.The arrangement shown in FIG. 18 implements the principle used in the first
practical electric motor and generator. At first inspection, the terms homopolar
or unipolar appear to be misnomers. Two magnetic poles are, indeed, present,
and any allusion to the elusive magnetic monopole was surely not intended by
the originators of these names. (The machines are also referred to as acyclic
types.) The basic operational difference from conventional motors and generators
is that the active conductor interacts with the magnetic field only once per
revolution. Note that whichever segment of the disk happens to be within the
field is inherently the active conductor. In conventional machines of even
the simplest type, a given armature conductor interacts with the field twice
per revolution, and in so doing, it either generates or requires an alternating
current. In contrast, the homopolar is a true dc ma chine. It needs no commutator
to convert dc to ac, or vice versa.

FIG. 18 The homopolar machine devised by Michael Faraday.
This method of developing motor and generator action is often thought
of as a primitive stepping stone to techniques representing greater technical
sophistication. However, the homopolar machine represents a very practical
approach for certain applications, and has been built in sizes ranging
up to several thousand kilowatts. It is basically a high-current low-voltage
machine, but higher voltages have been handled by extending the construction
to accommodate multiple disks. This machine is destined to enjoy revived
consideration because modern material technology, de vices, and techniques
make it again amenable to a hope that has never died—the elimination
of the commutator. Current is conducted to and from the disk by slip-ring
techniques. This has proved an obstacle in high-current applications;
however, many designers would rather contend with this problem than that
of clean and reliable commutation.
To illustrate what is implied by “modem methods,” consider the following:
homopolar motors and generators have been made in the several-hundred
to several thousand horsepower range and make use of superconducting
field windings. Such field excitation involves fluxes of 60,000 gauss,
and even stronger fields will be feasible. A shipboard propulsion motor
of this type tends to be about one half the physical size of ordinary
motors, In one design, contact to the disk is made by means of a liquid
metallic alloy that has more than twenty-five times the current-carrying
capacity of brushes. The success thus far indicated suggests the increase
of capacity to the 30,000- horsepower level. When combined with solid-state
control techniques, these grown-up Faraday disks can be expected to become
competitive, rather than archaic.
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