XIII 225 EXPERIMENTS ON THE CATHODE DISCHARGE DESCRIPTION of the BATTERY The battery was based on the principle employed by Poggendorff in his polarisation battery, and applied by Planté to the cells which bear his name. The cells are arranged in parallel, charged by a battery of comparatively small electro- motive force, and then arranged in series. In this way very high electromotive forces may be attained. It is not necessary to deal singly with each cell thus: groups of five or ten or more cells can be set up permanently in series; and during the charging only these groups need be placed in parallel. The larger the number of cells in each group, the simpler does the commutating mechanism become; of course the electromotive force required for charging increases at the same time. I arranged my cells in groups of five in series. The cells were made of test-tubes, 125 mm. high, 14-15 mm. in diameter, and were filled two-thirds deep with sulphuric acid diluted with nine times its volume of water. The electrodes were strips of lead of suitable length, 10 mm. broad and 1 mm. thick, varnished at the top with asphalt varnish. The neighbouring pairs of electrodes within each group of five cells were formed by bending a single strip of lead (so that no connecting wire was necessary); copper wires soldered to the outer electrodes led to two glass mercury cups which formed the poles of the group. The cells were cemented in fifties on boards, of which five (or 250 cells) went in a box 84 cm. long, 12 cm. wide, and 17 cm. high. The 100 glass cups forming the corresponding poles lay in a row on the front side of the box. The commutation was effected by two interchangeable commutators, of which one was used in charging and the other in discharging. These were made of bent wires attached to a strip of wood; the construction was simple and does not require special explanation. So long as the battery remained in good condition, it worked as follows. Ten Bunsen or Grove cells were required to charge it. When these had been in action for an hour the battery was charged sufficiently for a day's work. The difference of potential between its poles was about equal to that of 1800 Daniell cells. Its internal resistance, as M. P. Q