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US3621484A - Helical resonator having variable capacitor which includes windings of reduced diameter as one plate thereof - Google Patents

Helical resonator having variable capacitor which includes windings of reduced diameter as one plate thereof Download PDF

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US3621484A
US3621484A US16903A US3621484DA US3621484A US 3621484 A US3621484 A US 3621484A US 16903 A US16903 A US 16903A US 3621484D A US3621484D A US 3621484DA US 3621484 A US3621484 A US 3621484A
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coil
windings
helical
diameter
helical resonator
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Dale L Shult
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Motorola Solutions Inc
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P7/00Resonators of the waveguide type
    • H01P7/005Helical resonators; Spiral resonators
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03JTUNING RESONANT CIRCUITS; SELECTING RESONANT CIRCUITS
    • H03J3/00Continuous tuning

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  • the other plate is partially formed by a wall of the housing which is adjacent to the windings of reduced diameter.
  • a screw extends through the foregoing wall into a hollow portion in the core enclosed by the windings of reduced diameter. Adjustment of the screw controls the resonant frequency of the cavity.
  • helical resonators may be comprised of an inductive element in the form of a helical coil and a capacitive element formed by the proximity of the coil to a metallic enclosure surrounding the helical coil.
  • the grounded or low impedance end of the coil is directly connected to the metal enclosure and the high impedance end is capacitively coupled to the enclosure.
  • the resonant frequency of the resonator is a function of the physical dimensions of the coil, the capacitive structure, and the distance between the high impedance end of the coil and the enclosure. Since it is desirable to adjust the resonant frequency of the resonator, some prior art helical resonators have included a member which is in electrical contact with the enclosure and which can be moved with respect to the high impedance endof the helical coil thereby varying the equivalent capacitance of the composite structure.
  • a helical coil is wound around and supported by a ceramic form.
  • the combination of the form and coil is positioned in a metallic enclosure.
  • One plate of a variable tuning capacitor thereof is comprised of an annular element, the position of which is adjustable with respect to the high impedance end of the coil by means of a threaded shaft in engagement with the enclosure.
  • the other plate is comprised of a metal tab which is soldered to the high impedance end of the coil. This tab provides sufficient capacitive coupling between the coil and the annular element so that movement of the annular element can produce an appreciable change in the resonant frequency of the structure.
  • the coil of the helical resonator has a tendency to vibrate like a coil spring about the ceramic form.
  • This vibration produces corresponding changes in the inductance which undesirably modulate the radio frequency (RF) electrical signal passing therethrough. Since this modulation may be at audio frequency, it can result in an undesirable ringing" sound which emanates from the speaker of the receiver.
  • RF radio frequency
  • the physical dimensions of the coil to undesirably change in response to the temperature variations to which mobile or portable equipment is often subjected thereby tending to detune the resonator.
  • the electrical connection between the tab and the high impedance end of the coil produce an electrical discontinuity in the coil thereby increasing the insertion loss of the resonator.
  • the ceramic coil form could be manufactured with grooves therein corresponding to the turns of the helical coil. After being positioned in the grooves, the turns of the coil could be anchored in place on the form with cement.
  • Another object of the invention is to provide a simple and A further object of the invention is to provide a helical resonator including a minimum number of parts which can be quickly and easily assembled.
  • a still further object of the invention is to provide an inexpensive helical resonator which is suitable for use in portable electronic equipment which is subjected to vibration and temperature change.
  • the helical resonator of one embodiment of the invention is comprised of a conductive housing which surrounds a coil mounted in a plastic form that has been injection molded thereabout.
  • the coil is embedded in the plastic form to prevent vibration of the coil.
  • the windings at one end of the coil have a reduced diameter with respect to the diameter of the rest of the windings.
  • the other end of the coil is grounded to a portion of the conductive cavity.
  • the form has a flange integral therewith which is located adjacent to the windings of reduced diameter for mounting the coil on an inside surface of a wall of the housing.
  • This wall and the windings form an equivalent capacitor which is tuned by a screw passing through the wall into a hollow area enclosed by the windings of reduced diameter. Adjustment of the screw varies the resonant frequency of the helical resonator.
  • FIG. I is a partially exploded view of an RF coupling circuit or preselector utilizing a plurality of helical resonators which are in the form of one embodiment of the invention
  • FIG. 2 is a perspective view of one of the coils included in the coupling circuit of FIG. 1;
  • FIG. 3 is a cross-sectional view of the RF coupling circuit of FIG. I showing the physical relation of a coil to a cavity and tuning element.
