Page:Benton 1959 The Clock Problem (Clock Paradox) in Relativity.djvu/9

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10. Benedicks, Carl.SPACE AND TIME. AN EXPERIMENTAL PHYSICIST'S CONCEPTION OF THESE IDEAS AND OF THEIR ALTERATION. 98p., London, Methuen, 1924.

Time, p.19-30.

11. Bergmann, O.COMMENTS ON THE CLOCK PARADOX. Acta Phys. Austriaca 11:377-389, 1957.

In German. Not examined.

12. Bergmann, P. G.FIFTY YEARS OF RELATIVITY. American Astronautical Society. Proceedings, 3rd, Dec. 6-7, 1956, p.135-155, New York, The Society, 1957.

The special and general theories of relativity and the significance of these concepts are reviewed with brief mention of the clock paradox.

13. Bickerdike, C. H.RELATIVITY CLOCKS AND MEASURING RODS. Phil. Mag. 45:327-335, Feb.1923.

The author convicts, by quotations, even such experts as Einstein and Eddington of confusing the minds of readers of their popular writings on relativity by the use of language naturally interpretable as ascribing physical reality to the supposed behavior of the purely conventional contracting measuring rods and compensating clocks assumed for the purpose of popular explanation.

14. Blackett, P. M. S.FURTHER MEASUREMENTS OF THE COSMIC-RAY ENERGY SPECTRUM. Roy. Soc. London Proc. A. 159:1-18, Mar. 1937.

Measurements on the momentum distribution of µ mesons at sea-level. F.S. Crawford (See Item 45) connects this with his clock paradox assumptions.

15. Bollert, Karl.DAS HOMOGENE GRAVITATIONSFELD UND DIE LORENTZTRANSFORMATIONEN. Z. Phys. 10:256-266, 1922.

In German.

Translated title: The homogeneous gravitation field and the Lorenz transformation.

"The connection between the special and the general theory of relativity lies in that in any given gravitational field, local rigid systems of reference exist for every point at which the special theory of relativity is valid. For all freely moving bodies whose masses are so small that their effect on the field can be neglected, the gravitational acceleration is nil at a point with reference to an infinitesimal system of reference which is freely moving and therefore participates in the gravitational motion. In such a local inertial system

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