The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
From inside the book
Results 1-5 of 88
Page 1
... distance r apart be denoted by 3A1m12 / r , and that between two molecules M2 by 3A2m22 / 4 , then the attraction between an M , and an M , is or the attraction of two unlike molecules is equal to the square root of the product of the ...
... distance r apart be denoted by 3A1m12 / r , and that between two molecules M2 by 3A2m22 / 4 , then the attraction between an M , and an M , is or the attraction of two unlike molecules is equal to the square root of the product of the ...
Page 4
... distance x from it will be n1 + xdn1 / dx . The number of molecules leaving an element de after encounter in it to cross the plane before the next encounter must be proportional to n + xdn / dx , to da , to the mean number of collisions ...
... distance x from it will be n1 + xdn1 / dx . The number of molecules leaving an element de after encounter in it to cross the plane before the next encounter must be proportional to n + xdn / dx , to da , to the mean number of collisions ...
Page 6
... distance of the liquid surface below the open end of the tube , where Pi is 0 while at the liquid surface it is p , the saturation- pressure of the liquid at the temperature of the experiment , then dlog ( p — p1 ) / dx = log p— log ( p ...
... distance of the liquid surface below the open end of the tube , where Pi is 0 while at the liquid surface it is p , the saturation- pressure of the liquid at the temperature of the experiment , then dlog ( p — p1 ) / dx = log p— log ( p ...
Page 63
... distance between adjacent molecules is the same in the neighbourhood of each point . If the metallic body is subjected to electrostatic induction , it is easy to see that no electric influence from without can penetrate far beyond the ...
... distance between adjacent molecules is the same in the neighbourhood of each point . If the metallic body is subjected to electrostatic induction , it is easy to see that no electric influence from without can penetrate far beyond the ...
Page 65
... distances which rise of temperature produces ; and it is evident that ( on our model ) the specific heat of electricity for any metal is equal to the rise of conduction - potential for one degree rise of tem- perature . Phil . Mag . S ...
... distances which rise of temperature produces ; and it is evident that ( on our model ) the specific heat of electricity for any metal is equal to the rise of conduction - potential for one degree rise of tem- perature . Phil . Mag . S ...
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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