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Table of Contents
57

Villard, C. R. 130, pp. 1010, 1178, 1900.

58

Becquerel, C. R. 130, p. 1154, 1900.

59

Rutherford, Phys. Zeit. 3, p. 517, 1902.

60

McClelland, Phil. Mag. July 1904.

61

Paschen, Phys. Zeit. 5, No. 18, p. 563, 1904.

62

A. S. Eve, Phil. Mag. Nov. 1904.

63

Paschen, Annal. d. Physik, 14, p. 114, 1904; 14, 2, p. 389, 1904. Phys. Zeit. 5, No. 18, p. 563, 1904.

64

Paschen, Phys. Zeit. 5, No. 18, p. 563, 1904.

65

Rutherford and Barnes, Phil. Mag. May 1905. Nature, p. 151, Dec. 15, 1904.

66

Barkla, Nature, March 17, 1904.

67

Becquerel, C.R. 132, pp. 371, 734, 1286. 1901.

68

Mme Curie, Thèse présentée à la Faculté des Sciences, Paris 1903, p. 85.

69

A. S. Eve, Phil. Mag. Dec. 1904.

70

In a recent paper (Phil. Mag. Feb. 1905), McClelland has, in the main, confirmed the experimental results obtained by Eve. An electrometer was used instead of an electroscope. He finds, in addition, that the amount of secondary radiation depends on the angle of incidence of the primary rays, and is greatest for an angle of 45°. In a letter to Nature (Feb. 23, p. 390, 1905), he states that more recent experiments have shown that the amount of secondary radiation from different substances is a function of their atomic weights rather than of their densities. In every case examined, the amount of secondary radiation increases with the atomic weight, but is not proportional to it.

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