Haar wavelets operational matrix based algorithm for computational modelling of hyperbolic type wave equations
Purpose The purpose of this study is to develop an algorithm for approximate solutions of
nonlinear hyperbolic partial differential equations. Design/methodology/approach In this …
nonlinear hyperbolic partial differential equations. Design/methodology/approach In this …
Taylor polynomial solution of hyperbolic type partial differential equations with constant coefficients
B Bülbül, M Sezer - International Journal of Computer Mathematics, 2011 - Taylor & Francis
The purpose of this study is to give a Taylor polynomial approximation for the solution of
hyperbolic type partial differential equations with constant coefficients. The technique used …
hyperbolic type partial differential equations with constant coefficients. The technique used …
Numerical treatment of the sine-Gordon equations via a new DQM based on cubic unified and extended trigonometric B-spline functions
M Tamsir, MZ Meetei, N Dhiman - Wave Motion, 2024 - Elsevier
The purpose of this work is to propose a new composite scheme based on differential
quadrature method (DQM) and modified cubic unified and extended trigonometric B-spline …
quadrature method (DQM) and modified cubic unified and extended trigonometric B-spline …
Hyperbolic (3+ 1)‐Dimensional Nonlinear Schrödinger Equation: Lie Symmetry Analysis and Modulation Instability
The hyperbolic nonlinear Schrödinger equation in the (3+ 1)‐dimension depicts the
evolution of the elevation of the water wave surface for slowly modulated wave trains in …
evolution of the elevation of the water wave surface for slowly modulated wave trains in …
An Operator‐Difference Method for Telegraph Equations Arising in Transmission Lines
ME Koksal - Discrete Dynamics in Nature and Society, 2011 - Wiley Online Library
A second‐order linear hyperbolic equation with time‐derivative term subject to appropriate
initial and Dirichlet boundary conditions is considered. Second‐order unconditionally …
initial and Dirichlet boundary conditions is considered. Second‐order unconditionally …
Finite difference method for hyperbolic equations with the nonlocal integral condition
A Ashyralyev, N Aggez - Discrete Dynamics in Nature and …, 2011 - Wiley Online Library
The stable difference schemes for the approximate solution of the nonlocal boundary value
problem for multidimensional hyperbolic equations with dependent in space variable …
problem for multidimensional hyperbolic equations with dependent in space variable …
[HTML][HTML] Legendre approximation for solving linear HPDEs and comparison with Taylor and Bernoulli matrix methods
E Tohidi - 2012 - scirp.org
The aim of this study is to give a Legendre polynomial approximation for the solution of the
second order linear hyper-bolic partial differential equations (HPDEs) with two variables and …
second order linear hyper-bolic partial differential equations (HPDEs) with two variables and …
A numerical technique based on Legendre wavelet for linear and nonlinear hyperbolic telegraph equation
This study is devoted to the numerical investigation of linear and nonlinear hyperbolic
telegraph equation. We have proposed a wavelet collocation method based on Legendre …
telegraph equation. We have proposed a wavelet collocation method based on Legendre …
A comparative study for the numerical approximation of 1D and 2D hyperbolic telegraph equations with UAT and UAH tension B-spline DQM
M Kapoor - Nonlinear Engineering, 2023 - degruyter.com
Two numerical regimes for the one-and two-dimensional hyperbolic telegraph equations are
contrasted in this article. The first implemented regime is uniform algebraic trigonometric …
contrasted in this article. The first implemented regime is uniform algebraic trigonometric …
A note on nonlocal boundary value problems for hyperbolic Schrödinger equations
Y Ozdemir, M Kucukunal - Abstract and Applied Analysis, 2012 - Wiley Online Library
The nonlocal boundary value problem d2u (t)/dt2+ Au (t)= f (t)(0≤ t≤ 1), i (du (t)/dt)+ Au (t)=
g (t)(− 1≤ t≤ 0), u (0+)= u (0−), ut (0+)= ut (0−), Au (− 1)= αu (μ)+ φ, 0< μ≤ 1, for hyperbolic …
g (t)(− 1≤ t≤ 0), u (0+)= u (0−), ut (0+)= ut (0−), Au (− 1)= αu (μ)+ φ, 0< μ≤ 1, for hyperbolic …