Pumps and Hydraulics, Part 1 (of 2)Hawkins, N. (Nehemiah)
Science
Pumps and Hydraulics, Part 1 (of 2)
Hawkins, N. (Nehemiah)
Hydraulic machinery; Pumping machinery
It is natural that a machine which gives out electric energy when
driven by an external power, should, when electric energy is delivered
to it, reverse its action and give out mechanical power and do work.
Perhaps the simplest way to explain the cause of the movement of
an electric motor, when supplied with a current, is to compare its
action to the well-known attraction of unlike poles or magnets and
the repulsion of like poles. Unlike poles are North and South; like
poles are two North or two South. In all motors a current through the
field causes a North or South pole to be maintained, and a current
through the armature and brushes causes an opposite polarity. These
constantly-maintained unlike poles attract each other and pull the
armature around on its axis.
It has been explained that if a motor be driven by a belt an
electro-motive force is produced and the machine acts as a dynamo.
It is also a fact that an electro-motive force is produced whether
the power for driving the machine is received from a belt or from
the electric current,—that is, whether the machine be driven as a
dynamo or as a motor. In a dynamo, however, the current follows the
direction in which the electro-motive force is acting. In a motor, the
electro-motive force produced has a direction opposed to that of the
flow of current. This may be illustrated by the following experiment.
Two similar machines are driven independently at 600 revolutions and
give an electro-motive force of 100 volts. Similar terminals of the two
machines are connected together; no current flows between the machines,
because the two pressures are the same and are in opposite directions.
If now the belt be thrown off from one machine, its speed will begin to
fall; this will lower its electro-motive force below that of the other
machine or dynamo, but will not change the direction of the force.
There will now be a difference of pressure in favor of the machine
which is driven, and it will deliver a current through the other
machine and run it as a motor. The speed of the motor will continue to
fall until the difference in pressure or electro-motive force between
the two machines is only sufficient to cause the flow of enough current
to keep the motor running against whatever frictional resistance, and
other resistance there may be. The electro-motive force generated in
the motor, which is against, or counter to that of the current in the
circuit, is called the “counter electro-motive force.”
In order to determine how fast a motor will run without doing work
under any given pressure, it is not necessary to know anything
about the dynamo that furnishes the pressure. The pressure alone
is sufficient to determine the speed of the motor. For instance, if
a motor will give a pressure of 500 volts when running free at 100
revolutions, it will always run at about 100 revolutions when not doing
work on an electric circuit where the pressure is 500 volts.
MAGNETIC NEEDLE.
Public-domain text, read in full here on John Shaqi.
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