dotted line shows the variation of potential at any point between the plates when no ionization is produced between the plates; curve A for weak ionization, such as is produced by uranium, curve B for the intense ionization produced by a very active substance. In both cases the potential gradient is least near the active plate, and greatest near the opposite plate. For very intense ionization it is very small near the active surface. The potential gradient varies slightly according as the active plate is charged positively or negatively.
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Fig. 9.
47. Variation of current with voltage for surface ionization.
Some very interesting results, giving the variation of the
current with voltage, are observed when the ionization is intense,
and confined to the space near the surface of one of two parallel
plates between which the current is measured.
The theory of this subject has been worked out independently by Child[1] and Rutherford[2]. Let V be the potential difference
