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The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body. / Tikhonov, A. A.

In: Vestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya, No. 2, 01.04.1991, p. 90-99.

Research output: Contribution to journalArticlepeer-review

Harvard

Tikhonov, AA 1991, 'The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body', Vestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya, no. 2, pp. 90-99.

APA

Tikhonov, A. A. (1991). The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body. Vestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya, (2), 90-99.

Vancouver

Tikhonov AA. The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body. Vestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya. 1991 Apr 1;(2):90-99.

Author

Tikhonov, A. A. / The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body. In: Vestnik Sankt-Peterburgskogo Universiteta. Ser 1. Matematika Mekhanika Astronomiya. 1991 ; No. 2. pp. 90-99.

BibTeX

@article{2e08c7bf65754a2b9a952d3f6068783a,
title = "The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body",
abstract = "The charged solid body (CSB) moving along the near-earth ring equatorial orbit, is considered. CSB rotational motion in respect to its centre of mass under the action of the gravitational force moment and the Lorentz force moment occurring during CSB motion in the Earth magnetic field (EMF) is studied. The influence of EMF non-uniformity on CSB dynamics is investigated under assumption that the Earth gravitational field is the Newtonian central one. The model of direct dipole is considered as the EMF model, the EMF daily rotation together with Earth is taken into account. The simple case, when the CSB inertia ellipsoid is a sphere, is discussed. The results can be spread for more general case, when the CSB inertia ellipsoid is the ellipsoid of revolution.",
author = "Tikhonov, {A. A.}",
year = "1991",
month = apr,
day = "1",
language = "русский",
pages = "90--99",
journal = "ВЕСТНИК САНКТ-ПЕТЕРБУРГСКОГО УНИВЕРСИТЕТА. МАТЕМАТИКА. МЕХАНИКА. АСТРОНОМИЯ",
issn = "1025-3106",
publisher = "Издательство Санкт-Петербургского университета",
number = "2",

}

RIS

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T1 - The influence of the geomagnetic field non-uniformity on the evolution of the rotary attitude motion of a charged rigid body

AU - Tikhonov, A. A.

PY - 1991/4/1

Y1 - 1991/4/1

N2 - The charged solid body (CSB) moving along the near-earth ring equatorial orbit, is considered. CSB rotational motion in respect to its centre of mass under the action of the gravitational force moment and the Lorentz force moment occurring during CSB motion in the Earth magnetic field (EMF) is studied. The influence of EMF non-uniformity on CSB dynamics is investigated under assumption that the Earth gravitational field is the Newtonian central one. The model of direct dipole is considered as the EMF model, the EMF daily rotation together with Earth is taken into account. The simple case, when the CSB inertia ellipsoid is a sphere, is discussed. The results can be spread for more general case, when the CSB inertia ellipsoid is the ellipsoid of revolution.

AB - The charged solid body (CSB) moving along the near-earth ring equatorial orbit, is considered. CSB rotational motion in respect to its centre of mass under the action of the gravitational force moment and the Lorentz force moment occurring during CSB motion in the Earth magnetic field (EMF) is studied. The influence of EMF non-uniformity on CSB dynamics is investigated under assumption that the Earth gravitational field is the Newtonian central one. The model of direct dipole is considered as the EMF model, the EMF daily rotation together with Earth is taken into account. The simple case, when the CSB inertia ellipsoid is a sphere, is discussed. The results can be spread for more general case, when the CSB inertia ellipsoid is the ellipsoid of revolution.

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M3 - статья

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SP - 90

EP - 99

JO - ВЕСТНИК САНКТ-ПЕТЕРБУРГСКОГО УНИВЕРСИТЕТА. МАТЕМАТИКА. МЕХАНИКА. АСТРОНОМИЯ

JF - ВЕСТНИК САНКТ-ПЕТЕРБУРГСКОГО УНИВЕРСИТЕТА. МАТЕМАТИКА. МЕХАНИКА. АСТРОНОМИЯ

SN - 1025-3106

IS - 2

ER -

ID: 29121775