The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
From inside the book
Results 1-5 of 76
Page v
... Velocity of Sound in Air , Gases , and Vapours for Pure Notes of different Pitch Mr. F. W. Hill on the Hatchet Planimeter 249 Prof. John Perry on Magnetic Shielding by a Hollow Iron Cylinder : Simplest Case 265 270 Mr. S. Skinner on the ...
... Velocity of Sound in Air , Gases , and Vapours for Pure Notes of different Pitch Mr. F. W. Hill on the Hatchet Planimeter 249 Prof. John Perry on Magnetic Shielding by a Hollow Iron Cylinder : Simplest Case 265 270 Mr. S. Skinner on the ...
Page 2
... velocity a in one direction , and the other a velocity as in the other , the density of the first diminishes in the direction of a1 , of the second in that of a2 . Consider , then , an element of the first of section unity and length 8x ...
... velocity a in one direction , and the other a velocity as in the other , the density of the first diminishes in the direction of a1 , of the second in that of a2 . Consider , then , an element of the first of section unity and length 8x ...
Page 3
... velocity a collides with one of the second with velocity a in the opposite direction , then R = vμ . If α1 and a , are the radii of the molecules of the two sets treated as spheres , and 3,2 / 2 and 322/2 are their mean square ...
... velocity a collides with one of the second with velocity a in the opposite direction , then R = vμ . If α1 and a , are the radii of the molecules of the two sets treated as spheres , and 3,2 / 2 and 322/2 are their mean square ...
Page 5
... velocity combined with the velocity of agitation , and yet this velocity is different from that of the set as a whole . On theoretical grounds , therefore , Stefan's theory appears . not to have been improved by the later attempts , and ...
... velocity combined with the velocity of agitation , and yet this velocity is different from that of the set as a whole . On theoretical grounds , therefore , Stefan's theory appears . not to have been improved by the later attempts , and ...
Page 6
... velocity of evaporation in terms of the coefficient of diffusion . In the 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 ...
... velocity of evaporation in terms of the coefficient of diffusion . In the 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 ...
Contents
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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