摘要
球面上第二类 Fredholm积分方程经球坐标变换可化为矩形域 H0 上的问题求解 .用有限元法构造H0 上的插值函数 ,它必须满足在 H0 的左、右两边连续 。
In this paper, we consider solving integral equations of the second kind on a global surface using collocation method. The problem is transfered by mapping onto a rectongle H 0 . Interpolationg function is continue in left and right sides of H 0 .
出处
《数学的实践与认识》
CSCD
2000年第4期423-427,共5页
Mathematics in Practice and Theory