2013
DOI: 10.1134/s1063780x13090079
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Formation of an internal transport barrier and magnetohydrodynamic activity in experiments with the controlled density of rational magnetic surfaces in the T-10 Tokamak

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Cited by 5 publications
(7 citation statements)
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“…Для анализа характера турбулентного спектра и величины нижнего номера моды m 1 мы используем здесь, как хорошо проверенную в экспериментах на токамаках [9][10][11] гипотезу о механизме образования внутренних барьеров (ITB) в зонах без рациональных поверхностей с низкими значениями m и n (q = m/n), в так называемых «зазорах» (gap или Гэп), где для низких значений m нет рациональных поверхностей. Сравнивая измеренную экспериментально ширину барьера  ITB с расчётной величиной  gap , которая пропорциональна (m 1 dq/dr) -1 , мы находим нижнюю граничную моду m 1 .…”
Section: характеристики турбулентности ответственной за радиальный тunclassified
“…Для анализа характера турбулентного спектра и величины нижнего номера моды m 1 мы используем здесь, как хорошо проверенную в экспериментах на токамаках [9][10][11] гипотезу о механизме образования внутренних барьеров (ITB) в зонах без рациональных поверхностей с низкими значениями m и n (q = m/n), в так называемых «зазорах» (gap или Гэп), где для низких значений m нет рациональных поверхностей. Сравнивая измеренную экспериментально ширину барьера  ITB с расчётной величиной  gap , которая пропорциональна (m 1 dq/dr) -1 , мы находим нижнюю граничную моду m 1 .…”
Section: характеристики турбулентности ответственной за радиальный тunclassified
“…The phenomenon of the formation of ITB zones with reduced thermal conductivity was noted in the early 1990s. It was shown in a number of experimental studies [16][17][18][19][20] that the ITB is formed near the main rational surfaces with low poloidal numbers m and toroidal numbers n; the safety factor q = m/n in zones without rational surfaces with low values of m. A region without rational surfaces for a sufficiently low value of m was called 'the gap'. The existence of such regions was described for the first time in [21].…”
Section: Internal Transport Barriermentioning
confidence: 99%
“…An experimental verification of this position once again confirms the correctness of our explanation of the mechanism of ITB formation. Such experiments were performed in the T-10 tokamak [19]. The internal barrier was generated in a given plasma region with q = 1.5 as a result of off-axis electron cyclotron resonance heating (ECRH) and a rapid current ramp-up with a rate dI/dt = 3 MA s −1 .…”
Section: Experiments On the Formation Of The Barrier And The Islands ...mentioning
confidence: 99%
“…This means that when we increase Γ, the lower mode in the turbulent spectrum can get into the Gap near some rational surface, and if the derivative dq/dr is sufficiently low, it leads to the formation of a barrier. Taking into account that for ITB formation we need to organize a wide Gap, we performed experiments, in which the ITB was generated in a given place with a given q [24]. The barrier near the surface with q = 3/2 was generated using off-axis ECR heating and a rapidly increasing plasma current.…”
Section: Internal Transport Barriers (Itbs)mentioning
confidence: 99%
“…Taking into account that for ITB formation we need to organize a wide Gap, we performed experiments, in which the ITB was generated in a given place with a given q [24]. The barrier near the surface with q = 3/2 was generated using off-axis ECR heating and a rapidly increasing plasma current.…”
Section: Internal Transport Barriers (Itbs)mentioning
confidence: 99%