EP0326498B1 - Resonanzschaltung und Filter mit dergleichen - Google Patents
Resonanzschaltung und Filter mit dergleichen Download PDFInfo
- Publication number
- EP0326498B1 EP0326498B1 EP19890400242 EP89400242A EP0326498B1 EP 0326498 B1 EP0326498 B1 EP 0326498B1 EP 19890400242 EP19890400242 EP 19890400242 EP 89400242 A EP89400242 A EP 89400242A EP 0326498 B1 EP0326498 B1 EP 0326498B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- filter
- resonator
- micro tape
- resonators
- sides
- 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
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/201—Filters for transverse electromagnetic waves
- H01P1/203—Strip line filters
- H01P1/20327—Electromagnetic interstage coupling
- H01P1/20354—Non-comb or non-interdigital filters
- H01P1/20381—Special shape resonators
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/08—Strip line resonators
- H01P7/082—Microstripline resonators
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/08—Strip line resonators
- H01P7/088—Tunable resonators
Definitions
- the present invention relates to a resonant circuit and a filter using this circuit.
- the technical field of the invention is radioelectricity, electronics, filtering and multiplexing of frequencies, etc.
- the invention finds a particular application in the construction of stations for receiving television signals broadcast by satellites.
- One of the problems posed in this technique is to produce, in the reception station, a filter operating in the frequency band 950-1750 MHz and making it possible to very easily rearrange the frequency plans, according to the availability of channels and user demand.
- the object of the present invention is precisely to remedy this deficiency by proposing a circuit and a filter which have all these advantages.
- Ring resonators which operate on the principle of establishing a standing wave regime.
- a conductive tape or microstrip is used, the length of which is equal to the wavelength associated with the resonant frequency (or possibly at half the wavelength).
- the shape of the ribbon is limited to a few simple shapes capable of leading to a high overvoltage. There are therefore in practice always circular rings or possibly U.
- the dimension of the circuit is, in essence, of the order of the wavelength. As soon as the frequency becomes low, the dimensions of the resonator become prohibitive. For example, at 30 MHz a resonator of the prior art constituted by a circular ribbon will have a diameter of 1.60 m.
- the object of the present invention is precisely to remedy these drawbacks. To this end, it recommends a resonant circuit still using a conductive tape but under very different operating conditions from those of the prior art.
- the ribbon plays the role of pure inductance in the band of use of the circuit. To do this, its length is taken less than ⁇ / 8, if ⁇ is the wavelength associated with the working frequency of the resonator.
- resonant loops comprising an interrupted microstrip loop of length ⁇ / 8 and a capacitor in the opening are already known from the prior art, see for example the document "1986 IEEE-MTT-S INTERNATIONAL MICROWAVE SYMPOSIUM DIGEST , Baltimore, Maryland, June 2-4, 1986, pages 411-414, IEEE, New York, US; M. MAKIMOTO et al .: 'Varactor tuned bandpass filters using microstrip-line ring resonators' ".
- the ribbon is a simple inductive element means that its shape is in no way critical. It is therefore possible to retain any desired shape, in particular shapes that allow the ribbon to be folded up to save space.
- the subject of the present invention is a filter comprising several resonant circuits as defined above. These circuits (identical or different) are coupled to each other.
- the coupling is tight, critical or loose depending on the case.
- shape of the ribbon is not critical, as has been pointed out above, we are free to choose the shape best suited to the chosen coupling.
- the invention thus finds a wide field of application. Filters from 30 MHz to 2 or 3 GHz can be produced. Bandwidth ranges from a few fractions of a percent to about 10%.
- a resonant circuit according to the invention is shown in Figure 1, in top view (a), in section (b) and in a variant with a metal case (c).
- This element comprises a planar substrate 10, made of dielectric material (for example epoxy glass, Teflon, etc.).
- a conductive layer 12 in copper for example
- a microstrip 14 made of conductive material ( copper for example).
- the circuit is arranged in a metal housing 20 and the ground plane is constituted by the metal walls 22 lower and upper.
- the microstrip draws an "open" outline in the sense that it incompletely surrounds part of the plane. In other words, it has at least one opening.
- this outline is rectangular and the opening (single) is referenced 16.
