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| Art. | Page | |
|---|---|---|
| 503. | His method of experimenting | 146 |
| 504. | Ampère’s balance A sensitive instrument used by Ampère to measure the force between electric currents. | 147 |
| 505. | Ampère’s first experiment. Equal and opposite currents neutralize each other | 147 |
| 506. | Second experiment. A crooked conductor is equivalent to a straight one carrying the same current | 148 |
| 507. | Third experiment. The action of a closed current on a segment original: "element" of another current is perpendicular to that segment | 148 |
| 508. | Fourth experiment. Equal currents in systems that are geometrically similar produce equal forces | 149 |
| 509. | In all of these experiments the acting current is a closed circuit | 151 |
| 510. | Both circuits may, however, for mathematical purposes be conceived as consisting of elementary portions, and the action of the circuits as the total result original: "resultant" of the action of these elements | 151 |
| 511. | Necessary form of the relations between two elementary portions of lines | 151 |
| 512. | The geometrical quantities which determine their relative position | 152 |
| 513. | Form of the components of their mutual action | 153 |
| 514. | Resolution of these in three directions: parallel to the line joining them, and parallel to the elements themselves | 154 |
| 515. | General expression for the action of a finite current on the element of another | 154 |
| 516. | Condition provided by Ampère’s third case of equilibrium | 155 |
| 517. | Theory of the directrix A line used to determine the direction of force. and the determinants of electrodynamic action | 156 |
| 518. | Expression of the determinants in terms of the components of the vector-potential of the current | 157 |
| 519. | The part of the force which is indeterminate can be expressed as the space-variation of a potential | 157 |
| 520. | Complete expression for the action between two finite currents | 158 |
| 521. | Mutual potential of two closed currents | 158 |
| 522. | Appropriateness of quaternions A complex number system used in 19th-century physics to represent rotations and vectors. in this investigation | 158 |
| 523. | Determination of the form of the functions by Ampère’s fourth case of equilibrium | 159 |
| 524. | The electrodynamic and electromagnetic units of currents | 159 |
| 525. | Final expressions for electromagnetic force between two elements | 160 |
| 526. | Four different admissible forms of the theory | 160 |
| 527. | Of these, Ampère’s theory is to be preferred | 161 |