siderable quantity of electricity, and this passage requires a considerable time. When the polarized state has been set up, there is an internal electromotive force acting in the substance in the reverse direction, which will continue till it has either produced a reversed current equal in total quantity to the first, or till the state of polarization has quietly subsided by means of true conduction through the substance.
The whole theory of what has been called residual discharge, absorption of electricity, electrification, or polarization, deserves a careful investigation, and will probably lead to important discoveries relating to the internal structure of bodies.
367.] The resistance of the greater number of dielectrics diminishes as the temperature rises.
Thus the resistance of gutta-percha is about twenty times as great at 0°C as at 24°C. Messrs. Bright and Clark have found that the following formula gives results agreeing with their experiments. If is the resistance of gutta-percha at temperature centigrade, then the resistance at temperature will be
| , |
the number varies between 0.8878 and 0.9.
Mr. Hockin has verified the curious fact that it is not until some hours after the gutta-percha has taken its temperature that the resistance reaches its corresponding value.
The effect of temperature on the resistance of india-rubber is not so great as on that of gutta-percha.
The resistance of gutta-percha increases considerably on the application of pressure.
The resistance, in Ohms, of a cubic metre of various specimens of gutta-percha used in different cables is as follows[1].
| Name of Cable. | |||
| Red Sea | .267 × 10¹² | to .362 × 10¹² | |
| Malta-Alexandria | 1 | .23 × 10¹² | |
| Persian Gulf | 1 | .80 × 10¹² | |
| Second Atlantic | 3 | .42 × 10¹² | |
| Hooper's Persian Gulf Core | 74 | .7 × 10¹² | |
| Gutta-percha at 24°C | 3 | .53 × 10¹² |
368.] The following table, calculated from the experiments of
- ↑ Jenkin's Cantor Lectures.
