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www.americanradiohistory.com<br />

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.

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