8 STANDARD ELECTRICAL DICTIONARY.

Absolute Measurement.

Measurement based upon the centimeter, gram, and second. (See

Centimeter-Gram-Second System.)

Absolute Temperature.

Temperature reckoned from absolute zero (see "Zero, Absolute"). It is

obtained by adding for the centigrade scale 273, and for the Fahrenheit

scale 459, to the degree readings of the regular scale.

Absorption, Electric.

A property of the static charge. When a Leyden jar is being charged it

dilates a little and the capacity increases, so that it can take a

little more charge for a given potential difference existing between its

two coatings. This phenomenon occurs with other static condensers,

varying in degree with the dielectric. With shellac, paraffin, sulphur

and resin, for instance, the absorption is very slight; with

gutta-percha, stearine, and glass, the absorption is relatively great.

The term is due to Faraday. Iceland spar seems almost or quite destitute

of electric absorption.

A. C. C.

Symbol of or abbreviation for "anodic closure contraction" q. v.

Acceleration.

The rate of change of velocity. If of increase of velocity it is

positive; if of decrease, it is negative. It can only be brought about

by the exercise of force and is used as the measure of or as determining

the unit of force. It is equal to velocity (L/T) imparted, divided by

time (T); its dimensions therefore are L/(T^2). The c. g. s. unit of

acceleration is one centimeter in one second.

[Transcriber's note: The unit of acceleration is "centimeters per second

per second."]

Accumulator.

(a) A term sometimes applied to the secondary or storage battery. (See

Battery, Secondary.)

(b) See Accumulator, Electrostatic

(c) See Accumulator, Water Dropping.

(d) See Wheel, Barlow's

Accumulator, Electrostatic.

Two conducting surfaces oppositely placed, and separated by a

dielectric and arranged for the opposite charging of the two surfaces,

constitute an accumulator, sometimes termed a condenser. As this

arrangement introduces the element of a bound and of a binding charge,

the electrostatic capacity of such is greater than that of either or of

both of its component surfaces. The thinner the dielectric which

separates the conducting surfaces, and the larger the surfaces the

greater is the capacity; or the less will be the potential difference

which a given charge will establish between its two coatings. The nature

of the dielectric also determines its capacity. (See Capacity, Specific

Inductive.)

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