After referring to difficulties encountered when using standard conductivity cells, a brief reference is made to that part of the author's previous work on the measurement of electrolytic resistance which is essential to the present paper. Two new radio-frequency current arrangements for titration are described in both of which a length of Pyrex glass tube fitted with external electrodes displaces the usual type of conductivity cell. The attendant difficulties of the latter are thus avoided.
The solution under analysis is drawn into the Pyrex tube where its resistance is measured (a) by its effect upon the Q of the oscillator, and (b) by its resistance to radio-frequency currents which are rectified and then measured by a zero-shunted microammeter.
A syringe is employed to draw the solution into the Pyrex tube. The use of a variable coupling condenser is suggested when making microammeter settings before titrating.