Abstract
Two numerical methods are presented for the periodic initial-value problem of the long wave-short wave interaction equations describing the interaction between one long longitudinal wave and two short transverse waves propagating in a generalized elastic medium. The first one is the relaxation method, which is implicit with second-order accuracy in both space and time. The second one is the split-step Fourier method, which is of spectral-order accuracy in space. We consider the first-, second- and fourth-order versions of the split-step method, which are first-, second- and fourth-order accurate in time, respectively. The present split-step method profits from the existence of a simple analytical solution for the nonlinear subproblem. We numerically test both the relaxation method and the split-step schemes for a problem concerning the motion of a single solitary wave. We compare the accuracies of the split-step schemes with that of the relaxation method. Assessments of the efficiency of the schemes show that the fourth-order split-step Fourier scheme is the most efficient among the numerical schemes considered.
Original language | English |
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Pages (from-to) | 113-125 |
Number of pages | 13 |
Journal | Mathematics and Computers in Simulation |
Volume | 74 |
Issue number | 2-3 |
DOIs | |
Publication status | Published - 7 Mar 2007 |
Keywords
- Long wave-short wave interaction equations
- Relaxation method
- Solitary waves
- Split-step method