1982
DOI: 10.1016/0041-5553(82)90118-5
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Numerical methods of solving extremal problems

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Cited by 27 publications
(2 citation statements)
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“…with boundary F1 =g( F2 (4) and initial rt=O = r0 v=0 = V0 , (5) conditions. Here accordingly , E -potential and an electric intensity, r, v, -radius-vector, velocity and the relation of a charge to mass of the charged particle, ro, vo -coordinates and velocity of a particle in the initial moment of time, j -current density, g(r) -known function, F1 , '2 -pieces of boundary F , and F1 U F2 = F , n -a normal to F2 , t -time, e -a dielectric constant.…”
Section: Statement Of Tile Problemmentioning
confidence: 99%
See 1 more Smart Citation
“…with boundary F1 =g( F2 (4) and initial rt=O = r0 v=0 = V0 , (5) conditions. Here accordingly , E -potential and an electric intensity, r, v, -radius-vector, velocity and the relation of a charge to mass of the charged particle, ro, vo -coordinates and velocity of a particle in the initial moment of time, j -current density, g(r) -known function, F1 , '2 -pieces of boundary F , and F1 U F2 = F , n -a normal to F2 , t -time, e -a dielectric constant.…”
Section: Statement Of Tile Problemmentioning
confidence: 99%
“…The problem of the charged particle beams analysis in a mode of restriction of a current by a space charge is known 4 to have singularity near to the cathode of a kind , where r -distance from the current point up to the cathode.…”
Section: Introductionmentioning
confidence: 99%