  • FIG. 1 there is depicted an RF coupling circuit 10 which may be utilized, for instance, to preselect signals within a predetermined frequency band passing therethrough from an antenna to the first RF amplifier stage of a receiver by reducing the amplitude of all Rf signals outside of the desired passband.
  • the coupling circuit includes a conductive housing comprised of a metallic or conductive lower portion I2 and a metallic upper portion or plate 14. Plate 14 is fastened onto lower portion 12 by screws passing through holes 15.
  • Lower portion 12 includes a plurality of walls or partitions 16 which divide up the space therein to form a plurality of cavities 18.
  • a helical coil 20 is disposed within each cavity 18.
  • each coil is conveniently grounded by soldering it to notches 22 in the sidewall of housing 12 which may be positioned at convenient points along the sidewall with respect to the cavity.
  • An electrical connection for applying an input signal to a coil at one end of coupling circuit 10 or deriving an output signal from a coil at the other end is made through a standard RF connector which passes through the end wall of the lower portion, such as connector 23.
  • the portion of connector 23, which is located inside of cavity 18, is directly connected to a selected point 24 on coil 20 through connecting wire 26.
  • the exact point of connection on the coil is chosen to provide impedance matching between the external circuitry and coupling circuit 10.
  • An aperture or window 28 is provided in each partition 16 to allow energy to be transferred between cavities 18 through magnetic field coupling.
  • the coupling to and from RF coupling circuit 10, as well as between the helical resonating sections thereof, is very efficient thus permitting the use of a plurality of sections without the need for amplifying means interposed therebetween.
  • the number of sections depends on the overall desired frequency response characteristic of the coupling circuit.
  • helical inductor 20 which is suitable for use in coupling circuit 10 is illustrated as being comprised of several turns 30 made in a single piece of heavy copper wire.
  • the inside portions of windings 30 are embedded in tubular insulating plastic support core 32.
  • the outside portions of winding 30 are exposed to facilitate soldering of connecting wires, such as connecting wire 26, thereto.
  • Plastic form 32 which may be injection molded about prewound coil 20, is formed into a single supporting structurecomprised of an upper portion 34 having a circular cross section of a given diameter, a lower portion 36 having a smaller diameter, and a flange portion 38 at one end thereof.
  • Plastic ribs 39 extend from flange 38 across the lower portion 36 to the lower edge of upper portion 34.
  • ribs may be molded at quadrature with respect to each other about the lower portion to add strength and rigidity to unit 40 comprised of coil 20 and form 32.
  • the inside of form 32 is hollow as shown in FIG. 3 to reduce electrical losses.
  • Flange 38 includes aperture or hole 41 which extends into the hollow inner portion of the core. Holes 42 and 43 are provided through flange 38 to facilitate the mounting of coil 20 in any one of cavities 18.
  • Form 32 may be molded from polypropylene which is an inexpensive, lightweight plastic having relatively low water absorption characteristics, and exhibits low loss to high radio frequencies. Since turns 30 of coil 20 are embedded or injection molded into the plastic of form 32, coil 20 cannot oscillate when subjected to mechanical vibration. Unit 40, therefore, is free from the problem, inherent in most prior art resonators, wherein vibration or oscillation of the coils produces a change in inductance therein which provides undesirable modulation of the RF signal passing therethrough at an audiofrequency. Unit 40 is inexpensive, rugged, and can be quickly and easily fabricated. Furthermore, unit 40 is suitable for use in portable electronic equipment subject to vibration.
  • FIG. 3 which shows a cross-sectional view of the coupling circuit of FIG. 1, illustrates the mounting of unit 40.
  • self-tapping screws 46 and 48 pass through holes 42 and 43 to fasten flange 38 to base portion 50 of housing 10.
  • Low impedance end 21 of coil 20 is grounded by soldering it in groove 22.
  • a resonant structure is formed by the interreaction of inductor 20, which may be considered as electrically analogous to the inner conductor of a quarter wave coaxial transmission line, and the metallic walls of housing 12, which may be considered as analogous the outer conductor of the coaxial line.
  • This coaxial line may be thought of as being end loaded by an equivalent capacitor connected from the center conductor or coil to the outer conductor or walls.
  • One plate of this equivalent capacitor is comprised of turns 54 and 56 at the high impedance end of the coil which have reduced diameter with respect to the other turns of coil 20.
  • the other plate is comprised of base portion 50 of housing and screw 52 which extends through tapped portion 53 of base 50 into hollow portion 58 of core 32.
