2017
DOI: 10.4236/jemaa.2017.910012
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Point Charges and Conducting Planes for Yukawa’s Potential and Coulomb’s Potential

Abstract: In this work, we modeled and simulated the electric potential generated by point charges in the region of grounded conductor planes for Yukawa poten- with different values of µ . We observe that the electric potential decreases as the value of µ increases and that does not allow all the charge to be distributed on the surface of the conductor.

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Cited by 1 publication
(9 citation statements)
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“…For the case we have discussed in this work, we can verify this if we consider 60 α =  and the position of the actual charge as ϕ =  and this result corresponds to the case of a charge between two perpendicular conducting planes. These last two cases were recently discussed [1].…”
Section: Discussion Of Resultsmentioning
confidence: 91%
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“…For the case we have discussed in this work, we can verify this if we consider 60 α =  and the position of the actual charge as ϕ =  and this result corresponds to the case of a charge between two perpendicular conducting planes. These last two cases were recently discussed [1].…”
Section: Discussion Of Resultsmentioning
confidence: 91%
“…It can be used Yukawa potential ( e r r µ − ) or Coulomb potential (1/r) Procedure for the calculation of the potential and electric field of a charge Q between two planes forming an angle of 60˚ > restart; > with(plots): > with(plottools): > with(linalg): > with(StringTools): > poteimgs := proc(cpoint, centerp, angplan, r, q, typec) > local charget, i, n, chargex, phi, k, epsilon, angplanx, rxy; > charget := 0; > n := abs(((360)/convert(angplan [1], units, radians, degrees))) -1; > epsilon := 8.85*10^(-12); > k := 1/(4*Pi*epsilon); > angplanx := `if`(type(r, list) or type(r, vector) or type(r, matrix), in- [2]); > rxy := `if`(type(r, list) or type(r, vector) or type(r, matrix), sqrt(r [1]…”
Section: Discussion Of Resultsmentioning
confidence: 99%
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