Abstract

In this present study, we investigate the solutions for fractional kinetic equations involving k-Struve function using the Sumudu transform. The graphical interpretations of the solutions involving k-Struve function and its comparison with generalized Bessel function are given. The methodology and results can be considered and applied to various related fractional problems in mathematical physics.

Highlights

  • The Struve function Hν(x) introduced by Hermann Struve in, defined for ν ∈ C by ∞ (– )r x r+ν+ Hν(x) := r= (r + / ) (r + ν ) ( )

  • The Sumudu transform was introduced by Watugala

  • Corollary By putting k = in Theorem, we get the solution of fractional kinetic equation involving classical

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Summary

Introduction

The Struve function Hν(x) introduced by Hermann Struve in , defined for ν ∈ C by. is the particular solutions of the non-homogeneous Bessel differential equations, given by x y (x) + xy (x) +. Is the particular solutions of the non-homogeneous Bessel differential equations, given by x y (x) + xy (x) +. For more details about Struve functions, their generalizations and properties, the esteemed reader is invited to consider the references [ – ]. Nisar et al [ ] introduced and studied various properties of k-Struve function Skν,c defined by. The Sumudu transform was introduced by Watugala (see [ , ]). For more details about the Sumudu transform, see ([ , – ]). The Sumudu transform over the set of functions. We use the Sumudu transform technique to obtain the solutions of fractional kinetic equations by considering ( ). The applications of fractional order calculus are found in many papers (see [ – ]), and it has attracted researchers’ attention in various fields [ – ] because of its importance and efficiency. The fractional differential equation between a chemical reaction or a production scheme (such as in birthdeath processes) was established and treated by Haubold and Mathai [ ] ( see [ , , ])

Solution of generalized fractional kinetic equations for k-Struve function
Conclusion

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