This page needs to be proofread.
x | CONTENTS |
Art. | Page |
---|---|
480. Potential function due to a straight current. It is a function of many values | 130 |
481. The action of this current compared with that of a magnetic shell having an infinite straight edge and extending on one side of this edge to infinity | 131 |
482. A small circuit acts at a great distance like a magnet | 131 |
483. Deduction from this of the action of a closed circuit of any form and size on any point not in the current itself | 131 |
484. Comparison between the circuit and a magnetic shell | 132 |
485. Magnetic potential of a closed circuit | 133 |
486. Conditions of continuous rotation of a magnet about a current | 133 |
487. Form of the magnetic equipotential surfaces due to a closed circuit. Fig. XVIII | 134 |
488. Mutual action between any system of magnets and a closed current | 135 |
489. Reaction on the circuit | 135 |
490. Force acting on a wire carrying a current and placed in the magnetic field | 136 |
491. Theory of electromagnetic rotations | 138 |
492. Action of one electric circuit on the whole or any portion of another | 139 |
493. Our method of investigation is that of Faraday | 140 |
494. Illustration of the method applied to parallel currents | 140 |
495. Dimensions of the unit of current | 141 |
496. The wire is urged from the side on which its magnetic action strengthens the magnetic force and towards the side on which it opposes it | 141 |
497. Action of an infinite straight current on any current in its plane | 142 |
498. Statement of the laws of electromagnetic force. Magnetic force due to a current | 142 |
499. Generality of these laws | 143 |
500. Force acting on a circuit placed in the magnetic field | 144 |
501. Electromagnetic force is a mechanical force acting on the conductor, not on the electric current itself | 144 |
Chapter II.
Mutual Action of Electric Currents.
502. Ampère's investigation of the law of force between the elements of electric currents | 146 |