TOPP-LEONE EXPONENTIATED GOMPERTZ INVERSE RAYLEIGH DISTRIBUTION: PROPERTIES AND
APPLICATIONS
Sule Omeiza Bashiru1, Alaa Abdulrahman Khalaf2 and Alhaji Modu Isa3
department of Mathematics and Statistics, Confluence University of Science and Technology,
Osara, Kogi State, Nigeria.
2Diyala Education Directorate, Diyala, Iraq.
3Department of Mathematics and Computer Science, Borno State University, Nigeria.
Email: [email protected]; [email protected]; [email protected]
Abstract
This paper focused on deriving a new lifetime distribution having five parameters by compounding the Gompertz inverse Rayleigh model and the Topp-Leone exponentiated-G family of distributions. The new model is called Topp-Leone exponentiated Gompertz inverse Rayleigh (TLEGoIRa) distribution. The new model is very flexible and the shape of its pdf can be positively or negatively skewed and symmetric. Some statistical characteristics of the new model, such as the moments, incomplete moments, quantile function, renyi entropy and order statistics are derived and investigated. The pdf of the minimum and maximum order statistics of the new model were derived and studied. The model's parameters are estimated using the maximum likelihood approach. A simulation study was conducted to investigate the consistency of the newly proposed model, using the average bias and root mean square error (RMSE) as metrics. The outcome of the simulation suggested that as sample sizes increase, both the average bias and root mean square error (RMSE) decrease, indicating that the distribution is consistent. Finally, two real-life datasets were used to explore the new model's importance and adaptability in comparison to other competing models The results of the application revealed that the new distribution outperforms its competitors.
Keywords: Toppleone Exponentiated G., Gompertz Inverse Rayleigh, Quantile Function, Order Statistics, MLE.
I. Introduction
In the realm of distribution theory, the pursuit of developing models that accurately reflect the prevailing trends across various disciplines has proven challenging. Classical distributions, which form the foundation, often lack the required flexibility and robustness. This inherent limitation has spurred researchers within the distribution theory field to undertake the task of extending or generalizing existing distributions. The overarching goal is to imbue these distributions with greater flexibility and resilience, enabling them to effectively capture the evolving patterns present in datasets originating from diverse fields like engineering, environmental sciences, biological sciences, medical sciences, and beyond.
This process of extension or generalization entails the introduction of one or more additional parameters to the existing distributions. Contemporary approaches to distribution generalization frequently involve the utilization of distribution families. Examples of these families include the Topp-Leone exponentiated-G distribution by [1], Topp-Leone Kumaraswamy-G distribution by [2], Topp-Leone-G distribution by [3], type II half logistic-G distribution by [4], type I half logistic exponentiated-G distribution by [5], type II half logistic exponentiated-G distribution by [6], transmuted exponentiated generalized G distribution by [7], Topp-Leone odd Lindley G distribution by [8], and Topp-Leone Gompertz-G distribution by [9], among others. These families are constructed by introducing supplementary shape parameter(s) to the foundational distribution, thereby augmenting the efficacy and practicality of data modeling.
One significant continuous probability distribution, referred to as the inverse Rayleigh (IRa) distribution, was initially introduced by [10] and has since found extensive application in modeling system failure times. Notably, the IRa distribution is a specialized form of the broader inverse Weibull (IW) distribution. The statistical literature offers various adaptations and extensions of the IRa distribution, which can be explored further through references such as [11-13]. An extension of particular interest is the Gompertz inverse Rayleigh (GoIRa) distribution, developed by [14], which is considered as the baseline distribution in this study. Through the extension of the GoIRa distribution, we aim to develop a more adaptable compound distribution.
Reference [1] introduced the TLE-G, a distinct family of continuous distributions with the cumulative distribution function (cdf ) and probability density function (pdf ) given as:
F(x,d,a) =
2\ S
l-(l-G {X '¿J)
(1)
fx, e,a) = 2 eag (x x)c(x x)a-1 (l-G (x xf )f 1 -(l -G (x xf )' 1
(2)
The cdf and pdf corresponding to the baseline Gompertz inverse Rayleigh (GoIRa) distribution are given as:
G(x ,,',) = 1-e and
gx ,y,P,l) = 2yl2
rn2
1-
1-e
-'1
1- I J
(3)
(4)
Where A> 0 is the scale parameter and y,' > 0 are the shape parameters respectively.
