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>Integrals of periodic motion and periodic solutions for classical
equations of relativistic string with masses at ends. I. Integrals of
periodic motion
【2h】
Integrals of periodic motion and periodic solutions for classical
equations of relativistic string with masses at ends. I. Integrals of
periodic motion
Boundary equations for the relativistic string with masses at ends areformulated in terms of geometrical invariants of world trajectories of massesat the string ends. In the three--dimensional Minkowski space $E^1_2$, thereare two invariants of that sort, the curvature $K$ and torsion $\kappa$.Curvatures of trajectories of the string ends with masses are always constant,$K_i = \gamma/m_i (i =1,2,)$, whereas torsions $\kappa_i(\tau)$ obey a systemof differential equations with deviating arguments. For these equations withperiodic $\kappa_i(\tau+n l)=\kappa(\tau)$, constants of motion are obtained(part I) and exact solutions are presented (part II) for periods $l$ and $2l$where $l$ is the string length in the plane of parameters $\tau$ and $\sigma \(\sigma_1 = 0, \sigma_2 =l)$.
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机译:相对论的弦在末端具有质量的边界方程是根据弦的世界质量轨迹的几何不变量来计算的。在三维Minkowski空间$ E ^ 1_2 $中,存在两个这样的不变量,即曲率$ K $和扭转$ \ kappa $。具有质量的弦线轨迹的曲率始终恒定,$ K_i = \ γ/ m_i(i = 1,2,)$,而扭转$ \ kappa_i(\ tau)$则服从具有偏差参数的微分方程组。对于这些周期为$ \ kappa_i(\ tau + nl)= \ kappa(\ tau)$的方程,获得运动常数(第一部分),并给出了周期$ l $和$ 2l $的精确解(第二部分),其中$ l $是参数$ \ tau $和$ \ sigma \(\ sigma_1 = 0,\ sigma_2 = l)$平面中的字符串长度。
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