The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
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Results 1-5 of 90
Page iv
... Surface - Pressure Prof. John Trowbridge on Electrical Resonance and Electrical Interference . ( Plate VII . ) 161 182 Mr. William Sutherland on the Attraction of Unlike Mole- cules . - II . The Surface - Tension of Mixed Liquids Mr ...
... Surface - Pressure Prof. John Trowbridge on Electrical Resonance and Electrical Interference . ( Plate VII . ) 161 182 Mr. William Sutherland on the Attraction of Unlike Mole- cules . - II . The Surface - Tension of Mixed Liquids Mr ...
Page 6
... 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 — p . ) , h and the ...
... 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 — p . ) , h and the ...
Page 35
... surface . A difficulty , however , now presents itself , inasmuch as a liquid cooled below its melting- point ( unlike the corresponding case for vapours ) can be kept in a solid vessel without solidifying . Hence the method for ...
... surface . A difficulty , however , now presents itself , inasmuch as a liquid cooled below its melting- point ( unlike the corresponding case for vapours ) can be kept in a solid vessel without solidifying . Hence the method for ...
Page 57
... surface of the body . Thus the perfectly conductive bodies in Theorem I. may be replaced by perfectly conductive surfaces , without altering any of our conclusions ; but it would be hard to decide whether a perfectly conductive ...
... surface of the body . Thus the perfectly conductive bodies in Theorem I. may be replaced by perfectly conductive surfaces , without altering any of our conclusions ; but it would be hard to decide whether a perfectly conductive ...
Page 63
... surface ; for the outer particles of the superficial molecules , owing to their intermittent contacts with one another , will screen the interior of the metal as a network of continuous wires might do , and at a depth of a very few ...
... surface ; for the outer particles of the superficial molecules , owing to their intermittent contacts with one another , will screen the interior of the metal as a network of continuous wires might do , and at a depth of a very few ...
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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