The primary objective of this research is to utilize the GoIRa distribution as a foundational model within the TLE-G framework, aiming to develop a novel extension known as the TLEGoIRa distribution. This extension seeks to enhance the flexibility and applicability of the GoIRa distribution in capturing complex data patterns across various fields.
The remaining content of this article is organized as follows: Section 2 presents the development of the TLEGoIRa distribution, including the derivation of its properties and the method for estimating its parameters. Section 3 discusses simulation studies conducted to investigate the consistency of the estimates and the application of the model to two real datasets to demonstrate the practical potential of the new distribution. Finally, Section 4 provides concluding remarks.
II. Methods
2.1 Development of Topp-Leone Exponentiated Gompertz Inverse Rayleigh
(TLEGoIRa) Distribution
To derive the cdf of the new model, equation (3) is inserted into equation (1) as:
x,d,a,y,ß,l
1 -
1 -
1-e
rn2 y
1-
(5)
To derive the PDF of the new model, equations (3) and (4) are inserted into equation (2) as follows:
' f ,.2-»)i ( i
f
f
x,Q,a,y,ß,X
= 4ydaX2x-3e u
2
Yß-1
1-e
v
ß
1-e e*
V 1
1-e
1
V 1
1 -
1-e
r i y x2 2 -ßß
1- 1-e W
V V
1
e-1
(6)
1 -
1 -
1-e
f -ßß
1- 1-e UJ
V V
1
1 1 V V
where x > 0, and 0, a, X p, y > 0.
The hazard function for the TLEGoIRa distribution can be obtained using this expression:
f
x, e,a,y,ß,X
x,e,a,y,ß,l
1-F
x,d,a,y,p,X
\ V
The pdf and hazard function plots of the TLEGoIRa distribution are given figures 1 and 2 below:
Figure 1: pdf plots of the TLEGoIRa distribution with different parameter values
Figure 2: hazard function plots of the TLEGoIRa distribution with different parameter values
2.2 Statistical Properties of the TLEGoIRa Distribution
This section derives some statistical properties of the TLEGoIRa distribution including moments, survival function, hazard function, quantile functions, and order statistics.
2.2.1 Moment
The rth moment of the TLEGoIRa model is computed using the following expression:
r = * X r)=f-rf
x ,в, а, -, ß , y
dx
V
— q œ z
First expanding equation (6) by using generalized binomial expansion [l + u] = ^(-1 )
u,
V
U9=±(-i)z
г -,-a "По + w)
, С1-"] =X lw:M<iqq0. [15-16]
=0 w\T(q)
i -
i -
чЛв
J- 1- 1-е 1 в
1-е
(в-1 ^
да
■IM'
1 -
1-е
вЛа
And
1 -
1-e
'И +1
да
=1К
j=0
1-е
\а/
Again, using the generalized binomial expansion and the exponential expansion formula
[17]
c=0 C •
Then we get expansion pdf of TLEGoIRa distribution: f \
f
x, в, а, y, ß, -
= wx2e
r p
V+1)1 -
V
Where
¥p= 4ваГ-2 X
/=/=k=m =w==g=0
Hence,
r=e x 'r=p?
