The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
From inside the book
Results 1-5 of 36
Page 15
... considered , and as the experimenters have reduced their results to values at 0 ° C. by the approximate formula D273 / D = ( 273 / T ) 2 , which is near enough to the truth for small differences between T and 273 , we will take the ...
... considered , and as the experimenters have reduced their results to values at 0 ° C. by the approximate formula D273 / D = ( 273 / T ) 2 , which is near enough to the truth for small differences between T and 273 , we will take the ...
Page 45
... considered further subsequently . Approximate Isochronism of the Oscillations . An experiment was made , immediately after the per- formance of experiment M , to determine the period of oscillation over different ranges . The numbers in ...
... considered further subsequently . Approximate Isochronism of the Oscillations . An experiment was made , immediately after the per- formance of experiment M , to determine the period of oscillation over different ranges . The numbers in ...
Page 46
... considered also that the results showed a loss of energy much greater than any that could be accounted for by imperfection of elasticity . Though the compound - interest law was precisely that which would arise from viscous resistance ...
... considered also that the results showed a loss of energy much greater than any that could be accounted for by imperfection of elasticity . Though the compound - interest law was precisely that which would arise from viscous resistance ...
Page 56
... considered in any of our deductions from the theorem , and for my own part I am persuaded that in reality there is nothing corresponding to the possibility which they suggest . Consider now the case of any body whatever , at any tem ...
... considered in any of our deductions from the theorem , and for my own part I am persuaded that in reality there is nothing corresponding to the possibility which they suggest . Consider now the case of any body whatever , at any tem ...
Page 69
... considered here in § 6 it does not necessarily follow that two conductive particles oppositely charged like A and B ( fig . 1 ) , approaching one another and subject to the influence of an external E.M.F. acting from right to left ...
... considered here in § 6 it does not necessarily follow that two conductive particles oppositely charged like A and B ( fig . 1 ) , approaching one another and subject to the influence of an external E.M.F. acting from right to left ...
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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