The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1901 - English periodicals |
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Page 16
... 1 = = j j + 2 ' 1 3 ( 1 + j ) The values of k 1 thus calculated for a triatomic and tetra- tomic gas , and calculated as above in Ex . 3 for a diatomic - gas , are shown in the following table , and 16 Lord Kelvin on the.
... 1 = = j j + 2 ' 1 3 ( 1 + j ) The values of k 1 thus calculated for a triatomic and tetra- tomic gas , and calculated as above in Ex . 3 for a diatomic - gas , are shown in the following table , and 16 Lord Kelvin on the.
Page 17
... table . The values of k - 1 for all the gases are less than 3 , as they must be when there is any appreciable energy of rotation or vibration in the molecule . They are different for different diatomic gases ; ranging from 41 for oxygen ...
... table . The values of k - 1 for all the gases are less than 3 , as they must be when there is any appreciable energy of rotation or vibration in the molecule . They are different for different diatomic gases ; ranging from 41 for oxygen ...
Page 22
... table ; the boundary being of any shape whatever , instead of the ordinary rect- angular boundary of an ordinary billiard - table , and being perfectly elastic . An interesting illustration , easily seen * Phil . Mag . , January 1900 ...
... table ; the boundary being of any shape whatever , instead of the ordinary rect- angular boundary of an ordinary billiard - table , and being perfectly elastic . An interesting illustration , easily seen * Phil . Mag . , January 1900 ...
Page 35
... table . The number of times each velocity occurs was chosen to fulfil as nearly as may be the Maxwellian law , v2 which is Cdve the number of velocities between v + adv and v - dv . We took k = 1 , which , if de were infinitely small ...
... table . The number of times each velocity occurs was chosen to fulfil as nearly as may be the Maxwellian law , v2 which is Cdve the number of velocities between v + adv and v - dv . We took k = 1 , which , if de were infinitely small ...
Page 36
... TABLE SHOWING THE NUMBER OF THE DIFFERENT VELOCITIES ON THE DIFFERENT CARDS . Velocity . • 1 2 3 4 5 6 7 8 9 10 11 12 11 12 13 14 15 16 17 18 19 20 21 2-2 1 Card 1 100 2 17 7 93 10 90 99 " 9 19 99 4 5 6 991 184 15 60 40 2657 17 31 40 29 ...
... TABLE SHOWING THE NUMBER OF THE DIFFERENT VELOCITIES ON THE DIFFERENT CARDS . Velocity . • 1 2 3 4 5 6 7 8 9 10 11 12 11 12 13 14 15 16 17 18 19 20 21 2-2 1 Card 1 100 2 17 7 93 10 90 99 " 9 19 99 4 5 6 991 184 15 60 40 2657 17 31 40 29 ...
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æther apparatus atom bismuth calculated carbon cathode centim centre charge coil component condenser condensing-plates constant corresponding Crémieu crystal Crystallographic Axis curve cyanogen deflexion density diameter dielectric direction discharge disk distance effect electric electrodes electrometer electromotive force element equal equation equilibrium experiments field force formula frequency function galvanometer gases given gives harmonic heat Hence hydrogen increase ionization ions J. J. Thomson kilometres per second kinetic energy length light lines liquid magnetic mean measured metal method millimetres molecules motion needle negative ions observed obtained paper particles period Phil phosphorus plane plate positive potential pressure produced quaternions radiation radius ratio resistance reversed rotation sectors space spectra spectrum spheres suppose surface TABLE temperature theory tube vary velocity vibrations volts volume Voss machine wave-length waves wire zero