A new technique for solving a class of strongly nonlinear oscillatory equations
Introduction
The classical perturbation methods [1], [2], [3], [4], [5] have been developed for solving nonlinear oscillatorswhere . But modifications of some classical perturbation methods [6], [7], [8] overcome this limitation. On the other hand, some analytical techniques have been presented for handling strong nonlinear oscillators such as homotopy perturbation method [9], [10], [11], homotopy analysis method (HAM) [12], variational iteration method (VIM) [13], generalized homotopy method [14], harmonic balance method (HBM) [15], energy balance method [16], etc. However, most of the methods were formulated based on trigonometric functions. The differential transform method (DTM) [17], [18], [19] is a semi-analytical approach which is applied for solving strong nonlinear oscillators. Zhou [20] first introduced DTM and applied it to analyse linear and nonlinear electric circuit problems. Further the method is modified and applied to solve various differential equations. Shahed [21] also modified DTM based on Pade´ approximants. Combining Laplace transform and Pade ́ approximants, Momani and Erturk [22] presented a modified DTM method. Gokdogana et al. [23] proposed an adaptive multi-step differential transformation method to solve nonlinear differential equations. Besides, the DTM method is used by several researchers [24], [25], [26] to investigate nonlinear problems.
In this article, a new technique (like DTM) is presented for solving Eq. (1.1). The proposed solution is independent of trigonometric functions. The formulation as well as determination of the solution is very simple. Moreover, the solution is valid for all values of and .
Section snippets
The method
By a variable transformation , Eq. (1.1) readily becomes:where primes denote differentiation with respect to . Let us consider a polynomial-type solution of Eq. (2.1) in the form:where are unknown coefficients to be determined and is the period of oscillation. It is obvious that Eq. (2.2) satisfies the first initial condition given in Eq. (1.1). Solution Eq. (2.2) is valid for one
Simple harmonic oscillator
Let us consider a linear oscillator
Substituting Eq. (2.2) into Eq. (3.1) and then equating the coefficients of , , the following algebraic equations have been found:
Solving Eq. (3.2), the following unknown coefficients have been found:
Now differentiating Eq. (2.2) with respect to and then substituting (i.e., by utilization of the second initial condition), it
Results and discussion
A new technique has been presented to solve nonlinear oscillators. The determination of related unknown coefficients of the proposed solution is similar to that of HBM, but the method is independent of harmonic functions. The main advantage of the method is that algebraic equations of unknown coefficients are linear. In contrast, corresponding equations for HBM are nonlinear. The solution procedure of these nonlinear algebraic equations is another difficult task.
In the previous section the
Authors' statement
Authors declared the above paper has not been published elsewhere or is not under review.
Declaration of Competing Interest
Authors declared the above paper has not been published elsewhere or is not under review.
Acknowledgement
Authors are thankful to the honourable reviewers for their valuable comments.
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