relativistic mechanics

This was very important for the development of relativistic mechanics after 1900.

This idea had to be given up, however, in the course of the development of relativistic mechanics.

In relativistic mechanics time and length scales are related by the speed of light.

This inconsistency was resolved by the development of relativistic mechanics.

The theory used by physicists was thereafter changed from Newtonian to relativistic mechanics.

In relativistic mechanics, this is only a good approximation when v is much less than the speed of light.

Elastic collision in classical and relativistic mechanics.

For example, consider Newtonian mechanics and relativistic mechanics.

For instance, this is the case of non-reltivistic non-autonomous mechanics, but not relativistic mechanics.

The foundations of relativistic mechanics are the postulates of special relativity and general relativity.

Harshaw dug far back into his memory and recalled the personal tragedy that relativistic mechanics had proved to be for many distinguished scientists.

In addition, the paper claimed, the Foucault pendulum experiment "cannot be explained satisfactorily in either classical or relativistic mechanics".

He could not have done this, since he did not have relativistic mechanics, with which he could model the shell.

However, a number of modern sources do include relativistic mechanics, which in their view represents classical mechanics in its most developed and most accurate form.

To describe relativistic mechanics, one should consider a system of ordinary differential equations on a smooth manifold whose fibration over is not fixed.

Therefore, in anticipation of the transition to relativistic mechanics, the trajectories and curvatures are scaled with the speed of light .

Newtonian mechanics, quantum mechanics, relativistic mechanics.

In relativistic mechanics, the angular momentum of a particle is expressed as an antisymmetric tensor of second order:

As intriguing as geometric Newtonian gravity may be, its basis, classical mechanics, is merely a limiting case of (special) relativistic mechanics.

The fact that no classical body can exceed the speed of light (no matter how much acceleration applied) is a consequence of classical relativistic mechanics.

Relativistic mechanics (i.e. including the special and general theories of relativity), for bodies whose speed is close to the speed of light.

"The Environment in Modern Physics: A Study in Relativistic Mechanics" (1965)

In relativistic mechanics, the spatial coordinates and coordinate time are not absolute; any two observers moving relative to each other can measure different locations and times of events.

In these two examples, quantum mechanics and relativistic mechanics respectively, do predict what is OBSERVED.

"Relativistic Mechanics, Time and Inertia (Fundamental Theories of Physics) " (December 31, 1984)