US2459019A - Piezoelectric crystal filter - Google Patents
Piezoelectric crystal filter Download PDFInfo
- Publication number
- US2459019A US2459019A US718687A US71868746A US2459019A US 2459019 A US2459019 A US 2459019A US 718687 A US718687 A US 718687A US 71868746 A US71868746 A US 71868746A US 2459019 A US2459019 A US 2459019A
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- Prior art keywords
- crystal
- piezoelectric crystal
- electrodes
- capacitor
- frequency
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- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
- H03H9/46—Filters
- H03H9/54—Filters comprising resonators of piezo-electric or electrostrictive material
- H03H9/542—Filters comprising resonators of piezo-electric or electrostrictive material including passive elements
Definitions
- This invention relates to wave transmission networks and more particularly to wave filters which use piezoelectric crystals as impedance elements.
- the object of the invention is to increase the height and sharpness of an attenuation peak in a wave filter.
- the wave filter in accordance with the present invention is of the band-elimination type, that is, one having an attenuation band on each side of which is a transmission band.
- the lter comprises a piezoelectric crystal and a resistor.
- the crystal is dimensioned to be resonant at a frequency within the attenuation band and has two electrodes associated with one major face and a third electrode associated with the opposite face.
- One of the two electrodes is connected to an input terminal of the filter and the other to an output terminal.
- the third electrode is connected through a common shunt path to the remaining input and output terminals.
- the resistor is connected between the electrodes on the one side and given an ohmic value such as to balance the eiective resistance of the crystal at the resonant frequency. There is thus provided a comparatively narrow, sharply peaked attenuation band centered approximately at that frequency.
- a capacitor preferably variable, may be connected in the shunt path to adjust the location of the attenuation peak. Additional capacitors may be connected in shunt at the ends of the iilter to lower the image impedances, if desired.
- the lter comprises a piezoelectric crystal I dimensioned to be resonant at a frequency f within the band to be attenuated.
- Associated with one major face of the crystal I are two electrodes 2 and 3 which are connected, respectively, to an input terminal 4 and an output terminal 5.
- An electrode 6 associated with the opposite face of the crystal I is connected through a common shunt path 1 to the remaining input terminal 8 and output terminal 9.
- a resistor I0 which may be variable, is connected between the electrodes 2 and 3 and given a value approximately equal to four times the effective resistance of the crystal I at the frequency f with full plating on each side. In this way the resistance of the crystal I is balanced out in the lter circuit and there is provided a comparatively narrow, sharply peaked attenuation band centered approximately at the fre-- quency f, with adjacent transmission bands on each side thereof.
- the attenuation peak is slightly displaced from the frequency f due to the presence of stray capacitance, such as that between the electrodes 2 and 3.
- a capacitor II preferably variable, may be added in the common shunt path 'I to provide a precise adjustment of the frequency of this peak.
- the image impedances of the lter are too high for proper operation between the desired load impedances they may be lowered by adding the shunt capacitors I2 and I3 at the ends of the filter.
- the load impedance should have a value approximately equal in magnitude to the reactance of the end capacitor I2 or I3 at the fren quency f.
- a band-elimination wave filter comprising a pair of input terminals, a pair of output terminals, a piezoelectric crystal which is resonant at a frequency within the attenuation band, and a resistor, said crystal having two electrodes associated with one face and a third electrode associated with the opposite face, said two electrodes being connected, respectively, to one of said input terminals and one of said output terminals, said third electrode being connected through a common shunt path to the remaining terminals, and said resistor being connected loetween said two electrodes associated with said one face and having a value to balance the resistance of said crystal in the neighboring o said resonant frequency.
- a wave filter in accordance with claim l which includes a capacitor connected between -said input terminals and a second capacitor connected between said output terminals.
- a wave iilter in accordance with claim 1 which includes a capacitor in said common shunt path.
- a wave lter in accordance with claim 1 which includes a capacitor connected between said input terminals, a second capacitor connectedV between said output terminals, and a third capacitor in said common shunt path.
Description
Jan.. 11, 1949.
A. R. D HEEDEN E PIEZOEJECTRI C CRYSTAL FILTER Filed Dec. 27, 1946 A T TOP/JE V Patented Jan. 11, 1949 PIEZOELECTRIC CRYSTAL FILTER Albert R. Dheedene, Madison, N. J., assignor to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Application December 27, 1946, Serial No. 718,687
Claims.
This invention relates to wave transmission networks and more particularly to wave filters which use piezoelectric crystals as impedance elements.
The object of the invention is to increase the height and sharpness of an attenuation peak in a wave filter.
The wave filter in accordance with the present invention is of the band-elimination type, that is, one having an attenuation band on each side of which is a transmission band. The lter comprises a piezoelectric crystal and a resistor. The crystal is dimensioned to be resonant at a frequency within the attenuation band and has two electrodes associated with one major face and a third electrode associated with the opposite face. One of the two electrodes is connected to an input terminal of the filter and the other to an output terminal. The third electrode is connected through a common shunt path to the remaining input and output terminals. The resistor is connected between the electrodes on the one side and given an ohmic value such as to balance the eiective resistance of the crystal at the resonant frequency. There is thus provided a comparatively narrow, sharply peaked attenuation band centered approximately at that frequency. A capacitor, preferably variable, may be connected in the shunt path to adjust the location of the attenuation peak. Additional capacitors may be connected in shunt at the ends of the iilter to lower the image impedances, if desired.
'I'he nature of the invention will be more fully understood from the following detailed description and by reference to the accompanying drawing, the single iigure of which is a schematic circuit showing one embodiment of a bandelimination wave filter in accordance with the invention.
