Proceedings of the Royal Society of London, Volume 58Taylor & Francis, 1895 - Electronic journals Obituary notices of deceased fellows were included in v. 7-64; v. 75 is made up of "obituaries of deceased fellows, chiefly for the period 1898-1904, with a general index to previous obituary notices"; the notices have been continued in subsequent volumes as follows: v. 78a, 79b, 80a-b- 86a-b, 87a 88a-b. |
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Page 1
... Received February 21 , -Read March 15 , 1894 . ( From the Laboratory of the Pathological Department of University College , London . ) A. Object and Method of the Research . 1. Introduction . - This piece of work was undertaken at the ...
... Received February 21 , -Read March 15 , 1894 . ( From the Laboratory of the Pathological Department of University College , London . ) A. Object and Method of the Research . 1. Introduction . - This piece of work was undertaken at the ...
Page 24
... Received November 14 , -Read November 22 , 1894 . The temperature of the positive pole of the electric arc , which is now generally believed to be the boiling point of carbon , is usually taken , on the authority of Violle , * as ...
... Received November 14 , -Read November 22 , 1894 . The temperature of the positive pole of the electric arc , which is now generally believed to be the boiling point of carbon , is usually taken , on the authority of Violle , * as ...
Page 25
... receiving surfaces within . The diameter of the aperture at A is accurately known ; as also is its distance from the receiving - surface , so that the apparent area of platinum , as seen from the latter , may be calculated . L is the ...
... receiving surfaces within . The diameter of the aperture at A is accurately known ; as also is its distance from the receiving - surface , so that the apparent area of platinum , as seen from the latter , may be calculated . L is the ...
Page 27
... receiving surface of the radio - micrometer , and q = ƒ ( T ) be the " law of radiation " for a black surface , where q = quantity of radiation as a function of the absolute temperature T1 of the radiating surface . Then the radiation ...
... receiving surface of the radio - micrometer , and q = ƒ ( T ) be the " law of radiation " for a black surface , where q = quantity of radiation as a function of the absolute temperature T1 of the radiating surface . Then the radiation ...
Page 33
... receiving - surface of the radio- micrometer , and the incandescent platinum on the lower , the position is denoted as Position A , the reverse , by Position B. The angle subtended by the area of incandescent platinum , in both cases ...
... receiving - surface of the radio- micrometer , and the incandescent platinum on the lower , the position is denoted as Position A , the reverse , by Position B. The angle subtended by the area of incandescent platinum , in both cases ...
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acid æther argon atom average bichromate blue brain broth carbon Cayley cell centre chemical chlorine chromospheric corpus callosum cortex culture curve dark degenerate fibres discharge effect elastic electric electromotive force electrons experiments Extensometer F.R.S. Received fasciola cinerea filament fissure of Rolando further gases gelatine germination give given glass growth heat hydrogen hydrogen iodide hydrogen lines inch internal capsule Interval investigation iodide Journal later length lesion light lines load London LVIII Lyginodendron means measurements ments method microscope mins minutes molecule motion movement negative Normal doubling period observations obtained oxygen paper passing plate platinum positive posterior pressure Professor radiation rays refractive index rodlet Royal screens segment selenium septa septum side Society sodium spectra spectrum spores star surface Temp temperature theory thermometer tion tons tube uraninite velocity دو