US2485722A

US2485722A - Crystal

Info

Publication number: US2485722A
Application number: US575387A
Authority: US
Inventors: Wesley S Erwin
Original assignee: Motors Liquidation Co
Current assignee: Motors Liquidation Co
Priority date: 1945-01-31
Filing date: 1945-01-31
Publication date: 1949-10-25
Anticipated expiration: 1966-10-25

Description

W. S. ERWIN Oct. 25, 1949.

CRYSTAL Filed Jan. 31, 1945 Zmventor wagzzum Patented Oct. 25, 1949 CRYSTAL Wesley S. Erwin, Detroit, Mich., assignor to General Motors (io lmrfltion, Detroit, Mich, a corporation of Delaware Application January 31, 1945, Serial No. 575,387

This invention relates to vibration producing or oscillating means and more specifically to that branch of the art known as piezo-electric crystals. One of the main uses for crystals is, of course, to control electronic oscillators in which the crystal is vibrated at its natural or resonant frequency and thus provides a very stable oscillator frequency controller. However, there are uses for crystals in which the same are not vibrated at a resonant frequency but at frequencies oil resonance and used to impart such mechanical vibration to other structures. As an example of this latter use there may be mentioned that set forth in Patent Number 2,431,233 entitled "Supersonic measuring means" issued November 18, 1947, in the name of Wesley S. Erwin assigned to a common assignee.

In that instance a crystal is vibrated or set into motion by an oscillator which may be tuned over a predetermined frequency range, thus vibrating the crystal mechanically at a number of different frequencies. The crystal is mounted in contact with a part or portion to which it is desired to impart this vibration and for certain purposes as set forth does drive the mechanical load in order to determine certain physical or structural characteristics of the same. In this case it is desired to work not at natural resonance but of! crystal resonance and to depend entirely upon the mechanical drive from the crystal to the work or load and therefore, spurious vibrations of the crystal which may be caused by harmonics or modes within the crystal itself prevent the acquiring of accurate results. Since a mechanical part such as a crystal having regular configuration may be easily itself set into harmonic or spurious vibration, it is desired to so design the same that such a tendency is suppressed or attenuated.

It is therefore an object of my invention to provide a vibrating body having substantially no resonance frequency.

It is a further object of my invention to provide a piezo-electric crystal of such configuration that the same has substantially no resonant frequency vibrations.

It is a still further object of my invention toprovide a piezo-electric crystal in which the exterior dimensions are not uniform in order that nodes of vibration may not be set up by the application of predetermined frequencies thereto.

With these and other objects in view which will become apparent as the specification proceeds, my invention will be best understood by reference to the following specification and claims and the 3 Claims. (01. 171-327) illustrations in the accompanying drawings, in which:

Figure 1 is a perspective view showing a usual regular crystal.

Figure 2 is a perspective view of the same crystal with some possible vibration modes indicated.

Figures 3, 4, 5, 6, '7 and 8 are perspective views showing different modified forms for so designing and constructing the crystal as to suppress the formation of undesirable modes which might be set up by frequencies of driving oscillation.

Referring now more specifically to the drawings, Figure 1 is a perspective view of a normal crystal 2 having uniform th ckness along its X axis and uniform widths along its Y and Z axes. This is representative of crystals which are commercially available on the market and when used to impart vibrations to mechanical pieces at off resonant points frequently have set up therein spurious vibrations known as width or thickness modes which impress false indications on indicating means and thus prevent the obtaining of accurate measurements. Such modes as for example the lst and 5th may be set up along lines 4 or 6 as indicated in Figure 2 when certain frequencies of vibration are applied either electrically or mechanically to the crystal.

In order to suppress the formation of such modes, one method would be to break up the continuity by distorting the normal uniform shape of the crystal. In Figure 3 the crystal 2' is tapered so that elements along the Y axis have different lengths, the end 8 toward the right is shorter than the back edge III. This, of course, makes the two opposite sides I! and H nonparallel and thus breaks up the formation of modes along the Y axis. Another mode is suppressed as shown in Figure 4. In this case the X axis thickness is tapered for instance in the Z direction therefore making the forward face It of the crystal 2 narrower than the rear face It. This suppresses the formation of the thickness modes.

In Figure 5 the crystal 2 has its X axis thickness tapered in the Y direction causing the front edge 20 to be much narrower than the rear edge 22. In Figure 6 there is shown a compound taper in which one corner of the crystal is thinner than in Figure 3 orin which the X axis thickness is progressive from the origin in both to the Y and Z directions. In this case the comer 24 of the crystal 2 is the thinnest of the four. Figure 7 also discloses a compound taper in that it is tapered to the right in thickness and also in width. It might be stated that when both dimensions of the Y axis and the x axis are tapered simultaneously one eliminates both width and thickness modes. Thus, in crystal 2 the edge 26 is both shorter and thinner than the rear edge 28. The same result may also be obtained with a curved crystal as shown in Figure 8 in crystal 2 by tapering both the width and thickness of the crystal from right to left.

It will thus be evident that by manufacturing or producing crystals in the manner shown in Figures 3-8 that the uniformity of crystal dimensions are so varied as to break up the formation of either width or thickness modes and thus permit the usage of such a crystal between a source of electrical oscillations and means to which it is desired to impart mechanical vibrations or vice versa without the formation of spurious vibrations introducing erroneous readings into the indicating or measuring means.

I claim:

1. A piezo-electric crystal to impart mechanical vibration to a load said crystal being constructed with tapering width and thicknes dimensions to suppress the formation of width and thickness modes to produce a substantially nonresonant transducer.

2. A piezo-electric crystal to impart mechanical vibration to a load, said crystal having one face shaped to conform to the surface of a part to be vibrated and constructed with tapering dimensions in two major axes directions to suppress the formation of modes in the respective dimensions tapered to produce a substantially non-resonant transducer.

3. An X-cut piezo-electric crystal which is tapered in the Y axis dimension to substantially eliminate Y axis resonant modes of vibration.

WESLEY S. ERWIN.

REFERENCES CITED The following references are of record in the file of this patent:

UNITED STATES PATENTB Number Name Date 2,159,891 Guerbilsky May 23, 1939 2,240,449 Wolfskill Apr. 29, 1941 2,261,792 Bokovoy Nov. 4, 1941 2,431,233 Erwin Nov. 18, 1947