Hawkins Electrical Guide v. 01 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applicationsHawkins, N. (Nehemiah)
Science
Hawkins Electrical Guide v. 01 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applications
Hawkins, N. (Nehemiah)
Electrical engineering -- Handbooks, manuals, etc.
As soon as the loop rotates out of the vertical plane, the
electromotive force rises and the current begins to flow in the
direction indicated by the arrows, going out to the external
circuit through brush M, and returning through brush S.
Continuing the rotation, the electromotive force increases in
proportion to the sine of the angle made by the plane of the
loop with the horizontal, until the loop comes into the
horizontal position illustrated in fig. 170. This increase is
indicated by the gradual rise of the sine curve from E to F. The
loop has now made one quarter of a revolution and the
electromotive force reached its maximum value.
As the loop rotates past the horizontal position of fig. 170,
the electromotive force gradually decreases in intensity,
reaching the zero point at the end of the second quarter--that
is, when the loop has turned one half revolution. This is
indicated by the gradual fall of the curve from F to G.
When the loop turns out of the vertical position shown in fig.
171 the current reverses, because the movement of A B and C D is
reversed; at this instant the brush M becomes negative, and S
positive. This reversal of current is indicated by the curve
falling _below_ the axis from G to I.
During the second half of the revolution, figs. 171 to 173, the
changes that occur are the same as in the first half, with the
exception that the current is in the reverse direction; these
changes are as shown by the curve from G to I.
CHAPTER XIV
THE DYNAMO: CURRENT COMMUTATION
=How the Dynamo Produces Direct Current: The Commutator.=--The essential
difference between an alternator and a dynamo is that the alternator
delivers alternating current to the external circuit while the dynamo
delivers direct current. In both machines, as before stated, alternating
currents are induced in the armature, but the kind of current delivered to
the external circuit depends on the manner in which the armature currents
are collected.
In the case of an alternator, the method is quite simple. As
previously explained, each end of the loop is connected with an
insulated collector ring carried by the shaft, the current being
collected by means of brushes which bear against the rings. This
principle, rather than the actual construction, is shown in the
preceding illustrations. Its important point, as distinguished
from other methods of collecting the current, is that _each end
of the loop is always in connection with the same brush_.
=Ques. How is direct current obtained in a dynamo?=
Ans. A form of switch called the _commutator_ is placed between the
armature and the external circuit and so arranged that it will reverse the
connections with the external circuit at the instant of each reversal of
current in the armature.
=Ques. How is a commutator constructed?=
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