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Magnetic Field Evaluation at Vertex by Boundary Integral Equation Derived From Scalar Potential of Double Layer Charge

机译:利用双层电荷的标量势导出边界积分方程估算顶点处的磁场

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摘要

Adopting the integral representation of scalar potential due to double layer charge, we derive a boundary integral equation with one unknown to solve magnetostatic problems. The double layer charge produces a potential gap at the air–material boundary without disturbing the continuity of normal magnetic flux density and the potential gap makes the tangential component of magnetic field continuous; accordingly, the boundary conditions are fully fulfilled even with one unknown. The boundary integral equation is capable of solving the double layer charge at edges and corners. Once the double layer charge is solved, it gives directly the magnetic flux density by Biot–Savart law. In this paper, we investigate how to evaluate the magnetic flux density at the vertex.
机译:采用由双层电荷引起的标量势的积分表示,我们推导出了一个边界积分方程,其中一个未知数可以解决静磁问题。双层电荷在空气-材料边界处产生一个势隙,而不会干扰法向磁通密度的连续性,并且该势隙使磁场的切向分量连续。因此,即使有一个未知数,边界条件也能完全满足。边界积分方程能够求解边缘和拐角处的双层电荷。一旦解决了双层电荷,它就会根据Biot-Savart定律直接给出磁通密度。在本文中,我们研究了如何评估顶点处的磁通密度。

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