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The elastic energy-momentum tensor in special relativity

โœ Scribed by David N Williams


Publisher
Elsevier Science
Year
1989
Tongue
English
Weight
724 KB
Volume
196
Category
Article
ISSN
0003-4916

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โœฆ Synopsis


We consider the standard nonrelativistic theory of a continuous, elastic medium with fmite deformations, according to which the elastic energy is a function only of the state of strain, and the elastic stress tensor is proportional to the strain gradient of the elastic energy in appropriate coordinates.

We derive a special relativistic, energy-momentum tensor, which yields the standard class of theories in the nonrelativistic limit, from the requirement that it depend only on the state of deformation (including the minimal dependence on velocity consistent with covariance), plus conservation laws. The result agrees with an earlier theory proposed by B. Dewitt (in "Gravitation: An Introduction to Current Research" (L. Witten, Ed.), pp. 305-318, Wiley, New York, 1962). who generalized the nonrelativistic Lagrangian to general relativity.

The elastic momentum density turns out to be of order v/c', and therefore absent in the nonrelativistic theory.


๐Ÿ“œ SIMILAR VOLUMES


On redefinitions of the energy momentum
โœ Danilo Villarroel ๐Ÿ“‚ Article ๐Ÿ“… 1975 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 647 KB

We analyse some redefinitions of the energy-momentum tensor of Classical Electrodynamics. Usually it has been considered as a necessary and sufficient criterion for redefining the energy-momentum tensor that the new tensor yields the "true" equation of motion of the electron, that is, the Lorentz-Di