the capacity of the electrometer system is 50 electrostatic units. This current is equal to 2·8 × 10^{-13} amperes. If a steady deflection of 10 divisions is required, which corresponds to a rise of potential of the system of 1/100 of a volt, the resistance should be 36,000 megohms. For a deflection of 100 divisions, the resistance should be 10 times as large. Dr Bronson[1], working in the laboratory of the writer, has recently made some experiments in order to devise a practical method for measurements of this character. It is difficult to obtain sufficiently high and constant resistances to answer the purpose. Tubes of xylol had too great a resistance, while special carbon resistances were not sufficiently constant. The difficulty was finally got over by the use of what may be called an "air resistance." The arrangement of the experiment is shown in Fig. 20.
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Fig. 20.
The electrometer system was connected with the upper of two insulated parallel plates AB, on the lower of which was spread a layer of a very active substance. An active bismuth plate, coated with radio-tellurium, which had been obtained from Sthamer of Hamburg, proved very convenient for this purpose.
The lower plate B was connected to earth. The charge communicated to the upper plate of the testing vessel CD and the electrometer system leaked away in consequence of the strong
- ↑ Bronson, Amer. Journ. Science, Feb. 1905.
