US1908572A - Disk-shaped piezo-electric oscillator - Google Patents
Disk-shaped piezo-electric oscillator Download PDFInfo
- Publication number
- US1908572A US1908572A US577029A US57702931A US1908572A US 1908572 A US1908572 A US 1908572A US 577029 A US577029 A US 577029A US 57702931 A US57702931 A US 57702931A US 1908572 A US1908572 A US 1908572A
- Authority
- US
- United States
- Prior art keywords
- disk
- oscillator
- shaped piezo
- elasticity
- electric oscillator
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 239000013078 crystal Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000002349 favourable effect Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/15—Constructional features of resonators consisting of piezoelectric or electrostrictive material
- H03H9/17—Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator
- H03H9/19—Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator consisting of quartz
Definitions
- the piezo-electric oscillators (or resonators) generally used in technics are circular or rectangular disks.
- the invention aims at providing a new means which overcomes the said irregularity.
- This new means consists in giving the oscillator a form which compensates the disparities of the modulus of elasticity existing in the different directions.
- the frequencies are direct proportional to the square roots of the moduli of elastlcity and inversely proportional to the diameter lengths and, as a consequence, the frequency can be given an ample independence of the direction by making the lengths of these diameters proportional to the square roots of the moduli of elasticity.
- the resulting form of the disk represents a centre figure, in other words a figure containing a point which bisects all straight lines passing through it and having their end points at the edge of the disk.
- the conditions of vibration of the described disk-shaped oscillator are especially favourable when the frequency of the vibrations in the diameter directions is equal to the frequency of the vibration perpendicular thereto (thickness vibration) or when one of these kinds of vibration represents a higher harmonical of the other.
- Figure 1 is a view and Figure 2 a cross section through line 22 in Figure 1.
- the oscillator is given such a form that all straight lines passing through the point A (some of which are indicated by dots) are bisected by this point A.
- the halves a a of these straight lines have such lengths that they are proportional to the square roots of the moduli of elasticity in the respective directions.
- the thickness 7 which is shown in Figure 2, has such a dimension that the ratio of the thickness h and the square root of the modulus of elasticity in the thickness direction is an even multiple of the ratio of any of the lengths a and the square root of the modulus of elasticity in the respective direction.
- the frequency of the thickness vibration is a higher harmonical of the frequency of the oscillations in the directions a.
- the oscillator shown in the drawing is a so-called Curie cut, that is to say an oscillator cut out of a crystal in such a manner that the electric axis is at right angles to the plane of the drawing in Figure l and that the optical as well as the crystallographic axis lie in this plane.
- a disk-shaped piezo-electric oscillator or resonator the plane bounding surfaces of this oscillator or resonator forming a figure in which all straight lines passing through a point in the said figure are bisected by this point, the lengths of the said straight lines from the said point to the edge of the figure being proportional to the square roots of the moduli of elasticity in the respective directions.
- the thickness having such a dimension that the ratio of the thickness and the square root of the modulus of elasticity in the thickness direction is an even multiple of the ratio of any of the said lengths and the square root of the modulus of elasticity in the respective direc tion.
Description
May 9, 1933. H STRAUBEL 1,908,572
DISK SHAPED PIEZO ELECTRIC OSCILLATOR Filed Nov. 24, 1931 f o 7 lg yilultldllmllllmlawl a;
Patented May 9, 1933 HARALD STRAUBEL, OF JENA, GERMANY,
PATENT OFFIE ASSIGNOR TO THE FIRM CARL ZEISS, OF
JENA, GERMANY DISK-SHAPED PIEZO-ELECTRIG OSCILLATOR Application filed November 24, 1931, Serial No. 577,029, and in Germany December 2, 1930.
The piezo-electric oscillators (or resonators) generally used in technics are circular or rectangular disks.
As the modulus of elasticity is governed by the direction, the frequencies of oscillators of this kind are not uniform in the plane of the disk, which is proved for instance by the irregularity in the vibration of the surfaces of such disks.
Uniform frequencies being of advantage in some kinds of application of such oscillators, the invention aims at providing a new means which overcomes the said irregularity.
This new means consists in giving the oscillator a form which compensates the disparities of the modulus of elasticity existing in the different directions.
In the diflerent directions of diameter, the frequencies are direct proportional to the square roots of the moduli of elastlcity and inversely proportional to the diameter lengths and, as a consequence, the frequency can be given an ample independence of the direction by making the lengths of these diameters proportional to the square roots of the moduli of elasticity.
