Equation of motion for non-geodesic laboratory bodies
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Abstract
The gravitational equation of motion of laboratory bodies made up of electrically interacting molecules, the bodies being coupled to non-geodesic laboratories, is obtained for metrical theories of gravity. Application is made to the experiment of Witteborn and Fairbank in which electrons or positrons are ‘dropped’ inside a conducting shield. We show that the inertial and gravitational weight of a body depends on the location of the supporting force, and that a laboratory body, in general, possesses an inertial or gravitational masstensor which differs from the body's energy content divided by the speed of light squared.
Keywords
Field Theory Elementary Particle Quantum Field Theory Energy Content Supporting Force
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References
- Nordtvedt, K. Jr. (1968).Physical Review 169 (5), 1017.Google Scholar
- Nordtvedt, K. Jr. (1970).International Journal of Theoretical Physics Vol. 3, No. 2, p. 133.Google Scholar
- Nordtvedt, K. Jr. (1973). Submitted toAmerican Journal of Physics.Google Scholar
- Schiff, L. I. and Barnhill, M. V. (1966).Physical Review 151, 1067.Google Scholar
- Schiff, L. I., private communication.Google Scholar
- Witteborn, F. C. and Fairbank, W. M. (1967).Physical Review Letters 19, 1049.Google Scholar
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© Plenum Publishing Company Limited 1974