The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1894 - English periodicals |
From inside the book
Results 1-5 of 78
Page iii
... Calculating the Position of a Level of no Strain within a Solid Earth , and on the Contraction Theory of Mountains Mr. F. L. O. Wadsworth on an Improved Form of Littrow Spectroscope . ( Plate VI . ) 131 ....... 137 .... Dr. Alexander ...
... Calculating the Position of a Level of no Strain within a Solid Earth , and on the Contraction Theory of Mountains Mr. F. L. O. Wadsworth on an Improved Form of Littrow Spectroscope . ( Plate VI . ) 131 ....... 137 .... Dr. Alexander ...
Page 6
... calculate the 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 ) ...
... calculate the 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 ) ...
Page 9
... calculate from ( 8 ) a value of 1C2 which is a measure of the potential energy of molecules 1 and 2 in contact ... calculated therefrom . The diffusion - coefficients are given in terms of the centimetre and second as units , and ...
... calculate from ( 8 ) a value of 1C2 which is a measure of the potential energy of molecules 1 and 2 in contact ... calculated therefrom . The diffusion - coefficients are given in terms of the centimetre and second as units , and ...
Page 11
... calculated from that equation very sensitive to small errors in the ratio of the diffusion - coefficients at two ... calculate Č2 from the equation 1C2 { ( M1ß1 ) 3 / 2 | ( M2ß2 ) 3 / 2 } 3 = ( M1ß1 1C1 M2ß2 2C2 ) 3 , . ( 9 ) and then by ...
... calculated from that equation very sensitive to small errors in the ratio of the diffusion - coefficients at two ... calculate Č2 from the equation 1C2 { ( M1ß1 ) 3 / 2 | ( M2ß2 ) 3 / 2 } 3 = ( M1ß1 1C1 M2ß2 2C2 ) 3 , . ( 9 ) and then by ...
Page 12
... calculating C2 according to equation ( 9 ) , using therein the values of B and C1 given in the paper on the Viscosity of Gases and Molecular Force , but the calculations would possess more interest if carried out in connexion with the ...
... calculating C2 according to equation ( 9 ) , using therein the values of B and C1 given in the paper on the Viscosity of Gases and Molecular Force , but the calculations would possess more interest if carried out in connexion with the ...
Contents
1 | |
19 | |
36 | |
55 | |
81 | |
89 | |
110 | |
121 | |
279 | |
285 | |
295 | |
301 | |
336 | |
351 | |
358 | |
365 | |
131 | |
137 | |
143 | |
157 | |
159 | |
182 | |
188 | |
198 | |
206 | |
218 | |
225 | |
235 | |
241 | |
248 | |
249 | |
265 | |
271 | |
371 | |
379 | |
386 | |
393 | |
409 | |
421 | |
441 | |
456 | |
473 | |
482 | |
488 | |
505 | |
537 | |
553 | |
567 | |
580 | |
Other editions - View all
Common terms and phrases
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