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Thomas precession for spin and for a rod

机译:托马斯旋转和杆

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In this paper we obtain the differential equations which describe the rotating rod and precession of the spin of a gyroscope moving along a curved trajectory. Several examples of such motion are considered. The obtained equations differ from the traditional Thomas expression, interpreted as a rotation of the noninertial frame relative to the fixed one. The cause of this disagreement is the fact that, in general, the axes of the moving frame are not orthogonal for the fixed observers. When the velocity changes, the axes' direction changes, due to both Wigner rotation and Lorentz contraction. In the present paper we take into account both of these factors. It is shown that the vectors representing various physical quantities transform in different ways in the moving reference frame. Thus, the kinematic equations describing the motion of these quantities in a fixed frame are different as well.
机译:在本文中,我们获得了描述沿弯曲轨迹移动的陀螺旋转旋转杆和旋转旋转杆和动力的微分方程。 考虑了这种运动的几个例子。 所获得的方程与传统的托马斯表达不同,解释为相对于固定的框架的旋转。 这种分歧的原因是事实上,通常,移动框架的轴线对于固定观察者来说不是正交。 当速度变化时,由于Wigner旋转和洛伦兹收缩,轴的方向改变。 在本文中,我们考虑到这两个因素。 结果表明,在移动参考帧中以不同的方式表示各种物理量的载体。 因此,描述固定框架中这些数量运动的运动学方程也不同。

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