  • the distance between end 60 of screw 52 and winding 56 is a measure of the thickness of the dielectric of the capacitor.
  • the helical resonator of this embodiment provides a simple and inexpensive mechanism comprised of turns 56 and 58 and screw 52 which effectively tunes the resonant frequency.
  • the structure of coil has an advantage compared with prior art structures in that essentially no electrical discontinuity is created by the gradual decrease or necking down" of the diameter of coil 20 to form the aforementioned plate for the equivalent capacitor.
  • the cost and difficulties encountered in manufacturing and assembling the resonator of the embodiment of the invention are substantially less than that required for prior art structures.
  • the plate formed by windings 54 and 56 is relatively close to the plate formed by base 50, the thermal expansion or contraction of the plastic of the form therebetween will cause a minimum detuning of the resonator with changes in ambient temperature.
  • a helical resonator for passing radiofreqnency signals within a predetermined frequency range including in combination:
  • a helical coil comprised of conductive windings, said windings having a first cross-sectional diameter along a first portion of said coil and a second cross-sectional diameter which is less than said first cross-sectional diameter along a second portion of said coil including an endmost windings;
  • a conductive member forming a cavity enclosing said coil to form a resonant structure
  • a coupling surface forming part of said conductive member which is positioned in a plane that is essentially parallel to said endmost winding, said surface thereby forming a first plate and said endmost winding forming a second plate of an equivalent capacitor with the distance between said coupling surface and said endmost winding being the thickness of the dielectric of said capacitor;
  • movable conductive means having a portion extending through said coupling surface toward said endmost winding of the coil, said means being adjustable to vary said portion thus changing the effective surface area of said first plate and the thickness of said dielectric to change the capacitance of said equivalent capacitor thereby adjusting the resonant frequency of the helical resonator.
  • the helical resonator of claim 1 further including a form for supporting said coil, said form having a first cross-sectional diameter extending along a first portion thereof corresponding to said first cross-sectional diameter of the coil;
  • said form further having a second cross-sectional diameter along a second portion thereof corresponding to said second cross-sectional diameter of the coil;
  • said second portion of the form having a hollow area
  • said flange means having an aperture opening into said hollow area
  • said movable conductive means being adjustable to extend through said aperture into said hollow area.
  • windings of said coil being partially embedded in the plastic material to prevent oscillation of the windings with respect to the form 6.
  • said plastic is polypropylene.
  • a coil structure for use in a helical resonator having an adjustable tuning member said coil structure including in combination:
  • a coil having a longitudinal axis and with a first portion having a plurality of helical windings, each of a first diameter and with a second portion extending along the axis away from said first portion and having at least one helical winding of a second diameter, said second portion including an endmost winding;
  • a cylindrical form for supporting said coil having first, second and third integral parts, said first part having a first diameter supporting said first portion of said coil, said second part extending from said first part and having a second diameter supporting said second portion of said coil, said third part extending from said second part and forming a flange for mounting said coil;
  • said flange having an aperture therein for receiving the adjustable tuning member.
  • said second portion of said coil includes a plurality of helical windings each of a diameter which is less than said first diameter.

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Abstract

A helical resonator is comprised of a coil embedded in a plastic core which has been injection molded thereabout and a conductive housing. Windings at one end of the coil have a reduced diameter with respect to the diameter of the rest of the windings of the coil to provide one plate of an equivalent variable capacitor. The other plate is partially formed by a wall of the housing which is adjacent to the windings of reduced diameter. A screw extends through the foregoing wall into a hollow portion in the core enclosed by the windings of reduced diameter. Adjustment of the screw controls the resonant frequency of the cavity.

Description

United States Patent [72] Inventor Dale IL. Shult Mount Prospect, Ill.
[21] Appl. No. 16,903
[22] Filed Mar. 5, I970 [45] Patented Nov. 16, 1971 [73] Assignee Motorola, Inc.
Franklin Park, Ill.
[54] HELICAL RESONATOR HAVING VARIABLE CAPACITOR WHICH INCLUDES WINDINGS OF REDUCED DIAMETER AS ONE PLATE THEREOF [56] References Cited UNITED STATES PATENTS 2,190,082 2/1940 Polydorolf 334/76 X Primary Examiner-Herman Karl Saalbach Assistant Examiner-Marvin Nussbaum Attorney-Mueller, and Aichele ABSTRACT: A helical resonator is comprised of a coil embedded in a plastic core which has been injection molded thereabout and a conductive housing. windings at one end of the coil have a reduced diameter with respect to the diameter of the rest of the windings of the coil to provide one plate of an equivalent variable capacitor. The other plate is partially formed by a wall of the housing which is adjacent to the windings of reduced diameter. A screw extends through the foregoing wall into a hollow portion in the core enclosed by the windings of reduced diameter. Adjustment of the screw controls the resonant frequency of the cavity.
