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s divided into two equal halves, the _negative half_ is plainly that which joins the _positive post_, and the _positive half_ that which joins the _negative post_. From this it will be seen that what in practice are designated as the positive and negative _posts_, and also positive and negative _poles_ or _electrodes_ are _not_ such _in relation to each other_, but the _reverse_ of it; that is to say, the positive _post_ is not _positive_ in relation to the _negative post_, but is _negative_ to it; and the positive _electrode or pole_ is not positive in relation to the _negative_ electrode, but _negative_ to it. The positive _post_, like the positive _electrode_, is called _positive_, because it is the positive end of the sectional magnet next _behind_ it. And the _negative_ post, as also the negative electrode, is _called negative_ because it is the negative end of the sectional magnet next _in advance_ of it. THE CENTRAL POINT OF THE CIRCUIT. _The central point_ of the circuit--that point which divides between its positive and negative halves--is reckoned, in practice, to be the midway point in the line over which the current passes, in its whole course from the positive post around to the negative post. When the cords are of equal length, this point will always be in the person of the patient, about midway between the parts where the two electrodes are applied. This central point, or "point of centrality," is practically neuter--neither positive nor negative; and upon the two opposite halves of the circuit, the positive and negative _qualities_ of the current are in greatest force nearest to the posts, and in least force nearest to the central point. At this point they cease altogether, and the central point is _neuter_. It may, perhaps, be observed that, in _apparent_ contradiction of this statement, the _sensational_ effect of the current on the negative half of the circuit is _least_ nearest to the positive post, and becomes regularly _greater_ as the current advances towards the central point; and that _at_ this point it is greater than at any other point between this and the positive post. To relieve this seeming contradiction, it is only necessary to consider that, in fact, the _positive_ state on the negative half of the current _does_ increase regularly from the positive post to the central point. But that which is the _increase_ of the positive state is the _decrease_ of the negative state. So it i
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