436 OHM ON THE GALVANIC CIRCUIT. 



With the help of this law, which is not altogether imaginary, I 

 now arrive at the equations which make known for each case 

 all the individual circumstances constituting the permanent 

 state of the chemical separation in the galvanic circuit ; I have, 

 however, neglected the further use of them, as the present state 

 of our experimental knowledge in this respect did not appear 

 to me to repay the requisite trouble. Nevertheless, in order to 

 compare in their general features the results of this examination 

 with what has hitherto been supplied by experiments, I have 

 fully carried out one particular case, and have found that the 

 formula represents very satisfactorily the kind of wave of the 

 force, as I have above described it*. 



Having thus given a slight outline of the contents of this 

 Memoir, 1 will now proceed to the fundamental investigation 

 of the individual points. 



* Schweigger's Jahrhuch, 1826. Part 2. 



[To be continued.] 