The resulting form of the disk represents a centre figure, in other words a figure containing a point which bisects all straight lines passing through it and having their end points at the edge of the disk.
It can be proved by way of experiment that the desired effect is obtained to a great extent.
The conditions of vibration of the described disk-shaped oscillator are especially favourable when the frequency of the vibrations in the diameter directions is equal to the frequency of the vibration perpendicular thereto (thickness vibration) or when one of these kinds of vibration represents a higher harmonical of the other.
The accompanying drawing, which illustrates an example of the invention, shows an oscillator of quartz. Figure 1 is a view and Figure 2 a cross section through line 22 in Figure 1.
As shown in- Figure 1, the oscillator is given such a form that all straight lines passing through the point A (some of which are indicated by dots) are bisected by this point A. The halves a a of these straight lines have such lengths that they are proportional to the square roots of the moduli of elasticity in the respective directions. The thickness 7), which is shown in Figure 2, has such a dimension that the ratio of the thickness h and the square root of the modulus of elasticity in the thickness direction is an even multiple of the ratio of any of the lengths a and the square root of the modulus of elasticity in the respective direction. Hence the frequency of the thickness vibration is a higher harmonical of the frequency of the oscillations in the directions a.
The oscillator shown in the drawing is a so-called Curie cut, that is to say an oscillator cut out of a crystal in such a manner that the electric axis is at right angles to the plane of the drawing in Figure l and that the optical as well as the crystallographic axis lie in this plane.
I claim:
1. A disk-shaped piezo-electric oscillator or resonator, the plane bounding surfaces of this oscillator or resonator forming a figure in which all straight lines passing through a point in the said figure are bisected by this point, the lengths of the said straight lines from the said point to the edge of the figure being proportional to the square roots of the moduli of elasticity in the respective directions.
2. In a disk-shaped piezo-electric oscillator or resonator according to claim 1, the thickness having such a dimension that the ratio of the thickness and the square root of the modulus of elasticity in the thickness direction is an even multiple of the ratio of any of the said lengths and the square root of the modulus of elasticity in the respective direc tion.
HARALD STRAUBEL.
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| DE530582T | 1930-12-03 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| US1908572A true US1908572A (en) | 1933-05-09 |
Family
ID=34109828
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US577029A Expired - Lifetime US1908572A (en) | 1930-12-03 | 1931-11-24 | Disk-shaped piezo-electric oscillator |
Country Status (2)
| Country | Link |
|---|---|
| US (1) | US1908572A (en) |
| DE (1) | DE530582C (en) |
-
1930
- 1930-12-03 DE DE1930530582D patent/DE530582C/en not_active Expired
-
1931
- 1931-11-24 US US577029A patent/US1908572A/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| DE530582C (en) | 1931-07-30 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US2870521A (en) | Method of adjusting the resonant frequency of a vibrating system | |
| GB1121098A (en) | A vibrating string for measurement purposes | |
| JPS6275605A (en) | Differential absorptionn polarizer, method and apparatus formanufacturing same polarizer | |
| US10254481B2 (en) | Integrated waveguide with reduced brillouin gain and a corresponding reduction in the magnitude of an induced stokes wave | |
| US2261791A (en) | Piezoelectric thickness-mode quartz crystal | |
| US1908572A (en) | Disk-shaped piezo-electric oscillator | |
| JP3096472B2 (en) | SC-cut crystal unit | |
| FR1341963A (en) | Electromechanical crystal filter, vibration shear in thickness | |
| US2111384A (en) | Piezoelectric quartz element | |
| US3375379A (en) | Rotated y-cut rectangular piezoelectric quartz crystal plates | |
| US2159796A (en) | Quartz piezoelectric element | |
| US2111383A (en) | Piezoelectric quartz element | |
| US2261792A (en) | Quartz piezoelectric element | |
| US2119848A (en) | Quartz piezoelectric element | |
| US1724232A (en) | Piezo electric crystal | |
| DE2703335C2 (en) | ||
| US1913201A (en) | Instrument pointer | |
| US2176653A (en) | Two-frequency piezoelectric element | |
| US1822928A (en) | Piezo electric plate | |
| JP2017158146A (en) | Quartz oscillator | |
| US1696627A (en) | Piezo-electric crystal | |
| GB383075A (en) | Improvements in disc-shaped piezo-electric oscillators (or resonators) | |
| KR102029492B1 (en) | Crystal oscillator and manufacturing method thereof | |
| DE866806C (en) | Disc-shaped piezoelectric quartz oscillator | |
| US2029729A (en) | Piezoelectric quartz crystal |