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Electricity
: class of physical phenomena resulting from the existence of charge and
from the interaction of charges. When a charge is stationary or static, it
produces forces on objects in regions where it is present, and when it is
in motion, it produces magnetic effects. Electric and magnetic effects are
caused by the relative position and movement of positively and negatively
charged particles of matter. So far as electrical effects are concerned,
these particles are either neutral, positive, or negative.
Electricity is concerned with the positively charged particles, such as
protons, that repel one another and the negatively charged particles, such
as electrons, that also repel one another .
Negative and positive particles, however, attract each other. This
behavior may be summarized as follows: Like charges repel, and unlike
charges attract.

II.
Electrostatics

A
common manifestation of electricity is the repulsive or attractive force
between two stationary bodies. Electrically, they exert an equal force on
one another. The electric charge on each body may be measured in
statcoulombs or the electrostatic unit of charge, abbreviated to esu
.
The force between particles bearing charges q1
and q2 can be calculated by Coulomb's law— —that
is, the force is proportional to the product of charges, divided by the
square of the distance that separates them. The constant of
proportionality k is called the dielectric constant and it is equal
to . The constant
is called the permittivity, and its value depends on the medium
surrounding the charges. This law is named after the French physicist
Charles Augustin de Coulomb, who developed the equation.
Every
electrically charged particle is surrounded by a field of force. This field
may be represented by lines of force showing the direction of electrical
stresses within the field. To move a charged particle from one point in
the field to another requires work. The amount of energy needed to perform
such work on a particle bearing a unit charge is known as the potential
difference between these two points. The difference is usually measured in
volts. The earth, a large conductor, which may be assumed to be
substantially uniform electrically, is commonly used as the zero reference
level for potential
energy. Thus the potential of a positively charged body is said to be
a certain number of volts above the potential of the earth, and the
potential of a negatively charged body is said to be a certain number of
volts below the potential of the earth.
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