- Connected through this opening is a capacitor 18 adjustable or adjusted once and for all.
- FIG. 2 The equivalent electrical diagram is shown in FIG. 2, again considering the element in plan view (a) and in section (b) in the variant where the ground plane is arranged under the substrate.
- inductance L due to the non-rectilinear microstrip
- tuning capacitor Ca connected between the ends of the ribbon
- parasitic capacitors Cp which correspond to the volume separating the microstrip and the ground plan.
- l the length of the microstrip and by ⁇ the wavelength in the substrate at the operating frequency.
- the length l is always less than or equal to ⁇ / 8 in order to be able to be assimilated to an inductor independent of the frequency.
- the wavelength ⁇ o in the substrate corresponding to fo is determined, then the value of ⁇ o / 8 and a microstrip length less than this value is chosen.
- the value of the inductance L can be obtained approximately by the formula:
- the parasitic capacitance Cp value can be obtained by a formula of the type:
- the parameters of the resonant circuit are defined.
- the length of the coupled microstrip and the degree of coupling are determined experimentally.
- FIG. 5 shows a complete filter composed of five circuits C1 to C5 on a single substrate 10 with an input microstrip E and an output microstrip S.
- the filter of the invention uses a direct coupling at the input and output which performs the adaptation between the first and the last resonators and the circuits of use.
- the contours drawn by the microstrip are rectangular, two adjacent contours having two parallel sides. But one could also use triangular circuits for example mounted head to tail.
- circuits can be nested one inside the other.
- Figure 6 gives the main dimensions of an example filter designed to have a center frequency fo equal to 1131.620 MHz. Dimensions are in millimeters. The capacitors are adjustable from 0.5 to 5 pF. The substrate is made of 16/10 mm thick epoxy glass.
- the contours drawn by the microstrips are U-shaped, that is to say rectangles with one side missing.
- the orientation of these U alternates from one resonator to another, so that the capacitors are placed on both sides of the filter, sometimes at the top, sometimes at the bottom (in the sense of figure 6).
- Figures 7, 8 and 9 show the attenuation characteristic of a filter obtained according to the invention, with different frequency scales (on the abscissa).
- the curve goes from 1 to 2000 MHz; in FIG. 8, the width of the measurement band is 100 MHz; in Figure 9, it is 40 MHz.
- the curve in FIG. 10 represents the group time characteristic of the filter in nanoseconds by division.
Claims (3)
- Filter mit Flächenresonatoren, gebildet durch wenigstens zwei gekoppelte Resonatoren, wobei jeder Resonator umfaßt:- einen die Masseebene bildenden Leiter (12),- dieser Masseebene gegenüberstehend ein leitendes Mikrobändchen (14), aufgebracht auf eine der Seiten eines dielektrischen Substrats, wobei dieses Mikrobändchen eine Kontur beschreibt, die eine erste, durch eine Öffnung (16) unterbrochene Seite aufweist sowie eine zweite und eine dritte Seite, nichtunterbrochen und an an die erste Seite anschließend, und eventuell eine vierte, der ersten gegenüberliegende Seite, wobei die Länge des Mikrobändchens kleiner als λ/8 ist, wobei λ die der Resonanzfrequenz des Resonators zugeordnete Wellenlänge ist,- einen Kondensator (18), quer eingeschaltet in die Öffnung (16), die die erste Seite unterbricht,wobei dieses Filter dadurch gekennzeichnet ist:a) daß es mehr als zwei in Kaskadenschaltung angeordnete gekoppelte Resonatoren (C1, C2, C3, C4, C5) umfaßt,b) daß die gekoppelten Resonatoren so angeordnet sind, daß die zweiten und dritten nichtunterbrochenen Seiten von zwei benachbarten Resonatoren sich Seite an Seite befinden, wobei die elektrische Kopplung zwischen zwei benachbarten Resonatoren (C1, C2), (C2, C3), (C3, C4), (C4, C5) über die zweiten und dritten Seiten erfolgt; daß die ersten Seiten der Resonatoren mit ihren Kondensatoren sowie die eventuellen vierten Seiten angeordnet sind längs der Längsseiten des Filters, einmal auf einer der Längsseiten, einmal auf der anderen,c) daß der erste Resonator (C1) des Filters mit einem Generaleingang verbunden ist durch ein Eingangsmikrobändchen (E), direkt verbunden mit dem Mikrobändchen des ersten Resonators, wobei dieses Eingangsmikrobändchen (E) eine Adaptierung herstellt zwischen dem ersten Resonator (C1) und den Anwendungs-bzw. Ausgangsschaltungen,d) daß der letzte Resonator (C5) verbunden ist mit einem Generalausgang durch ein Ausgangsmikrobändchen (S), direkt verbunden mit dem Mikrobändchen des letzten Resonators, wobei dieses Ausgangsmikrobändchen (S) eine Adaptierung herstellt zwischen dem letzten Resonator (5) und den Anwendungs- bzw. Ausgangsschaltungen.