(-1)
fa\
i+j+k kw+q
m\
<2i + ^ (
v /
а
j 1)-1
VmV
w
-ß{1 + w)-1
q
-c?+1)1-
dx
On solving the integral part in the equation above, then the fir is:
(7)
/ur = e {x x = vt
—T(1 - 2)
q+1)1-r
(8)
2.2.2 Incomplete Moments
Equation (7) yields the incomplete moments for the TLEGoIRa distribution with rth (r > 0). [18-19]
xr3e u> dx
Let t = (q +1)| — | ^>x =
(.q+1)—2
V /
When x = 0 =>t = 0, and if x = u^> t = (q +1)| — | , then
UU
W
2-{(c[ +1)—2 )1
1 - 2,(q + 1)—2
(9)
2.2.3 Quantile Function
The quantile function of TLEGoIRa distribution is given as
x = Q (u) = —
-log
( f
1-
1-
ß
log
f 1\ ( 1 W 1-ue V )
1\ 1 WW
1-
V V
J)
(10)
The median of TLEGoIRa distribution is obtained by setting u = 0.5 in equation (10)
median
((o.5) = —
-log
1 ^
( ( 1 W
( 1Y
( 1W
1 -
1 -
Y
1 -
1 -(0.5)e
V V
Table 1: Quantiles for given parameter values of the TLEGoIRa distribution.
(9, A, a, ß, y)
U (0.4, 0.8, 1.2, 1.3, 2.2) (3, 1.3, 0.9, 0.7, 3.3) (2.3, 3, 1.7, 1.4, 1.2)
0.1 0.45276 0.59975 1.33661
0.2 0.52743 0.63546 1.41855
0.3 0.59314 0.66110 1.48066
0.4 0.65832 0.68289 1.53586
0.5 0.72712 0.70315 1.58933
0.6 0.80314 0.72329 1.64475
0.7 0.89111 0.74472 1.70628
0.8 0.99973 0.76965 1.78139
0.9 1.15324 0.80387 1.89139
2.2.4 Renyi Entropy
Define the Renyi entropy of the TLEGoIRa distribution using the following formula. [20] Tr(t) = 0gjg" fT(x)dx , t > 0t 1
By substitution equation (7) into the equation above:
( l
T(T) = -—log
1 - T
V f
, -Y1)1, ,
x-xe V1 dx
The last integral, we get
tr(t) = q log
1 - T
pH (t- 1)+1
(( l i2(3T+1)
++1
T-
V ^ / 1 1
(11)
2.2.5 Order Statistic
The pdf of the order statistics for the TLEGoIRa distribution is obtained as follows: [21-24]
gtn W = (t-Hn-tyi"W)]" t1 "" " Ml^ f W
Substituting equations (5) and (6) into equation (12), we have:
g,Jx)
(t-1)!U t)!
1- 1-e
1- 1-e
L-
(13)
4y0aÂ'X3e[*J 1-e w e
1-e
1- 1-e
Je
1-1-
1-e
2.3 Maximum Likelihood Estimation (MLE)
This section provides the method of estimation of the unknown parameters of the TLEGoIRa distribution. Suppose that x1, x2,..., xn be nth independent random sample from the TLEGoIRa distribution. Then, the log-likelihood function of the TLEGoIRa distribution is given as:
log I = lg(4) + nlog(0} + nlogga ) + n Ioggy) + 2nIoggx)-3£ log(* .)-Ä2
i=1 v x, (
-(ß + 1)£log
1-e
((
+ -Élog ßi
1-e
Xß
-(a- 1)^log
1-e
(14)
2
"Zlog
1 -
1-e
-(O- 1)£log
1 -
1-e
Differentiating equation (14) with respect to each unknown parameter and equating them zero, we have:
(
d(l=- . + Ï log
dO
f
1 -
1 -
( ( ( . ,2vß^
1- 1-e
ß
1-e
2 A
(15)
l
5a a i
£ log
1-e
1-e
log
1-e
1 -
1 — e
+2(e-1) £
i -
1-e
1-e
Y f
log
1-e
1 -
1 -
1 — e
f -ßl
- 1-e ^ xii
(16)
ln±z log 1-I1 -
dy Y ßi
-ßll
-1)£e
1-e
1-e
1- 1-e
+2a(e -1)£
1 -
1-e
/ -.2 -ßß
( - 1
1- 1-e Vi
ß Y
1-e
1 -
1 -
1-e
/ -.2 -ßl
( - 1
1- 1-e
(17)
£i4=2£--2X(p + -
dX X v I \H ( (,A2 A
( ( A2 A-(P+l)
2X/£ l-fl
l-e
V )
V )
( ( ( .2vlV
y i- e
+ 2Xp(a- l)^e
i'f 2
l- Y l eXi
P
1-e
l-e
-2Xf3aY}
l-e
l-e
l-e
l-e
(18)
dp
( X A ( -(Ai A -p ( -(4 A
¿log i = l l-e VX + Y ± pil l-e x log l-e x
V )
V )
V )
l-e
( A log e1
V )
l - l-e
( -(X2 A log ex
V_)
l-e
-2«(0-l)£-
i=l
l -
l-e
l-e
f ( , A2 A
log
l -
l-e
Since equations (15), (16), (17), (18), and (19) are non-linear in parameters, an iterative technique is resorted to using Newton-Raphson iterative algorithm to obtain the estimate of the parameters.
