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Extra resources for Advances in space science and technology. Volume 6

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Phys. 2, 525. Fletcher, J. G. (1962). Geometrodynamics, In "Gravitation, an introduction to current research" (L. ). Wiley, New York, 412. 18. DeWitt, B. S. (1962). Quantization of fields with infinite-dimensional invariance groups. I l l Generalized Schwinger-Feynman Theory. J. Math. Phys. 3, 1073. 19. Popper, D. M. (1954). Red shift in the spectrum of 40 ERIDANI B. Astrophys. J. 120, 316. 20. Mössbauer, R. L. (1958). Kernresonanzfluoreszenz von Gammastrahlung in Ir191. Z. Physik 151, 124. 21.

W. P. (1961). A search for anisotropy of inertial mass using a free precession technique. Phil. Mag. 6, 683. 30. Dicke, R. H. (1961). Experimental tests of Mach's principle. Phys. Rev. Letters 7, 359. 31. Epstein, S. T. (1960). On anisotropy of inertia. Nuovo Cimento 16, 587. 32. Singer, S. F. (1956). " Phys. Rev. 104, 11. 33. Schiff, L. I. (1960). Possible new experimental test of general relativity theory. Phys. Rev. Letters 4, 215. 34. Chiu, H. Y. (1962). Neutrino astronomy. Intern. Set. and Technol.

In a frictionless environment the gradual acceleration of nearly motionless (relatively speaking) bodies over periods of days or even weeks will be easily detectable. ) gravitation constant will be performable with much greater precision than on Earth. It should also be possible to perform a graduated series of gravitational induction experiments in a controlled manner in the laboratory. For example, a massive spherical body could be set in rapid rotation with a speed limited only by its mechanical strength, and small test bodies could be allowed to fall toward it.

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Advances in space science and technology. Volume 6 by III FREDERICK I. ORDWAY

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