On the Surface Integral Approximation of the Second Derivatives of the Potential of a Bulk Charge Located in a Layer of Small Thickness
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DOI: 10.1134/s0012266118090112
Abstract: We consider a bulk charge potential of the form $$u(x) = \int\limits_\Omega {g(y)F(x - y)dy,x = ({x_1},{x_2},{x_3}) \in {\mathbb{R}^3},} $$u(x)=∫Ωg(y)F(x−y)dy,x=(x1,x2,x3)∈R3, where Ω is a layer of small thickness h > 0 located around the midsurface… read more here.
Keywords: surface; second derivatives; partial partial; bulk charge ... See more keywords