HELICAL RESONATOR HAVING VARIABLE CAPACITOR WHICH INCLUDES WINDINGS OF REDUCED DIAMETER AS ONE PLATE THEREOF BACKGROUND OF THE INVENTION Radio equipment and other electronic apparatus operating at high frequencies have utilized helical resonators as tuning elements to select signals within desired frequency ranges. Such resonators may be comprised of an inductive element in the form of a helical coil and a capacitive element formed by the proximity of the coil to a metallic enclosure surrounding the helical coil. The grounded or low impedance end of the coil is directly connected to the metal enclosure and the high impedance end is capacitively coupled to the enclosure. The resonant frequency of the resonator is a function of the physical dimensions of the coil, the capacitive structure, and the distance between the high impedance end of the coil and the enclosure. Since it is desirable to adjust the resonant frequency of the resonator, some prior art helical resonators have included a member which is in electrical contact with the enclosure and which can be moved with respect to the high impedance endof the helical coil thereby varying the equivalent capacitance of the composite structure.
The structure of prior art helical resonators, however, has been found to be either inadequate or unduly expensive in some applications. In one prior art embodiment, for instance, a helical coil is wound around and supported by a ceramic form. The combination of the form and coil is positioned in a metallic enclosure. One plate of a variable tuning capacitor thereof is comprised of an annular element, the position of which is adjustable with respect to the high impedance end of the coil by means of a threaded shaft in engagement with the enclosure. The other plate is comprised of a metal tab which is soldered to the high impedance end of the coil. This tab provides sufficient capacitive coupling between the coil and the annular element so that movement of the annular element can produce an appreciable change in the resonant frequency of the structure.
Although the foregoing embodiment works well in most applications, if the helical resonator is included in a mobile receiver, for instance, which may be subjected to mechanical vibration, the coil of the helical resonator has a tendency to vibrate like a coil spring about the ceramic form. This vibration produces corresponding changes in the inductance which undesirably modulate the radio frequency (RF) electrical signal passing therethrough. Since this modulation may be at audio frequency, it can result in an undesirable ringing" sound which emanates from the speaker of the receiver. Moreover, it is possible for the physical dimensions of the coil to undesirably change in response to the temperature variations to which mobile or portable equipment is often subjected thereby tending to detune the resonator. Furthermore, the electrical connection between the tab and the high impedance end of the coil produce an electrical discontinuity in the coil thereby increasing the insertion loss of the resonator.
To overcome the problems created by vibration and changes in dimension with temperature of the coil, it has been proposed that the ceramic coil form could be manufactured with grooves therein corresponding to the turns of the helical coil. After being positioned in the grooves, the turns of the coil could be anchored in place on the form with cement. Although these precautions may satisfactorily solve the particular problems associated with vibration, the resulting resonator is disadvantageous because it is relatively expensive and complex.
SUMMARY OF THE INVENTION Hence, it is an object of the present invention to provide a simple, inexpensive and rugged structure for a helical resonator.
Another object of the invention is to provide a simple and A further object of the invention is to provide a helical resonator including a minimum number of parts which can be quickly and easily assembled.
A still further object of the invention is to provide an inexpensive helical resonator which is suitable for use in portable electronic equipment which is subjected to vibration and temperature change. I
In brief, the helical resonator of one embodiment of the invention is comprised of a conductive housing which surrounds a coil mounted in a plastic form that has been injection molded thereabout. The coil is embedded in the plastic form to prevent vibration of the coil. The windings at one end of the coil have a reduced diameter with respect to the diameter of the rest of the windings. The other end of the coil is grounded to a portion of the conductive cavity. The form has a flange integral therewith which is located adjacent to the windings of reduced diameter for mounting the coil on an inside surface of a wall of the housing. This wall and the windings form an equivalent capacitor which is tuned by a screw passing through the wall into a hollow area enclosed by the windings of reduced diameter. Adjustment of the screw varies the resonant frequency of the helical resonator.
BRIEF DESCRIPTION OF THE DRAWING FIG. I is a partially exploded view of an RF coupling circuit or preselector utilizing a plurality of helical resonators which are in the form of one embodiment of the invention;
FIG. 2 is a perspective view of one of the coils included in the coupling circuit of FIG. 1; and
FIG. 3 is a cross-sectional view of the RF coupling circuit of FIG. I showing the physical relation of a coil to a cavity and tuning element.
