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Non-relativistic model of the laws of gravity and electromagnetism, invariant under the change of inertial and non-inertial coordinate systems

Arkady Poliakovsky

Abstract

Under the classical non-relativistic consideration of the space-time we propose the model of the laws of gravity and Electrodynamics, invariant under the galilean transformations and moreover, under every change of non-inertial cartesian coordinate system. Being in the frames of non-relativistic model of the space-time, we adopt some general ideas of the General Theory of Relativity, like the assumption of invariance of the most general physical laws in every inertial and non-inertial coordinate system and equivalence of factious forces in non-inertial coordinate systems and the force of gravity. Moreover, in the frames of our model, we obtain that the laws of Non-relativistic Quantum Mechanics also invariant under the change of inertial or non-inertial cartesian coordinate system.

Non-relativistic model of the laws of gravity and electromagnetism, invariant under the change of inertial and non-inertial coordinate systems

Abstract

Under the classical non-relativistic consideration of the space-time we propose the model of the laws of gravity and Electrodynamics, invariant under the galilean transformations and moreover, under every change of non-inertial cartesian coordinate system. Being in the frames of non-relativistic model of the space-time, we adopt some general ideas of the General Theory of Relativity, like the assumption of invariance of the most general physical laws in every inertial and non-inertial coordinate system and equivalence of factious forces in non-inertial coordinate systems and the force of gravity. Moreover, in the frames of our model, we obtain that the laws of Non-relativistic Quantum Mechanics also invariant under the change of inertial or non-inertial cartesian coordinate system.

Paper Structure

This paper contains 136 sections, 45 theorems, 3066 equations.

Key Result

Theorem 1.1

Consider that the change of some non-inertial cartesian coordinate system $(*)$ to another cartesian coordinate system $(**)$ is given by noninchgravortbstrjgghguittu2int. Next, assume that in the coordinate system $(**)$ we observe a validity of the Second Law of Newton in the form: where $\mathbf{x}':=\mathbf{x}'(t')$, $\mathbf{u}':=\mathbf{u}'(t')=\frac{d\mathbf{x}'}{dt'}(t')$ and $m'$ are the

Theorems & Definitions (118)

  • Theorem 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Remark 1.1
  • Theorem 1.4
  • Definition 1.1
  • Proposition 1.1
  • Proposition 1.2
  • Definition 1.2
  • Proposition 1.3
  • ...and 108 more