If V = 0 this reduces to

F = ( V^2 * S ) / ( 8 * PI * d^2 ) (2)

or

V = d * SquareRoot( (8 * PI * F ) / S ) (3)

As F is expressed as a weight, and S and a as measures of area and

length, this gives a means of directly obtaining potential values in

absolute measure. (See Idiostatic Method--Heterostatic Method.)

Synonyms--Attracted Disc Electrometer--Weight Electrometer.

Fig. 152. SECTION OF BASE OF PORTABLE ELECTROMETER.

In some forms the movable disc is above the other, and supported at the

end of a balance beam. In others a spring support, arranged so as to

enable the attraction to be determined in weight units, is adopted. The

cuts, Figs. 152 and 154, show one of the latter type, the portable

electrometer. The disc portion is contained within a cylindrical vessel.

Fig. 153. DIAGRAM ILLUSTRATING THEORY OF ABSOLUTE ELECTROMETER.

Referring to Fig. 152 g is the stationary disc, charged through the

wire connection r; f is the movable disc, carried by a balance beam

poised at i on a horizontal and transverse stretched platinum wire,

acting as a torsional spring. The position of the end k of the balance

beam shows when the disc f is in the plane of the guard ring h h. The

end k is forked horizontally and a horizontal sighting wire or hair is

fastened across the opening of the fork. When the hair is midway between

two dots on a vertical scale the lever is in the sighted position, as it

is called, and the disc is in the plane of the guard ring.

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