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V. V. Voytik

Publications and source records attributed to V. V. Voytik.

2 recordsLinked to original sources

The proper characteristics of frame reference as a 4-invariants

The paper proposes 4-dimensional equations for the proper characteristics of a rigid reference frame \[ {{{W}'}^{γ}}=Λ^{0}_{\;\;i}\frac{dΛ^{γi}}{d{t}}\,\,,\] \[ {{{Ω}'}^{γ}}=-\frac{1}{2}\,{{e}^{αμγ}}Λ_{\;\;i}^{μ}\frac{d{{Λ}^{αi}}}{d{t}}\,\,.\] From these conditions follow the law of motion of the proper tetrad and the equations of the inverse problem of kinematics, i.e., differential equations that solve the problem of restoring the motion parameters of a rigid reference frame from known proper acceleration and angular velocity. In particular, it is shown that when boosted, a moving reference frame that has proper Thomas precession relative to the new laboratory frame will have a combination of two rotations: the new Thomas proper precession and the Wigner rotation, which together give the original frequency of Thomas precession $$ \frac{1-\sqrt{1-v^{2}}}{v^{2}\sqrt{1-v^{2}}}\,\,e^{βμν}v^μ\dot{v}^ν=ω'^β_{W} + b^{βα}_{W}\,\frac{1-\sqrt{1-v^{*2}}}{v^{*2}\sqrt{1-v^{*2}}}\,\,e^{αμν}v^{*μ}\dot{v}^{*ν}\,.$$

physics.gen-ph

The transformation of affine velocity and its application to a rotating disk

The aim of the article is to find a transformation that links the local affine velocity of a non-rigid body in the laboratory inertial reference frame $ S $ with the centro-affine velocity of motion of this body in the accompanying accelerated frame $ k $. This paper is based on the kinematics of a continuous medium and the generalized Lorentz transformation. In this paper we show the 3D transformation of velocity linking the reference system $ S $ and the reference system $ k $, which moves without rotation. Wherein the motion of various points of the rigid system $ k $ is inhomogeneous. Using these formulas, we obtain the desired direct and inverse transformation of the local affine velocity. Important special cases of this transformation are considered. They are the motion of particles in a uniform force field and the precession of Thomas. As an example of using the transformation of affine velocity in $ S $, accelerated rotation of the disk was considered and the local angular velocity and the magnitude of the deformation of its points were calculated. Wherein, the calculated stretching coefficient is consistent with the known one, and the formula found for the angular velocity is more general than the earlier result obtained for uniform rotation of the disk.

physics.gen-ph