US2530691A - Wave filter - Google Patents

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Publication number
US2530691A
US2530691A US614936A US61493645A US2530691A US 2530691 A US2530691 A US 2530691A US 614936 A US614936 A US 614936A US 61493645 A US61493645 A US 61493645A US 2530691 A US2530691 A US 2530691A
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United States
Prior art keywords
band
frequency
branch
filter
mid
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
Application number
US614936A
Inventor
Fox Arthur Gardner
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
AT&T Corp
Original Assignee
Bell Telephone Laboratories Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Priority to BE468045D priority Critical patent/BE468045A/xx
Priority to NL73887D priority patent/NL73887C/xx
Priority claimed from US452851A external-priority patent/US2432093A/en
Priority to GB22914/45A priority patent/GB578617A/en
Priority to GB18433/43A priority patent/GB578597A/en
Priority to US610957A priority patent/US2434645A/en
Priority to US610956A priority patent/US2607850A/en
Priority to US612680A priority patent/US2503549A/en
Priority to US612681A priority patent/US2422191A/en
Priority to US614937A priority patent/US2434646A/en
Application filed by Bell Telephone Laboratories Inc filed Critical Bell Telephone Laboratories Inc
Priority to US614936A priority patent/US2530691A/en
Priority to US614935A priority patent/US2432094A/en
Priority to CH265036D priority patent/CH265036A/en
Priority to FR938693D priority patent/FR938693A/en
Priority to US789811A priority patent/US2588226A/en
Priority to DEP28888A priority patent/DE818384C/en
Publication of US2530691A publication Critical patent/US2530691A/en
Application granted granted Critical
Priority to US266179A priority patent/US2740094A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/213Frequency-selective devices, e.g. filters combining or separating two or more different frequencies
    • H01P1/2138Frequency-selective devices, e.g. filters combining or separating two or more different frequencies using hollow waveguide filters
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/207Hollow waveguide filters
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/207Hollow waveguide filters
    • H01P1/209Hollow waveguide filters comprising one or more branching arms or cavities wholly outside the main waveguide
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P5/00Coupling devices of the waveguide type
    • H01P5/02Coupling devices of the waveguide type with invariable factor of coupling
    • H01P5/022Transitions between lines of the same kind and shape, but with different dimensions
    • H01P5/024Transitions between lines of the same kind and shape, but with different dimensions between hollow waveguides
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P5/00Coupling devices of the waveguide type
    • H01P5/08Coupling devices of the waveguide type for linking dissimilar lines or devices
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01QANTENNAS, i.e. RADIO AERIALS
    • H01Q13/00Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave

Definitions

  • the principal object of the invention is to transmit freely a band or bands of electromagnetic waves while eliectively blocking waves falling outside of the band or bands.
  • a further object is to improve the transmission characteristics of filters for use in wave guides.
  • a uniform metallic sheath with or without a dielectric filler will serve as a guide for suitable electromagnetic waves.
  • the sheath may be circular, rectangular, or of other shape.
  • the guide acts like a transmission line and has a specific propagation constant and characteristic impedance.
  • the element is primarily capacitive, and if parallel with the field, the element is primarily inductive.
  • the reactive impedance branch may be adjusted to provide a peak of attenuation, in the case of the band-pass filter, or a transmission peak, in the case of the band-suppression filter, at a frequency to one side or the other of the mid-band frequency.
  • Fig. 2 is a similar view of a modified form of the filter shown in Fig. 1.
  • Fig. 1 shows a band-suppression wave guide filter in accordance with the invention comprising a side-branch chamber III], opening into a main wave guide 96 through an aperture I06, and a second chamber I01, coupled to the chamber I I0 through an aperture I08 in the transverse partition I89.
  • Each of the chambers IE1! and III] is tuned to resonate at the mid-band frequency.
  • the filter will have two attenuation peaks the spacing between which depends upon the size of the aperture I03.
  • Fig. 2 shows a wave guide filter using a modified form of sid branch II I which may be designed either to transmit or to suppress a narrow band of frequencies.
  • the branch H4 comprises an end chamber I I I opening through an aperture II2 into a side-branch section II3 of length Q1 which connects the chamber I II with the main wave guide 96.
  • a reactive impedance branch Z4 Shunted across the section I I3 at a distance Q2 from a side of the main guide 96 is a reactive impedance branch Z4.
  • This branch may, for example, comprise a capacitive reactor or an inductive reactor.
  • a suitable variable capacitive reactor is shown in Fig. 8 of my above-mentioned Patent 2,432,093 and an appropriate variable inductive reactor is shown in Fig. 9 thereof. If the reactance Z4 is omitted, the transmission or suppression characteristic, as the case may be, will in general be unsymmetrical.
  • the impedance branch Z4 is introduced.
  • the distance Q2 is determined by finding experimentally a point of standing wave voltage minimum in the section H3.
  • the frequency of the waves is now changed to the desired frequency and the magnitude of the reactance Z4 adjusted to produce a peak of attenuation.
  • the value of Z4 is found first for a frequency at a certain distance to one side of the mid-band and then for a second frequency the same distance to the other side of the midband.
  • the reactance Z4 is then set at the average of the two values thus determined.
  • the adjustment is the same as just described except that the length Q1 is adjusted for reflection of power at the mid-band frequency and Z4 may be adjusted for a transmission peak at a frequency to one side or the other of the mid-band.
  • the wave guide 95 is assumed to be transmitting electromagnetic waves having their electric field polarized in the direction indicated by the arrow E.
  • a transmission line in the form of a hollow wave guide adapted for the through transmission of electromagnetic waves and a wave filter, said wave guide comprising an input section and an output section connected in tandem, said filter comprising a side branch closed at one end and at its other end opening into 'said wave guide atthe junction of said input andoutputsections, an apertured transverse partition positioned at an intermediate point in said branch to form an end chamber tuned to resonate at approximately the mid-band frequency of said filter, and a reactive shunt impedance branch-located in saidsidebranch between said partition and said wave guide at a point of standing wave voltage minimum'for said mid-band frequency, whereby wavesof one frequency will be freely transmitted from said input section to said output section but waves of a different frequency will be effectively prevented from passing from said input section to said output section.

