CHAPTER VIII.
EXPLORATION OF THE FIELD BY MEANS OF THE SECONDARY CIRCUIT.
585.] We have proved in Arts. 582, 583, 584 that the electromagnetic action between the primary and the secondary circuit depends on the quantity denoted by M, which is a function of the form and relative position of the two circuits.
Although this quantity M is in fact the same as the potential of the two circuits, the mathematical form and properties of which we deduced in Arts. 423, 492, 521, 539 from magnetic and electromagnetic phenomena, we shall here make no reference to these results, but begin again from a new foundation, without any assumptions except those of the dynamical theory as stated in Chapter VII.
The electrokinetic momentum of the secondary circuit consists of two parts (Art. 578), one, Mi1, depending on the primary current i1, while the other, Ni2, depends on the secondary current i2. We are now to investigate the first of these parts, which we shall denote by p, where
| (1) |
We shall also suppose the primary circuit fixed, and the primary current constant. The quantity p, the electrokinetic momentum of the secondary circuit, will in this case depend only on the form and position of the secondary circuit, so that if any closed curve be taken for the secondary circuit, and if the direction along this curve, which is to be reckoned positive, be chosen, the value of p for this closed curve is determinate. If the opposite direction along the curve had been chosen as the positive direction, the sign of the quantity p would have been reversed.
586.] Since the quantity p depends on the form and position of the circuit, we may suppose that each portion of the circuit
