The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
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Results 1-5 of 47
Page 8
... ratio { 1+ ( m1 + m2 ) ƒ ( 1 / a1 + a2 ) / V2 } . Now v12 and v22 denoting the mean squared velocities of m1 and ma , and V2 = v12 + vy2 = 3 ( k12 + K22 ) , k12 + k22 = k12 ( 1 + k22 / k12 ) = x12 ( 1 + m1 / m2 ) , so that the ratio ...
... ratio { 1+ ( m1 + m2 ) ƒ ( 1 / a1 + a2 ) / V2 } . Now v12 and v22 denoting the mean squared velocities of m1 and ma , and V2 = v12 + vy2 = 3 ( k12 + K22 ) , k12 + k22 = k12 ( 1 + k22 / k12 ) = x12 ( 1 + m1 / m2 ) , so that the ratio ...
Page 9
... ratio of D2 to D , at any two temperatures T , and T , we can calculate from ( 8 ) a value of 1C2 which is a measure of the potential energy of molecules 1 and 2 in contact . Loschmidt was the first to measure diffusion - coefficients ...
... ratio of D2 to D , at any two temperatures T , and T , we can calculate from ( 8 ) a value of 1C2 which is a measure of the potential energy of molecules 1 and 2 in contact . Loschmidt was the first to measure diffusion - coefficients ...
Page 11
... Ratio .... 455 1.4 196 796 • 92 1.4 O , & H2 . O , & N2 . O2 & CO . 10 - 1 ( M1ẞ12C1 M2ß2 2C2 ) 3 106 246 220 Ratio ....... 1.2 1.16 1.1 The mean value of the ratio is 1.2 , and the departures of some of the individual numbers from the ...
... Ratio .... 455 1.4 196 796 • 92 1.4 O , & H2 . O , & N2 . O2 & CO . 10 - 1 ( M1ẞ12C1 M2ß2 2C2 ) 3 106 246 220 Ratio ....... 1.2 1.16 1.1 The mean value of the ratio is 1.2 , and the departures of some of the individual numbers from the ...
Page 14
... ratio of the potential energy at contact to the mean kinetic energy in such a manner as to make the final effect of the forces acting during the collision of molecules the same as if the molecules were both forceless and perfectly resti ...
... ratio of the potential energy at contact to the mean kinetic energy in such a manner as to make the final effect of the forces acting during the collision of molecules the same as if the molecules were both forceless and perfectly resti ...
Page 44
... ratio to the range itself . This was first shown by Lord Kelvin and , more recently , was confirmed by Tomlinson . When the range is increased this law no longer holds , the logarithmic decrement becoming larger . In experiment C the ...
... ratio to the range itself . This was first shown by Lord Kelvin and , more recently , was confirmed by Tomlinson . When the range is increased this law no longer holds , the logarithmic decrement becoming larger . In experiment C the ...
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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