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Description

Nov. 21, 1950 A. G. FOX 2,530,691
WAVE FILTER Original Filed July 30, 1942 //v l/E/V TOR A. 6. FOX
A T TOR/W5 5 Patented Nov. 21, 1950 WAVE FILTER Arthur Gardner Fox, Red Bank, N. J., assignor to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Original application July 30, 1942, Serial No.
452,851. Divided and this application September 7, 1945, Serial No. 614,936
7 Claims.
This invention relates to wave transmission networks and more particularly to frequency selective networks for use in the transmission of guided electromagnetic waves.
The principal object of the invention is to transmit freely a band or bands of electromagnetic waves while eliectively blocking waves falling outside of the band or bands. A further object is to improve the transmission characteristics of filters for use in wave guides.
A uniform metallic sheath with or without a dielectric filler will serve as a guide for suitable electromagnetic waves. In cross-section the sheath may be circular, rectangular, or of other shape. For all frequencies above a minimum, known as the cut-01f frequency, the guide acts like a transmission line and has a specific propagation constant and characteristic impedance.
of the electric field, the element is primarily capacitive, and if parallel with the field, the element is primarily inductive.
The wave guide filter in accordance with the present invention comprises a plurality of coupled chambers in a single side branch. For example, a first chamber may open into the main wave guide and a second chamber open into the first, The chambers may be formed by introducing one or more apertured transverse partitions into a side branch which is closed at one end and at its other end opens into the main guide. An improvement in the transmission characteristics may be obtained by connecting a reactive impedance branch, preferably variable, across the side branch at a selected point between the first apertured partition and the point of juncture between the branch and the main guide. The filter may be designed either to transmit or to suppress a band of frequencies. The end chamber is tuned to resonate at the desired mid-band frequency. The reactive impedance branch may be adjusted to provide a peak of attenuation, in the case of the band-pass filter, or a transmission peak, in the case of the band-suppression filter, at a frequency to one side or the other of the mid-band frequency.
This is a continuation in part of application Serial No. 422,408, filed December 10, 1941, now Patent 2,396,044, and a division of application Serial No. 452,851, filed July 30, 1942, now Patent 2,432,093.
The nature of the invention will be more fully understood from the following detailed description and by reference to the accompanying drawings, in which like reference characters refer to similar parts and in which:
Fig. 1 is a perspective View, partly cut away, of a Wave guide filter in accordance with the invention comprising two coupled chambers in a single side branch; and
Fig. 2 is a similar view of a modified form of the filter shown in Fig. 1.
Fig. 1 shows a band-suppression wave guide filter in accordance with the invention comprising a side-branch chamber III], opening into a main wave guide 96 through an aperture I06, and a second chamber I01, coupled to the chamber I I0 through an aperture I08 in the transverse partition I89. Each of the chambers IE1! and III] is tuned to resonate at the mid-band frequency. The filter will have two attenuation peaks the spacing between which depends upon the size of the aperture I03.
Fig. 2 shows a wave guide filter using a modified form of sid branch II I which may be designed either to transmit or to suppress a narrow band of frequencies. The branch H4 comprises an end chamber I I I opening through an aperture II2 into a side-branch section II3 of length Q1 which connects the chamber I II with the main wave guide 96. Shunted across the section I I3 at a distance Q2 from a side of the main guide 96 is a reactive impedance branch Z4. This branch may, for example, comprise a capacitive reactor or an inductive reactor. A suitable variable capacitive reactor is shown in Fig. 8 of my above-mentioned Patent 2,432,093 and an appropriate variable inductive reactor is shown in Fig. 9 thereof. If the reactance Z4 is omitted, the transmission or suppression characteristic, as the case may be, will in general be unsymmetrical.
