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| 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 |