| 1842 - 588 pages
...Journal• Poggennorff's Annalen, and also in a separate work, entitled De Galcanische Kette MatJiematisch Bearbitet,^ published at Berlin in the year 1827....of the electro-motive forces divided by the sum of resistances ; and that whatever be the nature of the current, whether voltaic or thermo-electric, if... | |
| Royal Society (Great Britain) - 1843 - 552 pages
...hitherto been involved in obscurity and doubt. According to Ohm's system, the force of the current is equal to the sum of the electromotive forces divided by the sum of the resistances in the circuit. The several electromotive forces and resistances which enter into the circuit of a... | |
| Royal Society (Great Britain) - 1843 - 416 pages
...inversely proportional to the total resistance of all its parts, or in other words the force of the current is equal to the sum of the electro-motive forces divided by the sum of the resistances. Let F denote the force of the current, E the electro-motive forces, and R the resistances : then The... | |
| Royal Society (Great Britain) - 1843 - 444 pages
...The principle of my process is as follows : — In two circuits, producing equal rheometric effects, the sum of the electro-motive forces divided by the sum of the resist^ •pi pi ances is a constant quantity, ie-gr = ^ ; if E and R be proportionately increased... | |
| Yorkshire Geological Society - 1849 - 576 pages
...proportional to the total resistance of all its parts ; or, in other words, the force of the current is equal to the sum of the electro-motive forces divided by the sum of the resistances." This may be rendered more familiar by experiment. If we take a plate of amalgamated zinc and a plate... | |
| Henry Minchin Noad - 1855 - 566 pages
...positive element. The amount of Electricity realized, or, in other words, the force of the current, is equal to the sum of the electromotive forces, divided by the sum of the resistances in the circuit; thus, let F denote the actual force of the current, E the electromotive force, and... | |
| William Allen Miller - 1855 - 452 pages
...voltaic circuit or circuits : — 'In two circuits producing equal electro-motive (or voltaic) effects, the sum of the electro-motive forces divided by the sum of the resistances is a constant quantity ; ie, ^ = ^-| : if E aud R be proportionately increased or diminished A will... | |
| William Allen Miller - 1855 - 458 pages
...voltaic circuit or circuits : — ' In two circuits producing equal electro-motive (or voltaic) effects, the sum of the electro-motive forces divided by the sum of the resistances is a constant quantity ; ie, ^ = ^-| : if E and R be proportionately increased or diminished A will... | |
| William Allen Miller - 1858 - 244 pages
....?,•!••' TV! I" N&*' »-"^CU3r.*^ ' In two circuits producing equal electro-motive (or voltaic) effects, the sum of the electro-motive forces divided by the sum of the resistances is a constant quantity ; ie, -| = -" * : if E and R be proportionately increased or diminished A will... | |
| George Bartlett Prescott - 1860 - 496 pages
...the resistances of all the parts of the circuit ; in other words, that the intensity of the current is equal to the sum of the electro-motive forces divided by the sum of the resistances." p — H if =5 §5 gs g.- S* SQ«| SS T§ §§•!~ - ' ' ' ' 0060686 ph to, 228. s,m, 1. h, Superi... | |
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