Abstract

In this paper, we construct the group-invariant (exact) solutions for the generalised Fisher type equation using both classical Lie point and the nonclassical symmetry techniques. The generalised Fisher type equation arises in theory of population dynamics. The diffusion term and coefficient of the source term are given as the power law functions of the spatial variable. We introduce the modified Hopf-Cole transformation to simplify a nonlinear second Order Ordinary Equation (ODE) into a solvable linear third order ODE.

Highlights

  • The focus is on the generalised Fisher type equation arising in population dynamics

  • The analysis of the generalised Fisher equation has been carried out using Lie point symmetries and construction of conservation laws see e.g. [2])

  • The reaction-diffusion equations such as the generalized Fisher equation describe how the concentration of a substance is distributed in space changes, whereby the diffusion term causes the spread over the surface

Read more

Summary

Introduction

The focus is on the generalised Fisher type equation arising in population dynamics. The analysis of the generalised Fisher equation has been carried out using Lie point symmetries It turns out that reaction diffusion equations such as the generalised Fisher equation admit the genuine nonclassical symmetries if the source term is given by a cubic In a recent work [3] [11], the authors assume a diffusivity which depends on space variable In this case, the diffusivity may be given as a power law function of space variable for the given reaction-diffusion equation to admit nonclassical symmetries.

Mathematical Description
Symmetry Methods for Differential Equations
Nonclassical Symmetry Reductions
Classical Lie Point Symmetry Reductions
Some Discussions and Concluding Remarks
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.