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| Article | Page | |
|---|---|---|
| 788. | The specific inductive capacityNow commonly called the relative permittivity. of a dielectricAn insulating material that can be polarized by an electric field. is the square of its index of refraction | 388 |
| 789. | Comparison of these quantities in the case of paraffin | 388 |
| 790. | Theory of plane waves | 389 |
| 791. | The electric displacement and the magnetic disturbance are in the plane of the wave-front, and perpendicular to each other | 390 |
| 792. | Energy and stress during radiation | 391 |
| 793. | Pressure exerted by light | 391 |
| 794. | Equations of motion in a crystallized medium | 392 |
| 795. | Propagation of plane waves | 393 |
| 796. | Only two waves are propagated | 393 |
| 797. | The theory agrees with that of FresnelAugustin-Jean Fresnel (1788–1827), a physicist who established the wave theory of light. | 394 |
| 798. | Relation between electric conductivity and opacity | 394 |
| 799. | Comparison with facts | 395 |
| 800. | Transparent metals | 395 |
| 801. | Solution of the equations when the medium is a conductor | 395 |
| 802. | Case of an infinite medium, the initial state being given | 396 |
| 803. | Characteristics of diffusion | 397 |
| 804. | Disturbance of the electromagnetic field when a current begins to flow | 397 |
| 805. | Rapid approximation to an ultimate state | 398 |
| Article | Page | |
|---|---|---|
| 806. | Possible forms of the relation between magnetism and light | 399 |
| 807. | The rotation of the plane of polarizationThe orientation of the oscillations of light waves. by magnetic action | 400 |
| 808. | The laws of the phenomena | 400 |
| 809. | Verdet's discovery of negative rotation in ferromagneticMaterials, like iron, that exhibit strong magnetic properties. media | 400 |
| 810. | Rotation produced by quartz, turpentine, etc., independently of magnetism | 401 |
| 811. | KinematicalRelating to the motion of objects without reference to the forces causing the motion. analysis of the phenomena | 402 |
| 812. | The velocity of a circularly-polarized ray is different according to its direction of rotation | 402 |
| 813. | Right and left-handed rays | 403 |
| 814. | In media which of themselves have the rotatory property, the velocity is different for right and left-handed configurations | 403 |
| 815. | In media acted on by magnetism, the velocity is different for opposite directions of rotation | 404 |
| 816. | The luminiferousLight-bearing or light-producing. disturbance, mathematically considered, is a vector | 404 |
| 817. | Kinematic equations of circularly-polarized light | 405 |