Tolman, Richard C. (1930) On the use of the energymomentum principle in general relativity. Physical Review, 35 (8). pp. 875895. ISSN 0031899X. doi:10.1103/PhysRev.35.875. https://resolver.caltech.edu/CaltechAUTHORS:TOLpr30c

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Abstract
The primary purpose of this article is to obtain from the general relativity form of the energymomentum principle certain new consequences which are needed for later work that the author has in mind. In addition, it is the intention to give at the same time a somewhat comprehensive and coherent treatment of the principle and its consequences, which it is hoped will increase the confidence and facility of physicists in the use of this important part of the general theory of relativity. In carrying out the investigation, it has seemed desirable for English readers, to take Eddington's "Mathematical Theory of Relativity" as a starting point, and this has incidentally led to a new form of deduction for certain consequences of the energymomentum principle that were already known. After presenting the energymomentum principle in the form discovered by Einstein and showing its application to the case of the conservation of energy in an isolated system, an important expression is derived which gives the total densities of energy and momentum in the form of a divergence. This expression is equivalent to one previously obtained by Einstein but on account of the starting point adopted is derived and expressed in terms of the quantities gμν and gαμν instead of the gμν and gαμν. Following this, the limiting values at large distances from an isolated material system are obtained for the quantities gαβ∂L/∂gγαβ and gα4∂L/∂gγα4. These values, which have considerable use, have not previously received explicit expression. This is followed by a deduction from our present starting point of Einstein's famous relation U=m between the energy and gravitational producing mass of an isolated system. An important expression is then obtained which gives the energy of a quasistatic isolated system in the form of an integral which has to be extended only over the portion of space actually occupied by matter or radiation. This expression has not previously received a satisfactory derivation. The result is used to obtain an expression for the energy of a spherical distribution of a perfect fluid, and it is then shown that this expression, in the case of a sphere of ordinary material, approaches in a sufficiently weak field to the classical expression for energy including the potential gravitational energy. This result is not only intrinsically useful, but also shows for a particular case that a higher order of approximation to the general relativity value for total energy is obtained by including the classical gravitational energy than by going at once to flat spacetime as is often done. Finally, a general consideration is given to the problem of determining the conditions imposed on those changes from one static state to another which could occur in a nonisolated system forming part of a larger static system, without changing the distribution of matter and radiation outside the boundary and without contravening the energymomentum principle as applied to the system as a whole.
Item Type:  Article  

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Additional Information:  ©1930 The American Physical Society. Received 20 December 1930.  
Issue or Number:  8  
DOI:  10.1103/PhysRev.35.875  
Record Number:  CaltechAUTHORS:TOLpr30c  
Persistent URL:  https://resolver.caltech.edu/CaltechAUTHORS:TOLpr30c  
Usage Policy:  No commercial reproduction, distribution, display or performance rights in this work are provided.  
ID Code:  2577  
Collection:  CaltechAUTHORS  
Deposited By:  Tony Diaz  
Deposited On:  11 Apr 2006  
Last Modified:  08 Nov 2021 19:49 
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