- Filter nach Anspruch 1, dadurch gekennzeichnet, daß jedes Mikrobändchen nur drei Seiten umfaßt und eine dreieckige Form aufweist, wobei die verschiedenen Dreiecke der verschiedenen Resonatoren entgegengesetzt angeordnet sind.
- Filter nach Anspruch 1, dadurch gekennzeichnet, daß jedes Mikrobändchen einen einwärtsgebogenen Teil aufweist.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR8801060A FR2626716B1 (fr) | 1988-01-29 | 1988-01-29 | Filtre a resonateurs plans |
FR8801060 | 1988-01-29 |
Publications (2)
Publication Number | Publication Date |
---|---|
EP0326498A1 EP0326498A1 (de) | 1989-08-02 |
EP0326498B1 true EP0326498B1 (de) | 1994-11-09 |
Family
ID=9362768
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP19890400242 Expired - Lifetime EP0326498B1 (de) | 1988-01-29 | 1989-01-27 | Resonanzschaltung und Filter mit dergleichen |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP0326498B1 (de) |
DE (1) | DE68919239T2 (de) |
FR (1) | FR2626716B1 (de) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6895262B2 (en) | 1993-05-28 | 2005-05-17 | Superconductor Technologies, Inc. | High temperature superconducting spiral snake structures and methods for high Q, reduced intermodulation structures |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7231238B2 (en) | 1989-01-13 | 2007-06-12 | Superconductor Technologies, Inc. | High temperature spiral snake superconducting resonator having wider runs with higher current density |
FR2704983B1 (fr) * | 1993-05-04 | 1995-06-09 | France Telecom | Filtre passe-bande a lignes couplees court-circuitees. |
US5888942A (en) * | 1996-06-17 | 1999-03-30 | Superconductor Technologies, Inc. | Tunable microwave hairpin-comb superconductive filters for narrow-band applications |
Family Cites Families (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2751558A (en) * | 1952-04-02 | 1956-06-19 | Itt | Radio frequency filter |
NL7314269A (nl) * | 1973-10-17 | 1975-04-21 | Philips Nv | Microgolfinrichting voorzien van een 1/2 lambda resonator. |
CA1097755A (en) * | 1976-02-26 | 1981-03-17 | Mitsuo Makimoto | Electrical tuning circuit |
FR2510325B1 (fr) * | 1981-07-24 | 1987-09-04 | Thomson Csf | Filtre hyperfrequence de petites dimensions, a resonateurs lineaires |
JPS61128602A (ja) * | 1984-11-28 | 1986-06-16 | Pioneer Answerphone Mfg Corp | マイクロ波用フイルタ |
-
1988
- 1988-01-29 FR FR8801060A patent/FR2626716B1/fr not_active Expired - Lifetime
-
1989
- 1989-01-27 EP EP19890400242 patent/EP0326498B1/de not_active Expired - Lifetime
- 1989-01-27 DE DE1989619239 patent/DE68919239T2/de not_active Expired - Fee Related
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6895262B2 (en) | 1993-05-28 | 2005-05-17 | Superconductor Technologies, Inc. | High temperature superconducting spiral snake structures and methods for high Q, reduced intermodulation structures |
Also Published As
Publication number | Publication date |
---|---|
FR2626716B1 (fr) | 1990-04-20 |
DE68919239T2 (de) | 1995-05-18 |
FR2626716A1 (fr) | 1989-08-04 |
EP0326498A1 (de) | 1989-08-02 |
DE68919239D1 (de) | 1994-12-15 |
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