Magnetohydrodynamic wave spectra in large tokamaks with non-circular cross section of magnetic surfaces

There is considered the problem on the spectra of magnetohydrodynamic (MHD) waves with the frequencies of the order of the ion cyclotron frequency propagating almost along the toroidal magnetic field in the large-size tokamaks with a non-circular cross section of magnetic surfaces. In this case the...

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Бібліографічні деталі
Дата:2000
Автори: D’yakov, V.Ye., Girka, I.A., Yegorenkov, V.D., Stepanov, K.N.
Формат: Стаття
Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2000
Назва видання:Вопросы атомной науки и техники
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Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/78499
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Magnetohydrodynamic wave spectra in large tokamaks with non-circular cross section of magnetic surfaces / V.Ye. D’yakov, I.А. Girka, V.D. Yegorenkov, K.N. Stepanov // Вопросы атомной науки и техники. — 2000. — № 6. — С. 60-61. — Бібліогр.: 4 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Резюме:There is considered the problem on the spectra of magnetohydrodynamic (MHD) waves with the frequencies of the order of the ion cyclotron frequency propagating almost along the toroidal magnetic field in the large-size tokamaks with a non-circular cross section of magnetic surfaces. In this case the waves can propagate in the small vicinity of the extremum point for the square of the refractive index of the MHD wave travelling along the torus. Developing the dielectric permittivity tensor of the “cold” plasma in a Taylor series around this point enables one to separate the variables and to express the natural functions of the boundary problem for Maxwell’s equations through Hermite functions and to determine the natural frequencies of MHD waves. The solution obtained is a generalization of the previous result for arbitrary radial and azimuth numbers. On the ground of the perturbation theory the corrections to the natural functions and natural values are found which take into account the rotational transform.