TY - JOUR
T1 - Multi-symplectic scheme and simulation of solitary wave solution for generalized KdV-mKdV equation
AU - Hu, Weipeng
AU - Deng, Zichen
AU - Li, Wencheng
PY - 2008/8
Y1 - 2008/8
N2 - Aim. Many practical problems are nonlinear. Linearization often brings poor long-time numerical behavior. In order to keep long-time numerical behavior satisfactory, we consider the multi-symplectic formulations of the generalized KdV-mKdV equation with initial value condition in the Hamilton space. In the full paper, we explain our multi-symplectic scheme in some detail; in this abstract, we just add some pertinent remarks to listing the two topics of explanation. The first topic is: the multi-symplectic formulation of the generalized KdV-mKdV equation and its conservation laws. In this topic, we derive eq.(6) as the multi-symplectic formulation and eqs.(7), (8) and (9) as the conservation laws. The second topic is: the multi-symplectic Preissmann scheme and its equivalent form. In this topic, we construct the equivalent scheme of the Preissmann integrator, which is given as eq.(14). To verify the validity of eq.(14), we simulate the solitary wave solution of the generalized KdV-mKdV equation. The computer simulation results, shown in Figs.1 and 2 in the full paper, indicate preliminarily that the multi-symplectic scheme can keep unchanged the wave form of the solitary wave solution and preserve well the local energy and local momentum in the Hamilton space.
AB - Aim. Many practical problems are nonlinear. Linearization often brings poor long-time numerical behavior. In order to keep long-time numerical behavior satisfactory, we consider the multi-symplectic formulations of the generalized KdV-mKdV equation with initial value condition in the Hamilton space. In the full paper, we explain our multi-symplectic scheme in some detail; in this abstract, we just add some pertinent remarks to listing the two topics of explanation. The first topic is: the multi-symplectic formulation of the generalized KdV-mKdV equation and its conservation laws. In this topic, we derive eq.(6) as the multi-symplectic formulation and eqs.(7), (8) and (9) as the conservation laws. The second topic is: the multi-symplectic Preissmann scheme and its equivalent form. In this topic, we construct the equivalent scheme of the Preissmann integrator, which is given as eq.(14). To verify the validity of eq.(14), we simulate the solitary wave solution of the generalized KdV-mKdV equation. The computer simulation results, shown in Figs.1 and 2 in the full paper, indicate preliminarily that the multi-symplectic scheme can keep unchanged the wave form of the solitary wave solution and preserve well the local energy and local momentum in the Hamilton space.
KW - Computer simulation
KW - Generalized KdV-mKdV equation
KW - Multi-symplectic integrator
KW - Preissman scheme
KW - Solitary wave solution
UR - http://www.scopus.com/inward/record.url?scp=53649092798&partnerID=8YFLogxK
M3 - 文章
AN - SCOPUS:53649092798
SN - 1000-2758
VL - 26
SP - 450
EP - 453
JO - Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University
JF - Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University
IS - 4
ER -