DESCRIPTION THE PREFERRED EMBODIMENT In FIG. 1 there is depicted an RF coupling circuit 10 which may be utilized, for instance, to preselect signals within a predetermined frequency band passing therethrough from an antenna to the first RF amplifier stage of a receiver by reducing the amplitude of all Rf signals outside of the desired passband. The coupling circuit includes a conductive housing comprised of a metallic or conductive lower portion I2 and a metallic upper portion or plate 14. Plate 14 is fastened onto lower portion 12 by screws passing through holes 15. Lower portion 12 includes a plurality of walls or partitions 16 which divide up the space therein to form a plurality of cavities 18. A helical coil 20 is disposed within each cavity 18. The top or low impedance end 21 of each coil is conveniently grounded by soldering it to notches 22 in the sidewall of housing 12 which may be positioned at convenient points along the sidewall with respect to the cavity. An electrical connection for applying an input signal to a coil at one end of coupling circuit 10 or deriving an output signal from a coil at the other end is made through a standard RF connector which passes through the end wall of the lower portion, such as connector 23. The portion of connector 23, which is located inside of cavity 18, is directly connected to a selected point 24 on coil 20 through connecting wire 26. The exact point of connection on the coil is chosen to provide impedance matching between the external circuitry and coupling circuit 10. An aperture or window 28 is provided in each partition 16 to allow energy to be transferred between cavities 18 through magnetic field coupling. The coupling to and from RF coupling circuit 10, as well as between the helical resonating sections thereof, is very efficient thus permitting the use of a plurality of sections without the need for amplifying means interposed therebetween. The number of sections depends on the overall desired frequency response characteristic of the coupling circuit.
Referring now to FIG. 2, helical inductor 20 which is suitable for use in coupling circuit 10 is illustrated as being comprised of several turns 30 made in a single piece of heavy copper wire. The inside portions of windings 30 are embedded in tubular insulating plastic support core 32. The outside portions of winding 30 are exposed to facilitate soldering of connecting wires, such as connecting wire 26, thereto. Plastic form 32, which may be injection molded about prewound coil 20, is formed into a single supporting structurecomprised of an upper portion 34 having a circular cross section of a given diameter, a lower portion 36 having a smaller diameter, and a flange portion 38 at one end thereof. Plastic ribs 39 extend from flange 38 across the lower portion 36 to the lower edge of upper portion 34. These ribs may be molded at quadrature with respect to each other about the lower portion to add strength and rigidity to unit 40 comprised of coil 20 and form 32. The inside of form 32 is hollow as shown in FIG. 3 to reduce electrical losses. Flange 38 includes aperture or hole 41 which extends into the hollow inner portion of the core. Holes 42 and 43 are provided through flange 38 to facilitate the mounting of coil 20 in any one of cavities 18.
Form 32 may be molded from polypropylene which is an inexpensive, lightweight plastic having relatively low water absorption characteristics, and exhibits low loss to high radio frequencies. Since turns 30 of coil 20 are embedded or injection molded into the plastic of form 32, coil 20 cannot oscillate when subjected to mechanical vibration. Unit 40, therefore, is free from the problem, inherent in most prior art resonators, wherein vibration or oscillation of the coils produces a change in inductance therein which provides undesirable modulation of the RF signal passing therethrough at an audiofrequency. Unit 40 is inexpensive, rugged, and can be quickly and easily fabricated. Furthermore, unit 40 is suitable for use in portable electronic equipment subject to vibration.
FIG. 3, which shows a cross-sectional view of the coupling circuit of FIG. 1, illustrates the mounting of unit 40. In particular, self-tapping screws 46 and 48 pass through holes 42 and 43 to fasten flange 38 to base portion 50 of housing 10. Low impedance end 21 of coil 20 is grounded by soldering it in groove 22. A resonant structure is formed by the interreaction of inductor 20, which may be considered as electrically analogous to the inner conductor of a quarter wave coaxial transmission line, and the metallic walls of housing 12, which may be considered as analogous the outer conductor of the coaxial line. This coaxial line may be thought of as being end loaded by an equivalent capacitor connected from the center conductor or coil to the outer conductor or walls. One plate of this equivalent capacitor is comprised of turns 54 and 56 at the high impedance end of the coil which have reduced diameter with respect to the other turns of coil 20. The other plate is comprised of base portion 50 of housing and screw 52 which extends through tapped portion 53 of base 50 into hollow portion 58 of core 32. The distance between end 60 of screw 52 and winding 56 is a measure of the thickness of the dielectric of the capacitor. Hence, as screw 52 is adjusted so that it protrudes further into hollow portion 58, the effective plate area is increased and the thickness of the dielectric is decreased, both of which contribute to an increase in the capacitance of the equivalent capacitor. This change in equivalent capacitance varies the resonant frequency of the helical resonator.