III. Results
3.1 Simulation
This section describes the conclusions of a simulation research of the TLEGoIRa distribution. The study investigates five distinct sets of parameter values: (9 =0.9, a =1.2, y =0.3, p =0.3, X=0.5), (9 =1.2, a =0.9, y =0.7, p =0.3, X=0.5), (9 =1.3, a =1.3, y =0.8, ( =0.6, X=0.4), and (9 =2, a =2, y =0.6, ( =0.75, X=0.2). Each parameter set yields 1000 samples, with n = 50, 100, 150, and 300. We utilize these samples to compute the mean, average bias, and root mean square error (RMSE). To calculate bias and RMSE for the calculated parameters, use the formulas below:
N ijN 2"
xa, — °c)
Abias{cc) = ——--cc, and RMSE(cc) = =—-—-.
Tables 2 and 3 illustrate the results, which demonstrate a clear pattern: as the sample size increases, the mean parameter estimates get more precise and closer to the true values. Simultaneously, the corresponding RMSEs and Abias approach zero, proving MLEs' reliability and consistency.
Table 2: Results from Monte Carlo simulations of the TLEGoIRa distribution
9 =0.9, a =1.2, y =0.3, ß =0.3, 1=0.5 9 =1.2, a =0.9, y =0.7, ß =0.3, 1=0.5
Parameter N Mean RMSE Abias Mean RMSE Abias
0 50 3.3963 4.9674 2.4963 3.7293 3.6574 2.5293
100 2.2823 2.9373 1.3823 3.7169 3.3882 2.5169
150 1.9920 2.1471 1.0920 3.1464 2.3203 1.9464
300 1.5072 1.4519 0.6072 2.2718 2.2284 1.0718
a 50 1.1618 1.3257 0.0981 1.1671 1.6299 0.2671
100 1.2951 1.1776 0.0951 1.1055 1.3425 0.2055
150 1.1993 1.1490 0.0644 1.1023 1.3182 0.2060
300 1.3244 1.0653 0.0455 1.0609 1.0041 0.1609
Y 50 0.2144 0.1879 0.0855 0.5295 0.6465 0.1704
100 0.2459 0.1461 0.0540 0.5168 0.4134 0.1531
150 0.2632 0.1382 0.0367 0.5023 0.3071 0.1276
300 0.2599 0.1155 0.0200 0.4994 0.2535 0.1005
ß 50 0.3311 0.1891 0.0396 0.3246 0.2079 0.0246
100 0.3274 0.1864 0.0374 0.3136 0.1747 0.0136
150 0.3233 0.1581 0.0240 0.2956 0.1504 0.0043
300 0.3209 0.1324 0.0233 0.3020 0.1368 0.0020
X 50 0.9800 0.9588 0.4800 1.9086 1.6432 1.4086
100 0.8343 0.6752 0.3343 1.2474 1.4809 0.7474
150 0.7453 0.5092 0.2453 0.9105 1.0670 0.4105
300 0.6237 0.3144 0.1237 0.7456 0.5470 0.2456
Table 3: Results from Monte Carlo simulations of the TLEGoIRa distribution
6 =1.3, a =1.3, Y =0.8, ß =0.6, 1=0.4 6 =2, a =2, y =0.6, ß =0.75, 1=0.2
Parameter N Mean RMSE Abias Mean RMSE Abias
0 50 3.9020 3.2589 2.6020 4.6867 4.6171 2.6867
