US1908320A - Piezo-electric crystal holder - Google Patents
Piezo-electric crystal holder Download PDFInfo
- Publication number
- US1908320A US1908320A US412687A US41268729A US1908320A US 1908320 A US1908320 A US 1908320A US 412687 A US412687 A US 412687A US 41268729 A US41268729 A US 41268729A US 1908320 A US1908320 A US 1908320A
- Authority
- US
- United States
- Prior art keywords
- piezo
- crystal
- holder
- crystal holder
- electric crystal
- 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 title description 23
- 125000006850 spacer group Chemical group 0.000 description 21
- 239000000463 material Substances 0.000 description 5
- 239000002305 electric material Substances 0.000 description 3
- 239000010453 quartz Substances 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 229910001374 Invar Inorganic materials 0.000 description 1
- 229910000792 Monel Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000005755 formation reaction Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000000034 method Methods 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 elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/05—Holders or supports
- H03H9/09—Elastic or damping supports
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H3/00—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators
- H03H3/007—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks
- H03H3/02—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks for the manufacture of piezoelectric or electrostrictive resonators or networks
- H03H3/04—Apparatus or processes specially adapted for the manufacture of impedance networks, resonating circuits, resonators for the manufacture of electromechanical resonators or networks for the manufacture of piezoelectric or electrostrictive resonators or networks for obtaining desired frequency or temperature coefficient
Definitions
- PIEZO ELECTRIC CRYSTAL HOLDER Filed Dec. 9, 1929 INVENTOR J.W. CONKUN ATTOR N EY Patented May 9, 1933 UNITED STATES PATENT OFFICE JAMES W. CONKLIN, OF ROCKY POINT, NEW YORK, ASSIGNOR TO RADIO CORPORATION OF AMERICA, A CORPORATION OF DELAWARE PIEZO-ELEOTRIC CRYSTAL HOLDER Application filed December 9, 1929.
- This invention relates to the pieZo-electric art and deals more specifically with a piezoelectric crystal holder or housing.
- piezo-electric crystal holders or housings constructed in accordance with present day practice, it has been found that varlations in the ambient temperature of the housing, as well as variations in the temperature of the housing itself, and also of the crystal, cause corresponding variations in the width of the air gap between the crystal and plates or electrodes. It has been found in practice that this variation in the width of the air gap introduces serious errors in the operation of the crystal as a frequency standard or frequency control means.
- a further object of this invention is to provide a crystal holder in which the spacing of the electrodes is varied in a predetermined manner with changes in temperature.
- Fig. l is a sectional view of a device embodying the present invention.
- Fig. 2 is a plan view of the device shown in Fig. 1. 65
- the holder or housing 10 is seen to comprise a lower plate 11 and an upper plate 12; both plates being of any suitable metal, preferably Monel metal.
- thequartz spacer 13 which may be either an annular ring enclosing the crystal 14; or alternatively, separate spacer sections may be employed at suitable locations, whereby properly to separate and hold the plates 11 and 12 with respect to each other.
- the primary quartz spacer is of the same material and thickness as the crystal itself and preferably consists of pieces or corners of the particular crystal in use, which pieces or corners have been cut off after the grinding process of the crystal oscillator is completed.
- the screw members 15 pass through the upper electrode 12 and are fixed in the plate 11 in screw-threaded engagement therewith at 16.
- the plate 12 is provided With holes 12a through which the screw 15 passes.
- the secondary spacers may be in the shape of an annular ring or alternatively, these spacers may be separate sections mounted upon the primary spacers, depending upon whether or not the primary spacers are of the ring or separate formations as described above.
- the secondary spacers or shims 19 are of some material which has a zero coefiicient of thermal expansion such as invar, for example, and are also of a standard thickness such as 1 or 2 mils, for example, depending of course upon the width of the desired air gap.
- a complete set of secondary spacers or shims are prepared, each of which is of a predetermined standard thickness, and each of which varies in thickness from the others by a standard predetermined amount. Since these secondary spacers are easily replaceable it is merely necessary to insert a certain selected spacer to obtain the desired width of air gap in the crystal housing.
