1999
DOI: 10.1002/(sici)1097-0207(19990320)44:8<1055::aid-nme541>3.0.co;2-1
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A coupled boundary/finite element method for the computation of magnetically and electrostatically levitated droplet shapes

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Cited by 21 publications
(25 citation statements)
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“…Since the electric field inside the droplet is zero, only the potential distribution outside needs to be solved for. For this problem, the boundary integral can be obtained from the classical Green's theorem, [16] [ 18] where ⌽Ј ϭ ⌽ ϩ Er cos , ∂⍀ 2 designates the surface of the droplet, and denotes the boundary at infinity. The Green function, G, and its normal derivative are calculated by the following expressions written for a cylindrical coordinate system: [16] [19] [20] where is the geometric parameter calculated by [21] …”
Section: A Droplet Deformation Calculationsmentioning
confidence: 99%
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“…Since the electric field inside the droplet is zero, only the potential distribution outside needs to be solved for. For this problem, the boundary integral can be obtained from the classical Green's theorem, [16] [ 18] where ⌽Ј ϭ ⌽ ϩ Er cos , ∂⍀ 2 designates the surface of the droplet, and denotes the boundary at infinity. The Green function, G, and its normal derivative are calculated by the following expressions written for a cylindrical coordinate system: [16] [19] [20] where is the geometric parameter calculated by [21] …”
Section: A Droplet Deformation Calculationsmentioning
confidence: 99%
“…[18] simplifies to a boundary integral that involves only the surface of the droplet, ∂⍀ 2 . Following the standard boundary element discretization, noticing that the potential on the surface is a constant and substituting ⌽ ϭ ⌽Ј -Er cos into the resultant equation, one obtains the final matrix form for the unknowns on the surface of the droplet,…”
Section: A Droplet Deformation Calculationsmentioning
confidence: 99%
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“…(3) involves the integration over the surface only and thus the boundary element method can be applied naturally to discretize the domain for a numerical solution. Following the general procedures described by Brebbia et al [13], the surface can be discretized and both E b and q can be interpolated over each of the boundary elements by use of shape functions, i.e.…”
Section: Problem Statementmentioning
confidence: 99%
“…This traditional boundary element approach should work very well if the kernel function, Kðr; r 0 Þ; is a smooth function, as demonstrated repeatedly in the traditional boundary integral solution of a wide range of engineering problems [13,14]. Unfortunately, for most practical applications involving surface thermal radiation exchanges, the kernel function is not smooth and may experience abrupt disruptions or discontinuities due to various types of geometric obstructions, which can be either the third party blocking or self-blocking of the view between point i and a point of element j: Physically, an occurrence of obstruction means that the radiation intensity emitted from surface element j is intercepted by other bodies and hence does not reach point i: This geometric effect poses a serious problem for accurately calculating the kernel functions in general.…”
Section: Problem Statementmentioning
confidence: 99%