100 3.1574 2.2916 1.8574 3.9532 3.5984 1.9532
150 2.7310 2.6574 1.4310 3.4859 2.7741 1.4859
300 2.9938 1.1012 0.6938 3.0303 2.0658 1.0303
a 50 1.5031 2.1812 0.2031 2.2077 3.9702 0.2077
100 1.4930 2.1254 0.3930 2.6847 3.9583 0.0847
150 1.4756 2.0739 0.2756 2.0827 3.9374 0.0827
300 1.3273 1.3373 0.2273 2.4920 3.0661 0.0720
Y 50 0.7726 1.0620 0.9709 0.4879 0.3450 0.1920
100 0.7423 0.5469 0.1073 0.4565 0.2704 0.1434
150 0.7259 0.4181 0.0976 0.4367 0.2280 0.1132
300 0.7016 0.3897 0.0594 0.5271 0.1969 0.0728
ß 50 0.7850 0.5824 0.1850 1.3345 1.2143 0.5845
100 0.7450 0.5133 0.1450 1.2569 1.1121 0.5069
150 0.7342 0.4793 0.1342 1.3577 1.1337 0.4877
300 0.6869 0.4226 0.0869 1.1989 0.9787 0.4489
50 2.0712 2.7215 1.6719 1.0376 1.9009 0.8376
100 1.3579 2.1418 0.9579 0.6940 1.0649 0.4940
150 0.9976 1.3302 0.5976 0.6385 0.9570 0.4385
300 0.7083 0.7030 0.3083 0.4223 0.4678 0.2223
3.2 Applications
In this section, the practical use of the TLEGoIRa distribution is explored via two real-life data sets. Table 4 displays the cdf of the models, which will be compared to the TLEGoIRa distribution.
Table 4: CDF for the Comparative distributions
Distribution CDF
Truncated Exponentiated Exponential Gompertz inverse Rayleigh (TEEGoIRa) [15] f f 1-exp V v f -0 V f Y 1-e V f f ¥ - 1- 1-e K"> Tßiy A v y J
(l-exp{-0))a
Beta Gompertz inverse Rayleigh (BeGoIRa) (New) pbeti f f f Y 1-ß 1-e e v V x il 1-e 1x 0,a
Kumaraswamy Gompertz inverse Rayleigh (KuGoIRa) (New)
Exponential Generalized Gompertz inverse Rayleigh (EGGoIRa) (New)
Weibull Gompertz inverse Rayleigh (WeGoIRa) (New)
(
1 -
(
1 -
1-e
(312
1-
1-
1- 1-e
m2
1- 1( x J
1 -exp
( i
-log
1- 1-e
1- I j
W
The first dataset (I), shows the tensile strength in GPa of 69 carbon fibers evaluated at 20mm gauge lengths. It was utilized by Bader and Priest [25]
(1.312, 1.314, 1.479 ,1.552,1.700 ,1.803, 1.861 ,1.865 ,1.944, 1.958 ,1.966, 1.997 ,2.006, 2.021 ,2.027, 2.055, 2.063 ,2.098, 2.140, 2.179 ,2.224 ,2.240, 2.253 ,2.270, 2.272, 2.274, 2.301, 2.301 ,2.359 ,2.382 ,2.382 ,2.426 ,2.434, 2.435, 2.478 ,2.490, 2.511, 2.514, 2.535 ,2.554, 2.566, 2.570, 2.586, 2.629 ,2.633, 2.642, 2.648, 2.684 ,2.697, 2.726, 2.770, 2.773, 2.800, 2.809, 2.818, 2.821, 2.848 ,2.880, 2.954, 3.012, 3.067 ,3.084, 3.090, 3.096, 3.128, 3.233, 3.433 ,3.585, 3.585).