In the embodiment shown, the lter comprises a piezoelectric crystal I dimensioned to be resonant at a frequency f within the band to be attenuated. Associated with one major face of the crystal I are two electrodes 2 and 3 which are connected, respectively, to an input terminal 4 and an output terminal 5. An electrode 6 associated with the opposite face of the crystal I is connected through a common shunt path 1 to the remaining input terminal 8 and output terminal 9.
A resistor I0, which may be variable, is connected between the electrodes 2 and 3 and given a value approximately equal to four times the effective resistance of the crystal I at the frequency f with full plating on each side. In this way the resistance of the crystal I is balanced out in the lter circuit and there is provided a comparatively narrow, sharply peaked attenuation band centered approximately at the fre-- quency f, with adjacent transmission bands on each side thereof.
It may be found that the attenuation peak is slightly displaced from the frequency f due to the presence of stray capacitance, such as that between the electrodes 2 and 3. However, a capacitor II, preferably variable, may be added in the common shunt path 'I to provide a precise adjustment of the frequency of this peak.
If the image impedances of the lter are too high for proper operation between the desired load impedances they may be lowered by adding the shunt capacitors I2 and I3 at the ends of the filter. For an impedance match with the filter the load impedance should have a value approximately equal in magnitude to the reactance of the end capacitor I2 or I3 at the fren quency f.
What is claimed is:
1. A band-elimination wave filter comprising a pair of input terminals, a pair of output terminals, a piezoelectric crystal which is resonant at a frequency within the attenuation band, and a resistor, said crystal having two electrodes associated with one face and a third electrode associated with the opposite face, said two electrodes being connected, respectively, to one of said input terminals and one of said output terminals, said third electrode being connected through a common shunt path to the remaining terminals, and said resistor being connected loetween said two electrodes associated with said one face and having a value to balance the resistance of said crystal in the neighboring o said resonant frequency.
2. A wave filter in accordance with claim l which includes a capacitor connected between -said input terminals and a second capacitor connected between said output terminals.
3. A wave filter in accordance with claim 1 in which said resistor has a value approximately equal to four times the effective resistance of said crystal at said resonant frequency.
4. A wave iilter in accordance with claim 1 which includes a capacitor in said common shunt path.
5. A wave lter in accordance with claim 1 which includes a capacitor connected between said input terminals, a second capacitor connectedV between said output terminals, and a third capacitor in said common shunt path.
ALBERT R. DHEEDENE.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Number Name Date 2,198,684 Sykes Apr. 30, 1940 2,267,957 Sykes Dec. 30, 1941 2,308,397 Starr Jan. 12, 1943
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US718687A US2459019A (en) | 1946-12-27 | 1946-12-27 | Piezoelectric crystal filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US718687A US2459019A (en) | 1946-12-27 | 1946-12-27 | Piezoelectric crystal filter |
Publications (1)
Publication Number | Publication Date |
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US2459019A true US2459019A (en) | 1949-01-11 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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US718687A Expired - Lifetime US2459019A (en) | 1946-12-27 | 1946-12-27 | Piezoelectric crystal filter |
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Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2928069A (en) * | 1954-10-13 | 1960-03-08 | Gulton Ind Inc | Transducer |
US3009120A (en) * | 1961-11-14 | Electric | ||
US3168623A (en) * | 1954-10-13 | 1965-02-02 | Gulton Ind Inc | Piezoelectric transducer |
US3409787A (en) * | 1966-11-15 | 1968-11-05 | Air Force Usa | Piezoelectric transducer system |
FR2078805A5 (en) * | 1969-10-10 | 1971-11-05 | Motorola Inc | |
US4045753A (en) * | 1975-05-09 | 1977-08-30 | Toko, Inc. | Ceramic filter |
US4048595A (en) * | 1976-01-22 | 1977-09-13 | Westinghouse Electric Corporation | Information extraction for doppler radar |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2198684A (en) * | 1938-09-20 | 1940-04-30 | Bell Telephone Labor Inc | Wave filter |
US2267957A (en) * | 1940-09-14 | 1941-12-30 | Bell Telephone Labor Inc | Wave filter |
US2308397A (en) * | 1939-12-13 | 1943-01-12 | Rca Corp | Crystal filter circuit |
-
1946
- 1946-12-27 US US718687A patent/US2459019A/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2198684A (en) * | 1938-09-20 | 1940-04-30 | Bell Telephone Labor Inc | Wave filter |
US2308397A (en) * | 1939-12-13 | 1943-01-12 | Rca Corp | Crystal filter circuit |
US2267957A (en) * | 1940-09-14 | 1941-12-30 | Bell Telephone Labor Inc | Wave filter |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3009120A (en) * | 1961-11-14 | Electric | ||
US2928069A (en) * | 1954-10-13 | 1960-03-08 | Gulton Ind Inc | Transducer |
US3168623A (en) * | 1954-10-13 | 1965-02-02 | Gulton Ind Inc | Piezoelectric transducer |
US3409787A (en) * | 1966-11-15 | 1968-11-05 | Air Force Usa | Piezoelectric transducer system |
FR2078805A5 (en) * | 1969-10-10 | 1971-11-05 | Motorola Inc | |
US3727154A (en) * | 1969-10-10 | 1973-04-10 | Motorola Inc | Bandpass filter including monolithic crystal elements and resistive elements |
US4045753A (en) * | 1975-05-09 | 1977-08-30 | Toko, Inc. | Ceramic filter |
US4048595A (en) * | 1976-01-22 | 1977-09-13 | Westinghouse Electric Corporation | Information extraction for doppler radar |
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