General frame transformations between inertial observers are simplified by imposing three kinematical conditions. A theorem is proved that such conditions ultimately correspond to a suitable choice of the coordinates in the two frames. Accordingly, the three kinematical conditions do not imply any genuine restriction. A further, restrictive, condition concerning rotational invariance is imposed, so determining the final form of the frame transformation
Ever since the work of von Ignatowsky circa 1910 it has been known (if not always widely appreciated...
We present a new method for describing the kinematics of the rotational motion of a rigid body. The ...
A simplified and then general demonstration is presented here showing that the transformation formul...
Frame transformations between inertial observers can be conveniently analyzed by introducing a suita...
The projector operator formalism is used to deduce the relationships between all the quantities invo...
The Galilean transformation, relating the velocities of a particle observed in two different frames ...
The transformation of coordinates and time from an inertial frame to another inertial frame is obta...
Unlike the Lorentz transformation which replaces the Galilean transformation among inertial frames a...
Abstract. Transformation equations for the space-time coordinate, for the momentum and the energy an...
In the article, the whole class of time and position transformations was derived. These transformati...
By proper co-ordinates of non-inertial observers (shortly- proper non-inertial co-ordinates) we unde...
We reveal the frame-exchange space-inversion (FESI) symmetry and the frame-exchange time-inversion (...
This paper outlines the procedure of calculating inertial acceleration in a kinematic system involvi...
Several new ideas related to Special and General Relativity are proposed. The black-box method is us...
Assuming a general timelike congruence of worldlines as a reference frame, we derive a covariant gen...
Ever since the work of von Ignatowsky circa 1910 it has been known (if not always widely appreciated...
We present a new method for describing the kinematics of the rotational motion of a rigid body. The ...
A simplified and then general demonstration is presented here showing that the transformation formul...
Frame transformations between inertial observers can be conveniently analyzed by introducing a suita...
The projector operator formalism is used to deduce the relationships between all the quantities invo...
The Galilean transformation, relating the velocities of a particle observed in two different frames ...
The transformation of coordinates and time from an inertial frame to another inertial frame is obta...
Unlike the Lorentz transformation which replaces the Galilean transformation among inertial frames a...
Abstract. Transformation equations for the space-time coordinate, for the momentum and the energy an...
In the article, the whole class of time and position transformations was derived. These transformati...
By proper co-ordinates of non-inertial observers (shortly- proper non-inertial co-ordinates) we unde...
We reveal the frame-exchange space-inversion (FESI) symmetry and the frame-exchange time-inversion (...
This paper outlines the procedure of calculating inertial acceleration in a kinematic system involvi...
Several new ideas related to Special and General Relativity are proposed. The black-box method is us...
Assuming a general timelike congruence of worldlines as a reference frame, we derive a covariant gen...
Ever since the work of von Ignatowsky circa 1910 it has been known (if not always widely appreciated...
We present a new method for describing the kinematics of the rotational motion of a rigid body. The ...
A simplified and then general demonstration is presented here showing that the transformation formul...