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450 Radio News for November, 1928<br />
Magneto - Striction<br />
An Interesting Field for the Radio Experimenter;<br />
to Build a Magneto -Striction Oscillator<br />
By M. J. Cztttler<br />
RADIO NEWS LaGoratories<br />
ccERROMAGNETIC" substances<br />
(such as iron, cobalt, nickel and alloys<br />
into which those metals enter in<br />
considerable proportion) possess<br />
"magneto- strictioe" properties; which means<br />
that they undergo slight mechanical alterations<br />
of shape, and some of their physical<br />
properties change when they are subjected<br />
to the influence of a magnetic field. This<br />
action of the magnetic field on such sub<br />
stances is manifested in a series of effects<br />
discovered at different epochs and known<br />
under various names.<br />
The oldest among these is the "Joule effect,"<br />
discovered by Joule about 1847; this<br />
is the variation of the length of a ferromagnetic<br />
rod exposed to a magnetic field.<br />
Let us consider an iron rod freely suspended<br />
inside of a long solenoid; an electric current<br />
of constant intensity flowing through a<br />
solenoid creates a magnetic field which is<br />
practically uniform within the solenoid over<br />
n great part of its length; provided that the<br />
ratio between the length and diameter is<br />
sufficiently high. This is illustrated in Fig.<br />
1. The field strength within the coil is proportional<br />
to the intensity of the current, and<br />
the variation of the field may be governed<br />
through the regulation of the magnetizing<br />
current.<br />
AN ALTERNATING ACTION<br />
Let us now examine what happens to the<br />
iron rod if the field inside the solenoid is<br />
varied from zero upwards. First, an elongation<br />
will take place. This will continue<br />
until the field's strength reaches a certain<br />
value, after which any further increase of<br />
the field will cause a contraction; the rod<br />
then becomes shorter, will again reach its<br />
FIG.1<br />
The magnetic field within a solenoid is prac,<br />
Orally uniform in distribution, as illustrated<br />
herewith.<br />
11r. Outlier is shown here testing the magneto- striction oscillator described<br />
in the accompany article.<br />
original value, and will then continue to contract<br />
until a saturation point is reached.<br />
Any further increase of the field strength<br />
will have no more effect on the length of<br />
the rod.<br />
The behavior of other ferromagnetic substances<br />
under the same conditions will .be<br />
different. Nickel, for instance, continuously<br />
decreases in its length; while cast cobalt, in<br />
contrast to iron, first contracts and then expands,<br />
reaches its original length and continues<br />
to elongate until saturation occurs.<br />
The relation between the strength of the<br />
magnetic field and the variation of the<br />
length is shown clearly in Fig. 2. (Both<br />
figures are taken from an article on magneto<br />
-striction by S. R. Williams, published<br />
in the Bulletin of the National Research<br />
Council, August, 1922.<br />
Other ferromagnetic substances may respond<br />
differently, but one thing is common<br />
to them all; they vary in length (whether<br />
positively or negatively) with a rising field<br />
strength, and reach a point where saturation<br />
occurs, after which a further increase<br />
of the field has practically no effect on their<br />
length.<br />
An important remark is to be made here;<br />
the Joule effect is dependent on the direction<br />
of the field. As the extent of the variations<br />
in the length of such rods is extremely<br />
minute, their measurement is a matter of<br />
great difficulty; the utmost care must be<br />
taken to avoid temperature variations and<br />
changes in other physical conditions, which<br />
may conceal the real values.<br />
Various ingenious arrangements have been<br />
used for such measurements; Fig. 3 gives a<br />
schematic layout of the method used by<br />
Professor Williams. The method of operation<br />
is self -explanatory; the expansion or<br />
contraction of the rod under test is converted<br />
into angular rotation of the mirror<br />
by means of the lever.<br />
CORRESPONDING PHENOMENA<br />
To the Joule effect corresponds another<br />
phenomenon which is its opposite; the "Villari<br />
effect." The forcible lengthening of a<br />
ferromagnetic rod located in a magnetic<br />
field is accompanied by a variation in its<br />
magnetization or its permeability. As we<br />
have seen in the Joule effect, various substances<br />
behave differently under the same<br />
conditions; but there is a relation, for each<br />
metal, between its Villari effect and its<br />
Joule effect. An investigator (Nagaoka)<br />
who followed Joule, has confirmed his supposition<br />
that a magnetic field has an influence<br />
on the volume of a ferromagnetic<br />
substance.<br />
Another very interesting phenomenon<br />
which belongs to the same group is the<br />
"Wiedemann effect" and its two inverse effects.<br />
The Wiedemann effect is the twisting<br />
of a rod under the influence of a combination<br />
of two fields, one longitudinal and<br />
one circular. Suppose a magnetic rod is<br />
clamped at one end inside of a long solenoid;<br />
then a current passing through the<br />
solenoid produces a uniform longitudinal<br />
field inside of it. If, at the same time,<br />
another current flows through the rod, a<br />
circular field will be created around it. If<br />
one of these currents is kept constant while<br />
the other is varied, or if both currents are<br />
varied, a rotation of the further end will be<br />
observed.<br />
The two corresponding inverse effects are:<br />
first, a circular field is created when a rod<br />
which is located in a magnetic field is sud-<br />
These curves show how various metals change<br />
in length under the influence of a magnetic<br />
field.