- the piezo-electric material and the primary spacers have the same coefiicient of thermal expansion, variations in temperature of the primary spacers will not alter the width of the air gap. Also, since the Secondary spacers have a zero coefiicient of thermal expansion, the air gap will remain substantially constant as the temperature of the holder varies.
- the primary spacers shall also be of this material, for reasons apparent. If other than a zero coeflicient for the air gap is desired, secondary spacers having the desired coelficient would be used.
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- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Description
M y 9. 1933. J. w. CONKUN 1,908,320
PIEZO ELECTRIC CRYSTAL HOLDER Filed Dec. 9, 1929 INVENTOR J.W. CONKUN ATTOR N EY Patented May 9, 1933 UNITED STATES PATENT OFFICE JAMES W. CONKLIN, OF ROCKY POINT, NEW YORK, ASSIGNOR TO RADIO CORPORATION OF AMERICA, A CORPORATION OF DELAWARE PIEZO-ELEOTRIC CRYSTAL HOLDER Application filed December 9, 1929.
This invention relates to the pieZo-electric art and deals more specifically with a piezoelectric crystal holder or housing.
In piezo-electric crystal holders or housings, constructed in accordance with present day practice, it has been found that varlations in the ambient temperature of the housing, as well as variations in the temperature of the housing itself, and also of the crystal, cause corresponding variations in the width of the air gap between the crystal and plates or electrodes. It has been found in practice that this variation in the width of the air gap introduces serious errors in the operation of the crystal as a frequency standard or frequency control means.
It is therefore an object of this invention to provide a crystal holder or housing in which the plates are mounted so as to have an air gap or predetermined fixed width for varying conditions of temperature.
A further object of this invention is to provide a crystal holder in which the spacing of the electrodes is varied in a predetermined manner with changes in temperature.
It is a further object of this invention to provide a piezo-electric crystal holder having an air gap between the top plate and crystal, which air gap is designed to vary in accordance with a predetermined thermal coefficient.
It is a further object of this invention to provide certain standard spacing members,
' which may be selectively used to give a predetermined size of air gap in a piezo-electric crystal holder.
It is a further object of this invention to provide a pieZo-electric crystal holder, in which the spacing of the plates is predetermined in such a manner as to prevent variations in temperature of the housing or the material enclosed therein from affecting the desired frequency characteristic of the crystal oscillator.
Serial No. 412,687.
Further, it is an object of this invention to provide a pieZo-electric crystal housing having spacer members between the electrodes which are of the exact thickness of the piezo-electric material.
Finally, it is an object of this invention generally to improve the piezo-electric crys tal holder art by providing a housing or holder which is cheap to construct, easy to adjust and which is rugged and highly efii cient in its operation.
These and other objects of the invention will be readily apparent to those skilled in the art from the following description taken in connection with the accompanying drawing, in which:
Fig. l is a sectional view of a device embodying the present invention; and
Fig. 2 is a plan view of the device shown in Fig. 1. 65
In order to simplify the drawing the spacing between the oscillator and the elec trodes has been shown to be of considerable extent. It should be noted, however, that in actual practice this spacing is really only a few thousandths of an inch. Also, the terminals whereby the electrodes are connectedto an alternating current circuit have been omitted, for they may be readily applied in a manner now well understood in the art.
Referring in detail to the drawing, the holder or housing 10 is seen to comprise a lower plate 11 and an upper plate 12; both plates being of any suitable metal, preferably Monel metal. Between the plates 11 and 12 there is disposed thequartz spacer 13, which may be either an annular ring enclosing the crystal 14; or alternatively, separate spacer sections may be employed at suitable locations, whereby properly to separate and hold the plates 11 and 12 with respect to each other. The primary quartz spacer is of the same material and thickness as the crystal itself and preferably consists of pieces or corners of the particular crystal in use, which pieces or corners have been cut off after the grinding process of the crystal oscillator is completed. The screw members 15 pass through the upper electrode 12 and are fixed in the plate 11 in screw-threaded engagement therewith at 16. The plate 12 is provided With holes 12a through which the screw 15 passes. Coil springs 17 disposed between the head of the screw 15 and insulating bushings 18 press the plate 12 firmly against secondary spacers 19. The secondary spacers may be in the shape of an annular ring or alternatively, these spacers may be separate sections mounted upon the primary spacers, depending upon whether or not the primary spacers are of the ring or separate formations as described above. The secondary spacers or shims 19 are of some material which has a zero coefiicient of thermal expansion such as invar, for example, and are also of a standard thickness such as 1 or 2 mils, for example, depending of course upon the width of the desired air gap.
