The London, Edinburgh and Dublin Philosophical Magazine and Journal of ScienceTaylor & Francis, 1901 - English periodicals |
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Page 9
... shown to virtually include , not only this vitally important subject , but also the very interesting , though comparatively unimportant , case of an assemblage of particles of equal masses with a single particle of different mass moving ...
... shown to virtually include , not only this vitally important subject , but also the very interesting , though comparatively unimportant , case of an assemblage of particles of equal masses with a single particle of different mass moving ...
Page 14
... large number of vibrational freedoms , and therefore , if the Boltzmann - Maxwell doctrine were true , k - 1 would have some exceedingly small value , such as that shown in the ideal example of § 26 below . 14 Lord Kelvin on the.
... large number of vibrational freedoms , and therefore , if the Boltzmann - Maxwell doctrine were true , k - 1 would have some exceedingly small value , such as that shown in the ideal example of § 26 below . 14 Lord Kelvin on the.
Page 15
shown in the ideal example of § 26 below . On the other hand , Clausius ' theorem presents no difficulty ; it merely asserts that k - 1 is necessarily less than in each of these four cases , as in every case in which there is any ...
shown in the ideal example of § 26 below . On the other hand , Clausius ' theorem presents no difficulty ; it merely asserts that k - 1 is necessarily less than in each of these four cases , as in every case in which there is any ...
Page 16
... we find k - 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.
... we find k - 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
... shown in the 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 ...
... shown in the 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 ...
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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