Magnetic compression heating of extremely high beta plasma configuration
Magnetic compression heating of extremely high beta plasma configuration
批准号:
12480119
负责人:
OKADA Shigefumi
金额:
$8.06万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for Scientific Research (B)
财政年份:
2000
资助国家:
日本
项目状态:
已结题
起止时间:
2000 至 2002
中文摘要
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英文摘要
Plasma with field-reversed configuration has extremely high beta value (plasma pressure/ confining magnetic field pressure) of about 1. Therefore, confining magnetic field of the FRC fusion reactor can be far weaker than in low beta confinement schemes, which is favorable for technological viewpoint. High-energy neutral beam (NB) is the most important method to heat and sustain the FRC plasma. As the cost of the NB is expensive, it is desired that the FRC plasma should have good confinement property to reduce the cost of the NB. It is known that confinement time of the FRC plasma is proportional to 2-3 powers of the radius r_s of the FRC plasma. Up to present, r_s has increased by translating the plasma from formation region to confinement region. This technology of translation has an advantage that r_s can be increased without serious lowering of plasma temperature. But it has a disadvantage that obtainable value of r_s is limited: By the translation, the FRC plasma is ejected into th … More e confinement region with supersonic velocity and it must be stopped, when the plasma expands radially, excessively and the confinement is degraded because, perhaps, the plasma touches the wall. In order to increase r_s, new scheme of axial compression is proposed. The FRC plasma is compressed radially by decreasing the distance between the mirror fields, which are confining the plasma. Coils were developed to realize this compression, which coils produced magnetic field with the rise time of about 50μs, which is faster than confinement times and slower than propagation of sound wave. These coils were installed in the vacuum chamber and were energized successively. The result of the compression could be explained by adiabatic theory when the effect of energy loss and the magnetic flux loss were token into account. Moreover, it was also observed that the confinement property did not depend on the plasma length even when the plasma was compressed until the elongation (plasma length / plasma radius) or the aspect ratio became as small as 4.1. Less
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S.Yoshimura et al.: "Computer Tomography of Axially Compressed Field Reversed Configuration Plasma on the FIX Device"IEEE TRANSACTION ON PLASMA SCIENCE. Vol.30, No.1. 60-61 (2002)
S.Yoshimura 等人:“FIX 设备上轴向压缩场反转配置等离子体的计算机断层扫描”IEEE TRANSACTION ON PLASMA SCIENCE。
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S.Okada et al.: "Additional control experiment on field reversed configuration plasma"Fusion Science and Technology. Vol.43, No.1T. (2003)
S.Okada等:“场反构型等离子体的附加控制实验”聚变科学与技术。
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Y.Suzuki, S.Okada et. al.: "Two-dimensional equilibria of field-reversed configuration in the strong mirror field"PHYSICS OF PLASMAS. Vol.7, No.10. 4062-4069 (2000)
Y.Suzuki,S.Okada 等。
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S.Yoshimura, et.al.,: "Internal magnetic probe measurement in heating experiment of field-reversed configuration plasma by applying fast rising magnetic pulse"Transactions of Fusion Technology. 39. 378-381 (2001)
S.Yoshimura 等人:“通过应用快速上升磁脉冲进行场反转配置等离子体加热实验中的内部磁探针测量”Transactions of Fusion Technology。
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K.Kitano, S.Maeshima, S.Okada et al.: "Dynamic process during axial magnetic compression of field-reversed configuration for equilibrium shape control"PHYSICS OF PLASMAS. Vol.8, No8. 3630-3634 (2001)
K.Kitano、S.Maeshima、S.Okada 等人:“用于平衡形状控制的场反转配置的轴向磁压缩期间的动态过程”等离子体物理学。
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