In accordance with the principles of this invention a complete set of secondary spacers or shims are prepared, each of which is of a predetermined standard thickness, and each of which varies in thickness from the others by a standard predetermined amount. Since these secondary spacers are easily replaceable it is merely necessary to insert a certain selected spacer to obtain the desired width of air gap in the crystal housing.
Since the piezo-electric material and the primary spacers have the same coefiicient of thermal expansion, variations in temperature of the primary spacers will not alter the width of the air gap. Also, since the Secondary spacers have a zero coefiicient of thermal expansion, the air gap will remain substantially constant as the temperature of the holder varies.
Where other piezo electric materials then quartz are used, the primary spacers shall also be of this material, for reasons apparent. If other than a zero coeflicient for the air gap is desired, secondary spacers having the desired coelficient would be used.
Many changes in the present disclosure will readily suggest themselves to those skilled in the art. It is therefore to be understood that this invention is not limited except as defined in the appended claims.
Having thus described my invention, I claim:
1. The combination with a piezo-electric crystal oscillator of a holder therefor, said holder comprising a first plate. spacer means mounted upon said plate. said means L 'g of the same material and substantially one exact same thickness as said crystal, a sec ond spacer means removably mounted upon said first mentioned spacer means, and a JAMES W. CONKLIN.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US412687A US1908320A (en) | 1929-12-09 | 1929-12-09 | Piezo-electric crystal holder |
DE1930537199D DE537199C (en) | 1929-12-09 | 1930-11-30 | Temperature compensated socket for piezo crystals |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US412687A US1908320A (en) | 1929-12-09 | 1929-12-09 | Piezo-electric crystal holder |
Publications (1)
Publication Number | Publication Date |
---|---|
US1908320A true US1908320A (en) | 1933-05-09 |
Family
ID=23634030
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US412687A Expired - Lifetime US1908320A (en) | 1929-12-09 | 1929-12-09 | Piezo-electric crystal holder |
Country Status (2)
Country | Link |
---|---|
US (1) | US1908320A (en) |
DE (1) | DE537199C (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2460153A (en) * | 1946-07-30 | 1949-01-25 | Gen Electric | Piezoelectric crystal holder |
US2497966A (en) * | 1946-01-26 | 1950-02-21 | Reeves Hoffman Corp | Crystal holder |
US2518793A (en) * | 1944-04-10 | 1950-08-15 | Helen Keller | Crystal mounting |
US4135108A (en) * | 1976-01-16 | 1979-01-16 | L'Etat Francais represente par le Delegue Ministeriel | Quartz resonator with electrodes that do not adhere to the crystal |
-
1929
- 1929-12-09 US US412687A patent/US1908320A/en not_active Expired - Lifetime
-
1930
- 1930-11-30 DE DE1930537199D patent/DE537199C/en not_active Expired
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2518793A (en) * | 1944-04-10 | 1950-08-15 | Helen Keller | Crystal mounting |
US2497966A (en) * | 1946-01-26 | 1950-02-21 | Reeves Hoffman Corp | Crystal holder |
US2460153A (en) * | 1946-07-30 | 1949-01-25 | Gen Electric | Piezoelectric crystal holder |
US4135108A (en) * | 1976-01-16 | 1979-01-16 | L'Etat Francais represente par le Delegue Ministeriel | Quartz resonator with electrodes that do not adhere to the crystal |
Also Published As
Publication number | Publication date |
---|---|
DE537199C (en) | 1931-10-30 |
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