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Classical dynamics with curl forces, and motion driven by time-dependent flux

机译:带有弯曲力的经典动力学,以及由时变磁通驱动的运动

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摘要

For position-dependent forces whose curl is non-zero (curl forces), there is no associated scalar potential and therefore no obvious Hamiltonian or Lagrangean and, except in special cases, no obvious conserved quantities. Nevertheless, the motion is nondissipative (measure-preserving in position and velocity). In a class of planar motions, some of which are exactly solvable, the curl force is directed azimuthally with a magnitude varying with radius, and the orbits are usually spirals. If the curl is concentrated at the origin (for example, the curl force could be an electric field generated by a changing localized magnetic flux, as in the betatron), a Hamiltonian does exist but violates the rotational symmetry of the force. In this case, reminiscent of the Aharonov-Bohm effect, the spiralling is extraordinarily slow.
机译:对于卷曲非零的位置相关力(卷曲力),没有关联的标量势,因此没有明显的哈密顿量或拉格朗日根,并且在特殊情况下,没有明显的守恒量。然而,该运动是无耗散的(位置和速度保持量度)。在一类平面运动中,其中一些可以完全解决,卷曲力沿方位角指向,其幅度随半径而变化,并且轨道通常为螺旋形。如果卷发集中在原点(例如,卷发力可能是由变化的局部磁通量产生的电场,例如在电子感应加速器中),则哈密顿量确实存在,但违反了力的旋转对称性。在这种情况下,使人联想起阿哈罗诺夫-鲍姆效应,螺旋运动异常缓慢。

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