2005
DOI: 10.1088/0022-3727/38/21/025
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Image charge inclusions in the prolate dielectric spheroid

Abstract: A curious property of the electrostatic image theory for the perfectly conducting prolate spheroid, introduced in 2001, is pointed out: the potential outside the conducting spheroid remains unchanged if the conductor is replaced by a dielectric spheroid with an embedded charge which coincides with the image charge for the conducting spheroid case. The present note is a generalization of the corresponding observation about the classical Kelvin image theory for the conducting sphere, made in 1988.

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Cited by 18 publications
(21 citation statements)
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“…8 Since then the classical Kelvin image theory for a charged sphere was successfully generalized by Lindell 9,10 and extended to dielectric spheres. [11][12][13][14] Many models based on the image charge theory exist today, and these include a variety of boundary conditions suitable for describing some aspects of experiment, [15][16][17] most notably the methods proposed by Ohshima [18][19][20][21][22][23][24] for the interaction between spheres in media of homogeneous dielectric permittivity. However, at close separation image charge methods require increasing numbers of images leading to convergence problems for a series expansion of the electrostatic force.…”
Section: Introductionmentioning
confidence: 99%
“…8 Since then the classical Kelvin image theory for a charged sphere was successfully generalized by Lindell 9,10 and extended to dielectric spheres. [11][12][13][14] Many models based on the image charge theory exist today, and these include a variety of boundary conditions suitable for describing some aspects of experiment, [15][16][17] most notably the methods proposed by Ohshima [18][19][20][21][22][23][24] for the interaction between spheres in media of homogeneous dielectric permittivity. However, at close separation image charge methods require increasing numbers of images leading to convergence problems for a series expansion of the electrostatic force.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately, Van Siclen's original argument is somewhat involved and occasionally erroneous [7]. In this paper, we simplify the argument and show by direct calculation of the sources of the field how the surprising result reported in [6] comes about.…”
Section: Introductionmentioning
confidence: 86%
“…Using the dielectric constant reported for CdSe nanoparticles [ 148 ] ϵ / ϵ 0 = 6, one could estimate eV g ≈ 20 meV by assuming the dielectric filling the whole space. For a dielectric sphere surrounded by vacuum mimicking the SET, significantly higher values could be achieved, [ 149,150 ] which would further increase the operating temperature of the device. Nonetheless, here we prefer to make the conservative assumption eV g ≈ 20 meV to account for other possible charge screening effects and/or for a less favorable geometry in a practical realization, for example, with D farther from the SET.…”
Section: Ciss‐mediated Initialization and Readout Of Single Moleculesmentioning
confidence: 99%