The second dataset (II), shown here represents COVID-19 mortality rate data for Mexico over a 108-day period from March 4th to July 20, 2020. It was utilized by Almongy et al. [26]
(8.826, 6.105 ,10.383, 7.267 ,13.220, 6.015 ,10.855, 6.122 ,10.685, 10.035, 5.242 ,7.630 ,14.604 ,7.903 ,6.327 ,9.391 ,14.962 ,4.730 , 3.215 ,16.498, 11.665 ,9.284, 12.878, 6.656,3.440 ,5.854, 8.813 , 10.043, 7.260, 5.985, 4.424 ,4.344 ,5.143 ,9.935 ,7.840 ,9.550 , 6.968 ,6.370 ,3.537 ,3.286 ,10.158, 8.108 ,6.697 ,7.151 ,6.560 , 2.988 ,3.336 ,6.814 ,8.325 ,7.854 ,8.551 ,3.228, 3.499 ,3.751, 7.486 ,6.625 ,6.140 ,4.909 ,4.661 ,1.867 ,2.838 ,5.392, 12.042, 8.696 ,6.412 ,3.395 ,1.815 ,3.327 ,5.406 ,6.182 ,4.949 ,4.089 , 3.359 ,2.070, 3.298 ,5.317 ,5.442 ,4.557 ,4.292 ,2.500 ,6.535 , 4.648 ,4.697 ,5.459 ,4.120, 3.922 ,3.219, 1.402 ,2.438, 3.257 , 3.632, 3.233 ,3.027, 2.352 ,1.205 ,2.077, 3.778, 3.218, 2.926, 2.601, 2.065, 1.041, 1.800, 3.029, 2.058, 2.326, 2.506, 1.923).
Tables 5, and 6 for data (I), and (II) show that the TLEGoIRa distribution beats Comparative distributions in several key criteria, including Akaike information criterion (AIC) , Consistent AIC (CAIC),Bayesian information criterion (BIC), Hannan-Quinn information (HQIC),Kolmogorov-Smimov (KS) ststistic, Anderson-Darling (A), and Cramer-von Mises (W) values. The lower values of these measures for the TLEGoIRa distribution are preferable for comparative distributions.
Figures 3, and 5 show the Fitted densities for Data I, and II, respectively, and Figures 4, and 5 show the empirical cdf plots for Data I and II. These visualizations enable us to evaluate the goodness of fit and see how well the model fits the data.
Table 5: Goodness-of-Fit Statistics for Data I
Dist. MLEs -2L AIC CAIC BIC HQIC W A K-S p- value
TLEGoIRa 0:1.4173 c:1.4214 5:0.1896 P :1.6041 y:2.0224 48.81 107.62 108.58 118.79 112.05 0.0178 0.1600 0.0414 0.9997
TEEGoIRa 0:0.0443 c:0.8522 5:3.3049 P :3.5479 y:4.1427 49.36 108.74 109.69 119.91 113.17 0.0356 0.2930 0.0530 0.9900
BeGoIRa 0:1.7430 c:1.0087 5:0.0292 P :0.7674 Y:1.8205 50.50 111.03 111.99 122.21 115.47 0.0165 0.1487 0.0982 0.5177
KuGoIRa 0:1.7872 c:1.0734 5:0.0238 P :0.7657 Y:1.8912 49.63 109.29 110.24 120.46 113.72 0.0164 0.1481 0.0750 0.8313
EGGoIRa 0:0.9743 c:1.7609 5:0.0223 P :0.7207 Y:1.8454 50.12 110.28 111.23 121.45 114.71 0.0165 0.1483 0.0826 0.7330
WeGoIRa 0:1.8695 c:1.0161 5:0.0322 P :0.7167 Y:1.4519 49.64 109.29 110.24 120.46 113.72 0.0308 0.2515 0.0598 0.9659
Figure 3: Fitted densities for Data I
Figure 4: Empirical cdf plot for Data I
Table 6: Goodness-of-Fit Statistics for Data II
Dist. MLEs -2L AIC CAIC BIC HQIC W A K-S P- value
TLEGoIRa 0:0.6769 c:1.4676 5:0.1046 P :2.1082 Y :0.7180 265.12 540.24 540.83 553.65 545.68 0.0357 0.2127 0.0565 0.8805
TEEGoIRa 0:0.9677 c:1.1598 5:0.0450 P :1.2991 Y :0.8986 265.62 541.25 541.84 554.66 546.69 0.0517 0.3001 0.0646 0.7577
BeGoIRa 0:1.2413 c:0.9903 5:0.0079 P :0.3841 Y :0.8618 267.77 545.54 546.13 558.95 550.98 0.0909 0.5702 0.0833 0.4415
KuGoIRa 0:1.1977 c:0.9940 5:0.0108 P :0.3686 Y :0.7788 268.42 546.85 547.44 560.26 552.29 0.0802 0.4945 0.0683 0.6936
