The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
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Results 1-5 of 57
Page 1
... expression 3A , m , 2 for two like molecules can be split into two parts 3Am1 , the general law of the attraction of any two molecules , like or unlike , can be stated thus : -Any two molecules attract one another with a force inversely ...
... expression 3A , m , 2 for two like molecules can be split into two parts 3Am1 , the general law of the attraction of any two molecules , like or unlike , can be stated thus : -Any two molecules attract one another with a force inversely ...
Page 2
... expression for the force between them is Gm1m2 / r2 + a1a2 / r4 . The dependence of the coefficient of diffusion of two gases on the attraction between their molecules was indicated in general terms in a recent paper on the Viscosity of ...
... expression for the force between them is Gm1m2 / r2 + a1a2 / r4 . The dependence of the coefficient of diffusion of two gases on the attraction between their molecules was indicated in general terms in a recent paper on the Viscosity of ...
Page 4
... expressions are not equal , there is a gain of molecules on one side of the plane and a loss on the other proportional to - 2 ( Ã ̧à ̧dn / dx —Ã1⁄2λdn1⁄2 / dx ) ; and to preserve the uniformity of pressure Meyer supposes a bodily motion ...
... expressions are not equal , there is a gain of molecules on one side of the plane and a loss on the other proportional to - 2 ( Ã ̧à ̧dn / dx —Ã1⁄2λdn1⁄2 / dx ) ; and to preserve the uniformity of pressure Meyer supposes a bodily motion ...
Page 5
... expressions similar to Meyer's . The velocities a1 and a , are determined exactly as in Stefan's method , so that Tait's method labours under this difficulty , that he supposes each molecule of each set to have a certain velocity ...
... expressions similar to Meyer's . The velocities a1 and a , are determined exactly as in Stefan's method , so that Tait's method labours under this difficulty , that he supposes each molecule of each set to have a certain velocity ...
Page 6
... expression ( 2 ) for R , a1 ( 1 + n1 / n ) stands for a1 + a2 , so that if a = 0 the term n1 / n , in R drops out , and the equations ( 3 ) and ( 4 ) , which can be written pia1 = Ddp1 / dx , will in the case of evaporation have to be ...
... expression ( 2 ) for R , a1 ( 1 + n1 / n ) stands for a1 + a2 , so that if a = 0 the term n1 / n , in R drops out , and the equations ( 3 ) and ( 4 ) , which can be written pia1 = Ddp1 / dx , will in the case of evaporation have to be ...
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acid ampere amplitude angle apparatus axis Boyle's law calculated capillary carbon dioxide carbonic acid cell centim centimetre circuit Clark cell coefficient coil condensation constant copper corresponding curve cylinder deflexion density determined diameter dielectric discharge disk displacement distance effect electrical electrodes electromotive force energy equal equation experiments gabbro galvanometer gases gauge give given glass gutta-percha heat hydrogen increase induction iron J. J. Thomson layer length liquid magnetic maximum McLeod gauge means measured megohms mercury metal method metre millim mirror molecular molecules motion nitrogen observed obtained ohms oscillations oxygen paper particles Phil phosphorescence phosphorus plane plate poles position potential pressure prism Prof quantity quaternion radius ratio rays readings resistance rotation solution spectrum sun-heat surface surface-tension telephone temperature theory tion tube vapour velocity vibration volts volts volts volume wave-length waves wire zero