Because of the proximity of windings 54 and 56 to tuning screw 52, adjustment of tuning screw 52 effectively controls the value of the equivalent capacitor. Hence, one turn of screw 52 provides a relatively large change in the resonant frequency. The helical resonator of this embodiment, therefore, provides a simple and inexpensive mechanism comprised of turns 56 and 58 and screw 52 which effectively tunes the resonant frequency. Moreover, the structure of coil has an advantage compared with prior art structures in that essentially no electrical discontinuity is created by the gradual decrease or necking down" of the diameter of coil 20 to form the aforementioned plate for the equivalent capacitor. The cost and difficulties encountered in manufacturing and assembling the resonator of the embodiment of the invention are substantially less than that required for prior art structures. Furthermore, since the plate formed by windings 54 and 56 is relatively close to the plate formed by base 50, the thermal expansion or contraction of the plastic of the form therebetween will cause a minimum detuning of the resonator with changes in ambient temperature.
The following table gives information pertinent to the construction of a helical resonator which has been made in accordance with the teaching of this invention and which has been tested and found suitable for use in a commercial radio preselector operable in the frequency range from megacycles to 180 megacycles.
Coil 20 is made from No. l 1 copper wire A=l l 2 inches B=0. inch C =0.8 inch D=l.25 inches E=l.25 inches F=l .75 inches G=O.29 inch H=0.65 inch What has been described, therefore, is a simple, rugged and inexpensive structure for a helical resonator which is suitable for use in mobile or portable RF apparatus which is subjected to vibration, moisture and temperature change.
i claim:
1. A helical resonator for passing radiofreqnency signals within a predetermined frequency range, such helical resonator including in combination:
a helical coil comprised of conductive windings, said windings having a first cross-sectional diameter along a first portion of said coil and a second cross-sectional diameter which is less than said first cross-sectional diameter along a second portion of said coil including an endmost windings;
a conductive member forming a cavity enclosing said coil to form a resonant structure;
a coupling surface forming part of said conductive member which is positioned in a plane that is essentially parallel to said endmost winding, said surface thereby forming a first plate and said endmost winding forming a second plate of an equivalent capacitor with the distance between said coupling surface and said endmost winding being the thickness of the dielectric of said capacitor;
movable conductive means having a portion extending through said coupling surface toward said endmost winding of the coil, said means being adjustable to vary said portion thus changing the effective surface area of said first plate and the thickness of said dielectric to change the capacitance of said equivalent capacitor thereby adjusting the resonant frequency of the helical resonator.
2. The helical resonator of claim 1 wherein said conductive windings are made of copper.
3. The helical resonator of claim 1 further including a form for supporting said coil, said form having a first cross-sectional diameter extending along a first portion thereof corresponding to said first cross-sectional diameter of the coil;
said form further having a second cross-sectional diameter along a second portion thereof corresponding to said second cross-sectional diameter of the coil;
flange means integral with one end of said second portion of the form, said flange means being connected to said coupling surface thereby mounting said coil thereon;
said second portion of the form having a hollow area;
said flange means having an aperture opening into said hollow area; and
said movable conductive means being adjustable to extend through said aperture into said hollow area.
4. The helical resonator of claim 3 wherein said coupling surface has a tapped hole extending therethrough to said aperture and wherein said movable conductive means is a screw in engagement with said hole and extending through said hole and said aperture into said hollow area.
5. The helical resonator of claim 3 wherein said form including said flange is comprised of a plastic material which is molded about said coil;
said windings of said coil being partially embedded in the plastic material to prevent oscillation of the windings with respect to the form 6. The helical resonator of claim 5 wherein said plastic is polypropylene.
7. A coil structure for use in a helical resonator having an adjustable tuning member, said coil structure including in combination:
a coil having a longitudinal axis and with a first portion having a plurality of helical windings, each of a first diameter and with a second portion extending along the axis away from said first portion and having at least one helical winding of a second diameter, said second portion including an endmost winding;
a cylindrical form for supporting said coil having first, second and third integral parts, said first part having a first diameter supporting said first portion of said coil, said second part extending from said first part and having a second diameter supporting said second portion of said coil, said third part extending from said second part and forming a flange for mounting said coil; and
said flange having an aperture therein for receiving the adjustable tuning member.
