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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

机译:经典的周期运动和周期解的积分   具有末端质量的相对论串的方程。一,积分   周期性运动

摘要

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)$.
机译:相对论的弦在末端具有质量的边界方程是根据弦的世界质量轨迹的几何不变量来计算的。在三维Minkowski空间$ 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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  • 作者

    Barbashov, B. M.;

  • 作者单位
  • 年度 1996
  • 总页数
  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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