The atom and the Bohr theory of its structure : $b an elementary presentation — John Shaqi
The atom and the Bohr theory of its structure : $b an elementary presentationHolst, Helge
Science
The atom and the Bohr theory of its structure : $b an elementary presentation
Holst, Helge
Atomic theory
That the positive and negative states of electricity could not be
taken as “symmetric” seemed, however, to follow from the so-called
discharge phenomena, in which electricity, with the emission of light,
streams out into the air from strongly charged (positive or negative)
bodies, or passes through the air between positive and negative bodies
in sparks, electric arcs or in some other way. In a discharge in air
between a metal point and a metal plate, for instance, a bush-shaped
glow is seen to extend from the point when the charge there is
positive, while only a little star appears when the charge is negative.
Naturally, we cannot discuss here the many electric phenomena and laws,
and must be satisfied with a brief description of those which are of
importance in the atomic theory.
In this latter category belongs _Coulomb’s Law_, formulated about
1785. According to this law, the repulsions or attractions between
two electrically charged bodies are directly as the product of the
charges and inversely as the square of the distance between them (as in
the case of the gravitational attraction between two neutral bodies,
according to Newton’s Law). The unit in measuring electric charges can
be taken as that amount which will repel an equal amount of electricity
of the same kind at unit distance with unit force. If we use the
scientific or “absolute” system, in which the unit of length is one
centimetre, that of time one second and that of mass one gram, then
the unit of force is _one dyne_, which is a little greater than
the earth’s attraction on a milligram weight. Let us suppose that two
small bodies with equal charges of positive (or negative) electricity
are at a distance of one centimetre from each other. If they repel each
other with a charge of one dyne, then the amount of electricity with
which each is charged is called the _absolute electrostatic unit of
electricity_. If one body has a charge three times as great and
the other has a charge four times as great, the repulsion is 3 × 4 =
12 times greater. If the distance between the bodies is increased from
one to five, the repulsion is twenty-five times as small, since 5² =
25. If the charge of one body is substituted by a negative one of same
magnitude the repulsion becomes an attraction of the same magnitude.
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