156 Mr. G. von Kau£mann on th 



e Theory of Corresponding 





VAN DER WAALS. 



D. Bertiielot. 



Clausius. 



0i 

 =v 1 /b. 



X 



X 



K^ri^i ) , 



3+-*-g*»+ 





*,w 2 . 





A,Z+^W 2 

 (1+*).X 



02 



1 = V.Jb. 



TT 



=pja. 



i 



(l+O- x 



+(3-^r+ )■ 



3-'+|' 2 + 



(l + 0-X 2 Y 



* 2 . vv^wv 



(!)'• 



(1 + 0-Y 



w x .w 2 .z 



i 



7T (Berthelot) 

 ; (1+X)i 



J 



ar-'^-W )• 



«i-(- 



->•••)• 



9 

 =T/c. 



X . Z 2 



® 



z 



] 



Wi . w 2 



(Berthelot) 

 . (1+X)* 



) 



l-(l-4- )• 



4 •/ 



1 1- 



3.6 2 V 



- 7 V+ )• 



""01 



_ M pv, 

 R * T ' 



(1 + .WiY 

 Z 2 





(l + O-Y.^Z + tWO 



(l-f\).*Z 2 



H'-iiW 



2A+3 

 ' ' 8(1 + X) + 



"02 



M pv^ 



W 2 Y 

 Z 2 



Y.(\Z + *W 2 ) 

 (1 + \).*Z 2 



8 8' + 16&' + -- 



2X+3 





L.Z 

 Y 





2L.Z 

 Y 



4+ i5^ + 



i 



7 +lV + 



9 



M.r 

 ~R.T* 



L 



' 



2L-X 

 Z 



*-5« , + 



J-(- 



5*+ )• 



* p is here written for the reduced Latent Heat: p=rjab. 



