电磁场中扩展带电粒子的Poincare不变运动方程
Full Poincare-invariant equation of motion for an extended charged particle in an electromagnetic field
摘要:
对于任意电磁场中扩展电荷的刚性非旋转运动,通过对作用在电荷上的4-洛伦兹力=外力4+自身力4的洛仑兹不变式计算,导出了其运动方程。运动方程在任何完整的庞加莱变换下都是不变的。这是一个微分积分方程的粒子的4-中心在闵可夫斯基空间作为一个函数的适当的时间。在给定初始条件和外电磁场且迭代过程收敛的情况下,运动方程的二重真时积分形式适于迭代求解。各种近似的自我力,也与运动方程,推导出来。近似的运动方程求解了两个例子:(1)在均匀电场中的直线双曲运动。(2)均匀磁场中的螺旋(非相对论)运动。在这两种情况下,结果都非常简单。讨论了该运动方程相对于其他运动方程(如Lorentz-Dirac方程)的优越性。关键词:运动方程,扩展带电粒子,自作用力,有效惯性质量。
英文摘要:
For the rigid, nonrotating motion of an extended charge in an arbitrary electromagnetic field, an equation of motion is derived by Lorentz-invariantly calculating the 4-Lorentz force = external 4-force + 4-self-force, acting upon the charge. The equation of motion is invariant under any full Poincare transformation. It is a differential-integral equation for the particle's 4-centre in Minkowski space as a function of proper time. The twofold proper time integrated form of the equation of motion is suited to derive the solution iteratively if the initial conditions and the external electromagnetic field are given and the iteration procedere converges. Diverse approximations for the self-force, and with that also for the equation of motion, are derived. The (approximated) equation of motion is solved for two examples: (1) Rectilinear hyperbolic motion in a homogeneous electric field. (2) Spiral (nonrelativistic) motion in a homogeneous magnetic field. In both cases amazingly simple solutions result. The advantages of the equation of motion against other ones, for example the Lorentz-Dirac equation, are discussed. Keywords: Equation of motion, extended charged particle, self-force, effective inertial mass.
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