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Research Article | Open Access

The extended Weibull–Fréchet distribution: properties, inference, and applications in medicine and engineering

Ekramy A. Hussein1Hassan M. Aljohani2Ahmed Z. Afify3( )
Department of Statistics, Al-Azhar University, Nasr City 11651, Egypt
Department of Mathematics & Statistics, College of Science, Taif University, P.O. Box 11099, Taif 21944, Saudi Arabia
Department of Statistics, Mathematics and Insurance, Benha University, Benha 13511, Egypt
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Abstract

In this paper, a flexible version of the Fréchet distribution called the extended Weibull–Fréchet (EWFr) distribution is proposed. Its failure rate has a decreasing shape, an increasing shape, and an upside-down bathtub shape. Its density function can be a symmetric shape, an asymmetric shape, a reversed-J shape and J shape. Some mathematical properties of the EWFr distribution are explored. The EWFr parameters are estimated using several frequentist estimation approaches. The performance of these methods is addressed using detailed simulations. Furthermore, the best approach for estimating the EWFr parameters is determined based on partial and overall ranks. Finally, the performance of the EWFr distribution is studied using two real-life datasets from the medicine and engineering sciences. The EWFr distribution provides a superior fit over other competing Fréchet distributions such as the exponentiated-Fréchet, beta-Fréchet, Lomax–Fréchet, and Kumaraswamy Marshall–Olkin Fréchet.

CLC number: 60E05, 62F10

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AIMS Mathematics
Pages 225-246

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Cite this article:
Hussein EA, Aljohani HM, Afify AZ. The extended Weibull–Fréchet distribution: properties, inference, and applications in medicine and engineering. AIMS Mathematics, 2022, 7(1): 225-246. https://doi.org/10.3934/math.2022014

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Received: 06 July 2021
Accepted: 17 September 2021
Published: 15 January 2022
©2022 the Author(s), licensee AIMS Press.

This is an open access article distributed under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0)