8. The coil structure of claim 7 wherein said second portion of said coil includes a plurality of helical windings each of a diameter which is less than said first diameter.

Claims (8)

1. A helical resonator for passing radiofreqnency signals within a predetermined frequency range, such helical resonator including in combination: a helical coil comprised of conductive windings, said windings having a first cross-sectional diameter along a first portion of said coil and a second cross-sectional diameter which is less than said first cross-sectional diameter along a second portion of said coil including an endmost windings; a conductive member forming a cavity enclosing said coil to form a resonant structure; a coupling surface forming part of said conductive member which is positioned in a plane that is essentially parallel to said endmost winding, said surface thereby forming a first plate and said endmost winding forming a second plate of an equivalent capacitor with the distance between said coupling surface and said endmost winding being the thickness of the dielectric of said capacitor; movable conductive means having a portion extending through said coupling surface toward said endmost winding of the coil, said means being adjustable to vary said portion thus changing The effective surface area of said first plate and the thickness of said dielectric to change the capacitance of said equivalent capacitor thereby adjusting the resonant frequency of the helical resonator.
2. The helical resonator of claim 1 wherein said conductive windings are made of copper.
3. The helical resonator of claim 1 further including a form for supporting said coil, said form having a first cross-sectional diameter extending along a first portion thereof corresponding to said first cross-sectional diameter of the coil; said form further having a second cross-sectional diameter along a second portion thereof corresponding to said second cross-sectional diameter of the coil; flange means integral with one end of said second portion of the form, said flange means being connected to said coupling surface thereby mounting said coil thereon; said second portion of the form having a hollow area; said flange means having an aperture opening into said hollow area; and said movable conductive means being adjustable to extend through said aperture into said hollow area.
4. The helical resonator of claim 3 wherein said coupling surface has a tapped hole extending therethrough to said aperture and wherein said movable conductive means is a screw in engagement with said hole and extending through said hole and said aperture into said hollow area.
5. The helical resonator of claim 3 wherein said form including said flange is comprised of a plastic material which is molded about said coil; said windings of said coil being partially embedded in the plastic material to prevent oscillation of the windings with respect to the form.
6. The helical resonator of claim 5 wherein said plastic is polypropylene.
7. A coil structure for use in a helical resonator having an adjustable tuning member, said coil structure including in combination: a coil having a longitudinal axis and with a first portion having a plurality of helical windings, each of a first diameter and with a second portion extending along the axis away from said first portion and having at least one helical winding of a second diameter, said second portion including an endmost winding; a cylindrical form for supporting said coil having first, second and third integral parts, said first part having a first diameter supporting said first portion of said coil, said second part extending from said first part and having a second diameter supporting said second portion of said coil, said third part extending from said second part and forming a flange for mounting said coil; and said flange having an aperture therein for receiving the adjustable tuning member.
8. The coil structure of claim 7 wherein said second portion of said coil includes a plurality of helical windings each of a diameter which is less than said first diameter.
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Cited By (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3763447A (en) * 1970-12-16 1973-10-02 Yagi Antenna High frequency helical filter
US3825862A (en) * 1972-11-01 1974-07-23 Alps Electric Co Ltd Helical resonator
DE2905677A1 (en) * 1978-02-27 1979-09-06 Motorola Inc CAVITY RESONATOR
US4342969A (en) * 1980-10-06 1982-08-03 General Electric Company Means for matching impedances between a helical resonator and a circuit connected thereto
WO1982003499A1 (en) * 1981-03-30 1982-10-14 Inc Motorola Helical resonator filter
US4422058A (en) * 1981-11-10 1983-12-20 Motorola, Inc. Folded-over helical resonator
EP0089964A4 (en) * 1981-08-04 1984-02-07 Motorola Inc Tunable helical resonator.
