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On the Hamiltonian of a System of Charges Moving in a Magnetic Field

机译:关于电荷在磁场中运动的系统的哈密顿量

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The Hamiltonian for a system of charges moving in a static magnetic field is considered. It was brought to light that the magnetic energy, introduced commonly in the system, leads to a total annihilation of the kinetic energy of the system in the plane perpendicular to the magnetic field. Thus both the magnetic energy and the coincident momenta of charges terms disappear from the Hamiltonian, This has not been noted to date. The partial derivative of the Hamiltonian with respect to the magnetic field or to the considered momenta vanishes, whereupon the canonical transformations, a statistical sum, and the magnetic moment of the system turn out to be illusory. It is noted that the Hamiltonian function cannot be applied to the charges moving in a magnetic field at all because in this case the system becomes nonholonomic.
机译:考虑了在静磁场中移动的电荷系统的哈密顿量。人们发现,系统中通常引入的磁能导致系统在垂直于磁场的平面中完全抵消了动能。因此,磁能和同时的电荷动量项都从哈密顿量中消失了。迄今为止,这还没有被注意到。哈密​​顿量相对于磁场或所考虑的矩的偏导数消失了,于是规范变换,统计和以及系统的磁矩变得虚幻。注意,汉密尔顿函数根本不能应用于在磁场中移动的电荷,因为在这种情况下,系统变得不完整。

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