Philosophical MagazineTaylor & Francis., 1923 - Physics |
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Page 12
... Equation ( 442 ) refers to the case in which no rotation is impossible ; the molecule of lowest quantum grade has no longer no energy , but energy e Since X retains its old meaning , xe is now the heat of dissociation per molecule ...
... Equation ( 442 ) refers to the case in which no rotation is impossible ; the molecule of lowest quantum grade has no longer no energy , but energy e Since X retains its old meaning , xe is now the heat of dissociation per molecule ...
Page 23
... equation E = Xx + zXkT . This equation is impossible of fulfilment unless E > Xx . The impossibility has of course entered in the limiting process No. The equation must really mean that all the energy goes into lifting the electrons ...
... equation E = Xx + zXkT . This equation is impossible of fulfilment unless E > Xx . The impossibility has of course entered in the limiting process No. The equation must really mean that all the energy goes into lifting the electrons ...
Page 25
... equation for C. To evaluate the integrals for C and CN , we proceed as in §5 . By the arguments there used it ... equations Nr / ( Mr M2r ... Ms ) = Br , ( r = 1 , ... , ) . ( 9.5 ) These equations , j in number , with the s equations ...
... equation for C. To evaluate the integrals for C and CN , we proceed as in §5 . By the arguments there used it ... equations Nr / ( Mr M2r ... Ms ) = Br , ( r = 1 , ... , ) . ( 9.5 ) These equations , j in number , with the s equations ...
Page 27
... equations Etqtr log xt - log x * = - Xr ( Et¶tr - 1 ) ( - log P + § log T ) kT —log Br ( T ) + Σ19tr log { : { " -log ( 2mm ) 3/25/2 { σελι ( 2πm ) 3 / 21,5 / 2 h3 ( r = 1 , ... , j ) . ( 9.82 ) In this equation B , ( T ) is the ...
... equations Etqtr log xt - log x * = - Xr ( Et¶tr - 1 ) ( - log P + § log T ) kT —log Br ( T ) + Σ19tr log { : { " -log ( 2mm ) 3/25/2 { σελι ( 2πm ) 3 / 21,5 / 2 h3 ( r = 1 , ... , j ) . ( 9.82 ) In this equation B , ( T ) is the ...
Page 28
... equation , d log K dT = Qp RT2 ' ( 9.9 ) where Q is the heat of reaction per gram - molecule at constant pressure and K the equilibrium constant ; in particular , we shall see how the term B ( T ) enters the reaction - isobar . By ...
... equation , d log K dT = Qp RT2 ' ( 9.9 ) where Q is the heat of reaction per gram - molecule at constant pressure and K the equilibrium constant ; in particular , we shall see how the term B ( T ) enters the reaction - isobar . By ...
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absorption æther apparatus approximately argon atoms axis calculated carbon dioxide cathode centimetre coefficient collisions constant corresponding curve deflexion density determined diameter dielectric constant discharge distance effect electric electrons emission emitted energy entropy equal equation experimental experiments expression force formula frequency function galvanometer gases give given grid heating helium hydrogen increase intensity ionization potential ions J. J. Thomson light lines liquid magnetic field mass maximum mean measured mercury metal method molecular molecules motion nitrogen nitrous oxide observed obtained orbit paper partition function Phil Phys plane plate polarization positive possible pressure Proc quantity quantum radiation ratio reflexion relative rotation scattering secondary emission shown solution spectra spectrum substance surface Table temperature theorem theory tube vapour velocity vibrations voltage volts wave-length wire zero