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A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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Magnetic flux depends on three factors: the strength of the magnetic field, the area through which the field lines pass, and the field's orientation with respect to the surface area. If any of these quantities vary, a corresponding variation in magnetic flux occurs. If the area through which the magnetic field lines are passing changes, then the magnetic flux also changes. This change in the area can be of two types: the flux through the rectangular loop increases as it moves into the...
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Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Determining the rotation direction in pulsars.

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在旋转的镜子等离子体中,巨大的,长寿命的静电潜力.

E J Kolmes1, I E Ochs2, J-M Rax3,4

  • 1Department of Astrophysical Sciences, Princeton University, Princeton, NJ, 08544, USA. ekolmes@princeton.edu.

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概括

这项研究提出了一种用于磁性封闭装置的新方法,以管理热等离子体内的高电压下降. 通过在内部战略性地放置电压下降,它允许比以前可能更大的稳定状态电压.

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科学领域:

  • 等离子体物理学的物理学
  • 磁性封闭融合技术的使用
  • 高电压工程 高电压工程

背景情况:

  • 热等离子体与磁场平行表现出高电导率,导致沿磁场线沿近恒定的电潜.
  • 在开放场线磁性封闭中,交叉场电压下降受限于面向等离子体的组件在场线碰撞的地方的材料耐受性.

研究的目的:

  • 提出一种新的配置,用于管理磁性等离子装置中的大电压下降.
  • 为了规避边界电压下降所造成的物质限制,在开放场线磁性封闭中.

主要方法:

  • 在设备内部安排显著的电压下降,同时在边界保持小的下降.
  • 确保流体表面内的漂移-流动剪切最小,并避免大平行电场驱动大量平行电流.

主要成果:

  • 证明了大的内部电压下降可以与小的边界下降共存.
  • 证明可以同时满足防止过度散射 (低漂流切割和低平行电流) 的要求.
  • 表明可以实现稳定状态电压下降的可能性,远远超过材料公差.

结论:

  • 介绍了一种方法,使磁化等离子体能够承受显著更大的稳定状态电压下降.
  • 这种方法克服了面向等离子体的组件中固体材料公差的局限性.
  • 这些发现为先进的磁束聚变和等离子装置设计打开了新的可能性.