“…Hybrid Latticeu n (t) = (1 + αu n + βu 2 n )(u n−1 − u n+1 ) [17] u n (t) = −α± Table 2 Examples of DDEs and their solutions computed with DDESpecialSolutions.m.…”
A new algorithm is presented to find exact traveling wave solutions of differentialdifference equations in terms of tanh functions. For systems with parameters, the algorithm determines the conditions on the parameters so that the equations might admit polynomial solutions in tanh.Examples illustrate the key steps of the algorithm. Parallels are drawn through discussion and example to the tanh-method for partial differential equations.The new algorithm is implemented in Mathematica. The package DDESpecialSolutions.m can be used to automatically compute traveling wave solutions of nonlinear polynomial differential-difference equations. Use of the package, implementation issues, scope, and limitations of the software are addressed.
Program summary
“…Hybrid Latticeu n (t) = (1 + αu n + βu 2 n )(u n−1 − u n+1 ) [17] u n (t) = −α± Table 2 Examples of DDEs and their solutions computed with DDESpecialSolutions.m.…”
A new algorithm is presented to find exact traveling wave solutions of differentialdifference equations in terms of tanh functions. For systems with parameters, the algorithm determines the conditions on the parameters so that the equations might admit polynomial solutions in tanh.Examples illustrate the key steps of the algorithm. Parallels are drawn through discussion and example to the tanh-method for partial differential equations.The new algorithm is implemented in Mathematica. The package DDESpecialSolutions.m can be used to automatically compute traveling wave solutions of nonlinear polynomial differential-difference equations. Use of the package, implementation issues, scope, and limitations of the software are addressed.
Program summary
“…The Volterra type equations are discretizations of the Kortewegde Vries (KdV) and modified KdV equations [26,27]. The exact solutions of (1) have been obtained by the tanh method [28].…”
Section: Optimal Ham For Volterra Latticementioning
The travelling-wave solution of the Volterra lattice has been constructed by the optimal homotopy analysis method. The optimal method used here contains three auxiliary convergence-control parameters to adjust and control the convergence region of the solution. By minimizing the averaged residual error, the optimal convergence-control parameters can be obtained, which give much better approximations than those given by the usual homotopy analysis method. The obtained results show that the optimal homotopy analysis method is also very efficient for differential-difference equations.
“…B. Diaz and T. J. Osler [7] defined the fractional difference by the rather natural approach of allowing the index of differencing, in the standard expression for the n th difference, to be any real or complex number. Later, R. Hirota [9], defined the fractional order difference operator ∇ α where α is any real number, using Taylor's series. A. Nagai [10] adopted another definition for fractional difference by modifying Hirota's definition.…”
Abstract. Discrete inequalities, in particular the discrete analogues of the Gronwall-Bellman inequality, have been extensively used in the analysis of finite difference equations. The aim of the present paper is to establish some fractional difference inequalities of Gronwall-Bellman type which provide explicit bounds for the solutions of fractional difference equations.
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