EGGoIRa 0:0.9884 c:1.2186 5:0.0095 P :0.3768 Y :0.8146 267.83 545.66 546.25 559.07 551.10 0.0846 0.5260 0.0605 0.8236
WeGoIRa 0:1.4253 c:1.0311 5:0.1373 P :1.3555 Y:0.51167 265.26 540.56 541.15 553.97 546.00 0.0433 0.2484 0.0607 0.8208
Figure 5: Fitted densities for Data II
Figure 6: Empirical cdf plot for Data II
IV. Discussion
In this paper, we introduce a novel extension of the GoIRa model, referred to as the TLEGoIRa distribution. We provide explicit expressions for various statistical properties, including ordinary moments, incomplete moments, quantile function, renyi entropy and order statistics of the TLEGoIRa distribution. To estimate the unknown parameters, we employ the method of maximum likelihood estimation and undertake a simulation research to investigate the average bias and root mean square error (RMSE) as sample sizes rise. The results show a consistent model performance, with diminishing Abias and Rmse as the sample size grows. Furthermore, we validate the effectiveness of the proposed model through two real-life applications. Through these applications, we demonstrate that the proposed model outperforms several other competitive models in terms of goodness of fit. This empirical evidence underscores the enhanced flexibility and robustness of our novel model in accurately representing and modeling the characteristics of the given datasets when compared to the other competitive models under consideration.
References
[1] Sule I., Sani I.D., Audu I., and Jibril H.M. (2020). On the Topp Leone exponentiated-G family of distributions: Properties and applications. Asian Journal of Probability and Statistics, 7, 1-15.
[2] Sule I., Doguwa S.I., Isah A., and Jibril H.M. (2020). The Topp Leone Kumaraswamy-G Family of Distributions with Applications to Cancer Disease Data. Journal of Biostatistics and Epidemiology, 6, 37-48.
[3] Al-Shomrani A., Arif O., Shawky A., Hanif S., and Shahbaz M.Q. (2016). Topp-Leone Family of Distributions: Some Properties and Application. Pakistan Journal of Statistics and Operation Research, 12(3), 443-451.
[4] Soliman A.H., Elgarhy M.A.E., and Shakil M. (2017). Type II half logistic family of distributions with applications. Pakistan Journal of Statistics and Operation Research, 13, 245-264.
[5] Bello O.A., Doguwa S.I., Yahaya A., and Jibril H.M. (2021). A Type I Half Logistic Exponentiated-G Family of Distributions: Properties and Application. Communication in Physical Sciences, 7(3), 147-163.
[6] Bello O.A., Doguwa S.I., Yahaya A., and Jibril H.M. (2021). A Type II Half Logistic Exponentiated-G Family Of Distributions with Applications to Survival Analysis. FUDMA Journal of Sciences, 5(3), 177-190.
[7] Yousof H.M., Afify A.Z., Alizadeh M., Butt N.S., Hamedani G., and Ali M.M. (2015). The transmuted exponentiated generalized-G family of distributions. Pakistan Journal of Statistics and Operation Research, 11(4), 441-464.
[8] Reyad H., Alizadeh M., Jamal F., and Othman S. (2018). The Topp Leone odd Lindley-G family of distributions: Properties and applications. Journal of Statistics and Management Systems, 21(7), 12731297.
