–104. Suche in Google Scholar

[61] Wijngaard JB, Klein Tank AMG, Konnen GP. Homogeneity of 20th century European daily temperature and precipitation series. Int J Climatol 2003;23:679–92. 10.1002/joc.906Suche in Google Scholar

[62] Suhaila J, Deni SM, Wan Zin WZ, Jemain AA. Spatial patterns and trends of daily rainfall regime in Peninsular Malaysia during the southwest and northeast monsoons: 1975–2004. Meteorol Atmos Phys. 2010;110:1–18. 10.1007/s00703-010-0108-6Suche in Google Scholar

Received: 2024-10-10
Revised: 2025-09-27
Accepted: 2025-10-01
Published Online: 2025-11-07

© 2025 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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