Philosophical MagazineTaylor & Francis, 1913 - Physics |
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Page 33
Eliminating dp between equations ( 3 ) and ( 5 ) we obtain the equation 8 ( 1 + 8 ) ds v ( x , p , 0 ) ds v ( s , p , 0 ) = dG So ( s , p , 0 ) ( 6 ) This equation is due to Duhem * , who deduced it from first principles . It has also ...
Eliminating dp between equations ( 3 ) and ( 5 ) we obtain the equation 8 ( 1 + 8 ) ds v ( x , p , 0 ) ds v ( s , p , 0 ) = dG So ( s , p , 0 ) ( 6 ) This equation is due to Duhem * , who deduced it from first principles . It has also ...
Page 34
... equation which is the ordinary equation of hydrostatic equilibrium . By the above device we are able to deduce immediately the Gibbs equation for the solvent in the solution by means of the coexisting column of solvent vapour . The ...
... equation which is the ordinary equation of hydrostatic equilibrium . By the above device we are able to deduce immediately the Gibbs equation for the solvent in the solution by means of the coexisting column of solvent vapour . The ...
Page 152
... equation m = mo for the mass of a moving body , where m 。 is √1 - q3 / c2 the mass of the body at rest and q is its velocity . By sub- stitution of equation ( 12 ) we may obtain the following equation for transforming measurements of ...
... equation m = mo for the mass of a moving body , where m 。 is √1 - q3 / c2 the mass of the body at rest and q is its velocity . By sub- stitution of equation ( 12 ) we may obtain the following equation for transforming measurements of ...
Contents
SIXTH SERIES | 1 |
Dr N Bohr on the Theory of the Decrease of Velocity | 10 |
Dr S A Shorter on the Application of the Theory | 31 |
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