[9] Oluyede B., Chamunorwa S., Chipepa F., and Alizadeh M. (2022). The Topp-Leone Gompertz-G family of distributions with applications. Journal of Statistics and Management Systems, 25(6), 13991423.
[10] Voda, V. G. (1972). On the inverse Rayleigh distributed random variable, Rep. Statist. App. Res., JUSE 19: 13-21.
[11] Sule O. B., Adegoke T. M and Kayafat T.U (2021). Bayes Estimators of Exponentiated Inverse Rayleigh Distribution using Lindleys Approximation. Asian Research Journal of Mathematics, 17(2): 60 -71.
[12] Malik A., and Ahmad S. (2018). A New inverse Rayleigh distribution: Properties and application. International Journal of Scientific Research in Mathematical and Statistical Sciences, 5(5), 9296.
[13] Sule O.B., and Halid O.Y. (2023). On the properties and applications of Toppleone Gompertz Inverse Rayleigh Distribution. Reliability: Theory and Applications, 18(4), 1032-1045.
[14] Halid O.Y., and Sule O.B. (2022). A classical and Bayesian techniques for Gompertz Inverse Rayleigh Distribution. Pakistan Journal of Statistics, 38(1), 49-76.
[15] Khalaf A.A., Yusur K., and Khaleel M.A. (2023). [0, 1] Truncated Exponentiated Exponential Inverse Weibull Distribution with Applications of Carbon Fiber and COVID-19 Data. Journal of Al-Rafidain University College For Sciences, 1, 387-399.
[16] Khalaf A.A., and Khaleel M.A. (2022). [0, 1] Truncated exponentiated exponential Gompertz distribution: Properties and applications. AIP Conference Proceedings, 2394(1), 1-12.
[17] Khalaf A.A., and Khaleel M.A. (2020). Truncated Exponential Marshall-Olkin-Gompertz Distribution Properties and Applications. Tikrit Journal of Administration and Economics Sciences, 16, 483-497.
[18] Noori N.A., Khalaf A.A., and Khaleel M.A. (2023). A New Generalized Family of Odd Lomax-G Distributions: Properties and Applications. Advances in the Theory of Nonlinear Analysis and its Applications, 7(4), 01-16.
[19] Ibrahim M.Q., Khalaf A.A., Noori N.A., and Khaleel M.A. (2023). Exploring the Properties, Simulation, and Applications of the Odd Burr XII Gompertz Distribution. Advances in the Theory of Nonlinear Analysis and its Applications, 7(4), 60-75.
[20] Khalaf A.A., Ibrahim M.Q., Noori N.A., and Khaleel M.A. (2024). [0, 1] Truncated Exponentiated Exponential Burr Type X Distribution with Applications. Iraq Journal of Science, 65(8), 15.
[21] Sule O. B. (2021). A New Extended Generalized Inverse Exponential Distribution: Properties and Applications. Asian Journal of Probability and Statistics. 11(2): 30 - 46.
[22] Adegoke T.M., Oladoja O.M., Sule O.B., Mustapha A.A., Aderupatan D.E and Nzei L.C. (2023). Topp-Leone Inverse Gompertz Distribution: Properties and different estimations techniques and Applications. Pakistan Journal of Statistics. 39(4): 433 - 456.
[23] Sule O. B. and Ibrahim I.I (2023). Modeling of Reliability and Survival data with Exponentiated Generalized Inverse Lomax Distribution. Reliability: theory & applications. 18(4): 493 -501.
[24] Sule O. B. (2023). A study on the properties of a New Exponentiated Extended Inverse Exponential Distribution with applications. Reliability: theory & applications. 18(3): 59 - 72.
[25] Bader M.G., and Priest A.M. (1982). Statistical aspects of fibre and bundle strength in hybrid composites. Progress in Science and Engineering of Composites, 1129-1136.
[26] Almongy H.M., Almetwally E.M., Aljohani H.M., Alghamdi A.S., and Hafez E.H. (2021). A new extended Rayleigh distribution with applications of COVID-19 data. Results in Physics, 23, 1-9.