Philosophical MagazineTaylor & Francis., 1879 - Physics |
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Page 495
... electromotive force E generated by the concentrations z " and z ' of the boundary layers between the two electrodes at the moment t ( > 1 ) , E = A ( : " - ( [ 1 + B ( z ' " + z ' ) ] A4 ( 22-21 ) π sin π π2 ekt - 1 + 2B ( 22-21 ) π ...
... electromotive force E generated by the concentrations z " and z ' of the boundary layers between the two electrodes at the moment t ( > 1 ) , E = A ( : " - ( [ 1 + B ( z ' " + z ' ) ] A4 ( 22-21 ) π sin π π2 ekt - 1 + 2B ( 22-21 ) π ...
Page 496
... electromotive force to be measured , w the resistance of length of the measuring wire , W the total resistance of first circuit , and D the electromotive force of the compe ting Daniell , the expression of the electromotive force to ...
... electromotive force to be measured , w the resistance of length of the measuring wire , W the total resistance of first circuit , and D the electromotive force of the compe ting Daniell , the expression of the electromotive force to ...
Page 531
... electromotive force began an hour and a half after the in- terruption of the current ; accordingly equation ( 13 ) can be employed throughout as perfectly exact . The value of being so considerable , causes the electromotive force to ...
... electromotive force began an hour and a half after the in- terruption of the current ; accordingly equation ( 13 ) can be employed throughout as perfectly exact . The value of being so considerable , causes the electromotive force to ...
Contents
FIFTH SERIES | 1 |
JULY 1879 | 17 |
Mr F Guthrie on the Fracture of Colloids Plates II III | 33 |
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