US4490699A (en) * 1982-05-27 1984-12-25 Alps Electric Co., Ltd. Intermediate frequency band-pass filter
US4977383A (en) * 1988-10-27 1990-12-11 Lk-Products Oy Resonator structure
EP0455505A3 (en) * 1990-05-04 1992-08-05 Lk-Products Oy Temperature compensation in a helix resonator
EP0623965A1 (en) * 1993-04-08 1994-11-09 Lk-Products Oy A method of making a coupling aperture for a filter
US5689221A (en) * 1994-10-07 1997-11-18 Lk Products Oy Radio frequency filter comprising helix resonators
US20030137369A1 (en) * 2002-01-23 2003-07-24 Bruker Biospin S.A. L-C type filter module and helical filter made up of at least two such modules
US20040075616A1 (en) * 2000-12-18 2004-04-22 Takanori Endo Antenna for rfid
US6816037B2 (en) * 1998-11-27 2004-11-09 Mark Allan Hoffman Helical filters and methods for specifying assembly thereof
US20110030197A1 (en) * 2009-08-10 2011-02-10 Lagrotta James Thomas Method of constructing a tunable rf filter
US20120249267A1 (en) * 2011-03-29 2012-10-04 Radio Frequency Systems, Inc. Radio frequency filter stabilization

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US2753530A (en) * 1950-11-04 1956-07-03 Itt High q. frequency tuner
US2982888A (en) * 1957-05-23 1961-05-02 Rea Magnet Wire Company Inc Sleeve type encapsulated electrical component
US2941172A (en) * 1957-09-24 1960-06-14 Essex Electronics Electrical winding construction
US3169234A (en) * 1959-08-17 1965-02-09 Coileraft Inc Coil form, and coils and transformers mounted thereto
US3138771A (en) * 1961-12-12 1964-06-23 Nytronics Inc Meltable plastic spacer for securing coil to tubular support and housing, and methodof assembly
US3247475A (en) * 1963-09-06 1966-04-19 Motorola Inc Helical resonator with variable capacitor having fixed plate which also functions as inductance
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Cited By (25)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3763447A (en) * 1970-12-16 1973-10-02 Yagi Antenna High frequency helical filter
US3825862A (en) * 1972-11-01 1974-07-23 Alps Electric Co Ltd Helical resonator
DE2905677A1 (en) * 1978-02-27 1979-09-06 Motorola Inc CAVITY RESONATOR
US4205286A (en) * 1978-02-27 1980-05-27 Motorola, Inc. Temperature stabilized helical resonator
US4342969A (en) * 1980-10-06 1982-08-03 General Electric Company Means for matching impedances between a helical resonator and a circuit connected thereto
WO1982003499A1 (en) * 1981-03-30 1982-10-14 Inc Motorola Helical resonator filter
US4374370A (en) * 1981-03-30 1983-02-15 Motorola, Inc. Helical resonator filter
EP0089964A4 (en) * 1981-08-04 1984-02-07 Motorola Inc Tunable helical resonator.
US4422058A (en) * 1981-11-10 1983-12-20 Motorola, Inc. Folded-over helical resonator
US4490699A (en) * 1982-05-27 1984-12-25 Alps Electric Co., Ltd. Intermediate frequency band-pass filter
US4977383A (en) * 1988-10-27 1990-12-11 Lk-Products Oy Resonator structure
US5159303A (en) * 1990-05-04 1992-10-27 Lk-Products Temperature compensation in a helix resonator
EP0455505A3 (en) * 1990-05-04 1992-08-05 Lk-Products Oy Temperature compensation in a helix resonator
EP0623965A1 (en) * 1993-04-08 1994-11-09 Lk-Products Oy A method of making a coupling aperture for a filter
US5508668A (en) * 1993-04-08 1996-04-16 Lk-Products Oy Helix resonator filter with a coupling aperture extending from a side wall
US5689221A (en) * 1994-10-07 1997-11-18 Lk Products Oy Radio frequency filter comprising helix resonators
US6816037B2 (en) * 1998-11-27 2004-11-09 Mark Allan Hoffman Helical filters and methods for specifying assembly thereof
US20040075616A1 (en) * 2000-12-18 2004-04-22 Takanori Endo Antenna for rfid
US7161542B2 (en) * 2000-12-18 2007-01-09 Mitsubishi Materials Corporation Antenna for RFID
US20030137369A1 (en) * 2002-01-23 2003-07-24 Bruker Biospin S.A. L-C type filter module and helical filter made up of at least two such modules
US6970058B2 (en) * 2002-01-23 2005-11-29 Bruker Biospin S.A. L-C type filter module and helical filter made up of at least two such modules
US20110030197A1 (en) * 2009-08-10 2011-02-10 Lagrotta James Thomas Method of constructing a tunable rf filter
US8333005B2 (en) * 2009-08-10 2012-12-18 James Thomas LaGrotta Method of constructing a tunable RF filter
US20120249267A1 (en) * 2011-03-29 2012-10-04 Radio Frequency Systems, Inc. Radio frequency filter stabilization
US8810339B2 (en) * 2011-03-29 2014-08-19 Alcatel Lucent Radio frequency filter stabilization

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