Standard

Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow. / Gunko, Yuri F.; Gunko, Natalia A.

In: AIP Conference Proceedings, Vol. 1959, 100002, 02.05.2018.

Research output: Contribution to journal › Conference article › peer-review

Harvard

Gunko, YF & Gunko, NA 2018, 'Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow', AIP Conference Proceedings, vol. 1959, 100002. https://doi.org/10.1063/1.5034749

APA

Gunko, Y. F., & Gunko, N. A. (2018). Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow. AIP Conference Proceedings, 1959, [100002]. https://doi.org/10.1063/1.5034749

Vancouver

Gunko YF, Gunko NA. Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow. AIP Conference Proceedings. 2018 May 2;1959. 100002. https://doi.org/10.1063/1.5034749

Author

Gunko, Yuri F. ; Gunko, Natalia A. / Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow. In: AIP Conference Proceedings. 2018 ; Vol. 1959.

BibTeX

@article{4e5c5420c1bf4a21829f0aba908e6580,
title = "Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow",
abstract = "In this paper we consider the problem of determining the structure of the electric field near the surface of a flat insulated body under conditions of a deep vacuum. It is assumed that the emitted particles are electrons leaving the body surface under the influence of ionizing radiation whose velocities distribution near the surface is isotropic. It is estimated the thickness of the screening layer under conditions of stationary emission from a flat surface. The solutio of the problem of determining a stationary self-consistent electric field near the surface is found in a simple analytical form. The thickness of the screening layer is calculated from this formula.",
keywords = "SPACE-CHARGE, CURRENTS, GASES",
author = "Gunko, {Yuri F.} and Gunko, {Natalia A.}",
year = "2018",
month = may,
day = "2",
doi = "10.1063/1.5034749",
language = "English",
volume = "1959",
journal = "AIP Conference Proceedings",
issn = "0094-243X",
publisher = "American Institute of Physics",
note = "International Scientific Conference on Mechanics - Eighth Polyakhov's Reading : 8th Polyakhov's Reading ; Conference date: 29-01-2018 Through 02-02-2018",
url = "https://events.spbu.ru/events/polyakhov_readings, http://nanomat.spbu.ru/en/node/175, http://nanomat.spbu.ru/ru/node/192, http://spbu.ru/news-events/calendar/viii-polyahovskie-chteniya",

}

RIS

TY - JOUR

T1 - Structure of the screening layer near a plane isolated body in the deep vacuum. Part 2. Monoenergetic isotropic flow

AU - Gunko, Yuri F.

AU - Gunko, Natalia A.

N1 - Conference code: 8

PY - 2018/5/2

Y1 - 2018/5/2

N2 - In this paper we consider the problem of determining the structure of the electric field near the surface of a flat insulated body under conditions of a deep vacuum. It is assumed that the emitted particles are electrons leaving the body surface under the influence of ionizing radiation whose velocities distribution near the surface is isotropic. It is estimated the thickness of the screening layer under conditions of stationary emission from a flat surface. The solutio of the problem of determining a stationary self-consistent electric field near the surface is found in a simple analytical form. The thickness of the screening layer is calculated from this formula.

AB - In this paper we consider the problem of determining the structure of the electric field near the surface of a flat insulated body under conditions of a deep vacuum. It is assumed that the emitted particles are electrons leaving the body surface under the influence of ionizing radiation whose velocities distribution near the surface is isotropic. It is estimated the thickness of the screening layer under conditions of stationary emission from a flat surface. The solutio of the problem of determining a stationary self-consistent electric field near the surface is found in a simple analytical form. The thickness of the screening layer is calculated from this formula.

KW - SPACE-CHARGE

KW - CURRENTS

KW - GASES

UR - http://www.scopus.com/inward/record.url?scp=85047178626&partnerID=8YFLogxK

U2 - 10.1063/1.5034749

DO - 10.1063/1.5034749

M3 - Conference article

AN - SCOPUS:85047178626

VL - 1959

JO - AIP Conference Proceedings

JF - AIP Conference Proceedings

SN - 0094-243X

M1 - 100002

T2 - International Scientific Conference on Mechanics - Eighth Polyakhov's Reading

Y2 - 29 January 2018 through 2 February 2018

ER -

ID: 36987877