--- It took a long time to recognize and substantiate the correctness of his (Ohm's) conclusions, as also to know how to apply the law and to be satisfied that all the vagueness concerning the relation between current, tension, and resistance had vanished. Though we possessed standard ohm resistances and Wheatstone bridges, could measure infinity low or high resistances, and could make a shunt of known resistance, yet we did not know a single simple method of determining current. We possessed standard batteries with which, using Thomson's high resistance reflecting galvanometer, we could likewise determine tension (or voltage). Thus we had an easy and practical way the units of resistance and tension (probably should have added the words --- could be measured). Yet no one had the common sense to tell us how to get the current. No budding thinker appeared on the horizon to tell us to measure the resistance of a part of the wire through which the current flowed, and then take the drop of potential on that known resistance, all of which could have been most easily done. With E and R given, the other unit, C, would have appeared. In other words it simply amounted to taking a known shunt and the drop of voltage on it.
Even in 1880 theorists were behind as regards the value of Ohm's law. ---