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_:Nc2506372f92d40728fc79364f5a34e16 _:N7b453fd767014eafb67a296a8998a081 .
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"2018-09-01" .
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"Institute of Plasma Physics, National Science Center \u201CKharkiv Institute of Physics and Technology,\u201D, 61108, Kharkiv, Ukraine" .
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_:N7b453fd767014eafb67a296a8998a081 "Rudakov" .
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"Physical Parameters of a Reactor-Stellarator with Small Ripples of the Helical Magnetic Field" .
"2019-04-10T22:37" .
"http://link.springer.com/10.1134%2FS1063780X18090118" .
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_:N7b453fd767014eafb67a296a8998a081 "V. A." .
_:N3b2e0686ff014f11b202e224e04e9308 .
"Plasma Physics Reports" .
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_:Nad0e5017459f4df19aaf6213c6ea274b "Springer Nature - SN SciGraph project" .
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"Atomic, Molecular, Nuclear, Particle and Plasma Physics" .
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_:N3b2e0686ff014f11b202e224e04e9308 "pub.1107110954" .
"The paper describes the calculation data on the physical parameters of a reactor-stellarator, where the nonuniformities of the helical field are smaller than the toroidal magnetic field nonuniformities: \u03B5h < \u03B5t. Unlike the previous studies, where the ion-component transport coefficients had the collision frequency dependence proportional to \u03BD1/2, this being equivalent to the \u03B5h > \u03B5t case, in the present calculations, these coefficients were assumed to be in proportion to the first power of the collision frequency, Di \u221D \u03BD for \u03BDeff < 2\u03C9E, and to Di \u221D \u03BD\u22121 for the inverse inequality. Here, \u03C9E is the rotation frequency of plasma in the radial electric field. As before, the plasma electrons corresponded to the mode of De \u221D \u03BD\u22121. As initial parameters for numerical calculations, a reactor with R = 8 m, rp = 2 m, and B0 = 5 \u0422 was taken. A numerical code was used to solve the set of equations that describes the plasma space\u2212time behavior in the reactor-stellarator under the conditions of equal diffusion fluxes. The start of reactor operation in the mode of thermonuclear burning was provided by heating sources with a power of several tens of megawatts. Steady-state operating conditions of a self-sustained thermonuclear reaction were attained by maintaining the plasma density through DT fuel pellet injection into the plasma." .
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