The adjustment of the filter of Fig, 2 for the transmission of a narrow band of frequencies is as follows: First, the end chamber III is tuned to resonate at the desired mid-band frequency. Then the length Q1 of the section H3 is adjusted until waves of the mid-band frequency traveling through the main guide 96 are freely transmitted. In general the narrower the aperture H2 is made, the sharper will be the transmission band.
If it is desired to obtain a peak of attenuation at one side or the other of the transmission band, the impedance branch Z4 is introduced. The distance Q2 is determined by finding experimentally a point of standing wave voltage minimum in the section H3. The frequency of the waves is now changed to the desired frequency and the magnitude of the reactance Z4 adjusted to produce a peak of attenuation. On the other hand, if a symmetrical characteristic having maximum possible attenuation on either side of thetransmission band is desired, the value of Z4 is found first for a frequency at a certain distance to one side of the mid-band and then for a second frequency the same distance to the other side of the midband. The reactance Z4 is then set at the average of the two values thus determined.
For a band suppression characteristic the adjustment is the same as just described except that the length Q1 is adjusted for reflection of power at the mid-band frequency and Z4 may be adjusted for a transmission peak at a frequency to one side or the other of the mid-band.
In each of the figures the wave guide 95 is assumed to be transmitting electromagnetic waves having their electric field polarized in the direction indicated by the arrow E.
What is claimed is:
1. In combination, a transmission line 'in the form of a hollow wave guide adapted for the through transmission of electromagnetic waves and a wave filter, said wave guide comprising an input section and an output section connected in tandem, said filter comprising a side branch closed at one end and at its other end opening into 'said wave guide atthe junction of said input andoutputsections, an apertured transverse partition positioned at an intermediate point in said branch to form an end chamber tuned to resonate at approximately the mid-band frequency of said filter, and a reactive shunt impedance branch-located in saidsidebranch between said partition and said wave guide at a point of standing wave voltage minimum'for said mid-band frequency, whereby wavesof one frequency will be freely transmitted from said input section to said output section but waves of a different frequency will be effectively prevented from passing from said input section to said output section.
2. The combination in accordance with claim 1 in which said reactive shunt impedance branch comprises a variable capacitive reactor.
3. The combination in accordance with claim 1 in which said reactive shunt impedance branch comprises a variable inductive reactor.
4. The combination in accordance with claim 1 in which the distance between said partition and said wave guide is so chosen that waves of .said mid-band frequency are freely transmitted from said input section to said output section.
5. The combination in accordance with claim 4 in which the magnitude of the reactance of said shunt impedance branch is chosen to produce a peak of attenuation at a frequency near said mid-band frequency.
6. Fhe combination in accordance with claim 1 in which the distance between said partition and said wave guide is so chosen that waves of said mid-band frequency are reflected in said wave guide.
7. The combination in accordance with claim 6 in which the magnitude of the reactance of said shunt impedance branch is chosen to producea transmission peak ata frequency near said mid-band frequency.
ARTHUR GARDNER FOX.
REFERENCES CITED The following references are of record in the file of this patent:
UNITED STATES PATENTS Number Name Date 2,106,768 Southworth Feb. 1, 1938 2,253,503 Bowen Aug. 26, 1941 2,253,589 Southworth Aug. 26,1941 2,284,529 .Mason May 26, 1942 2,288,030 Salinger June 30, 1942 2,321,521 Salinger June 8, 1943 2,403,025 Samuel .July 2, 194.6
US614936A 1942-07-30 1945-09-07 Wave filter Expired - Lifetime US2530691A (en)

Priority Applications (16)

Application Number Priority Date Filing Date Title
BE468045D BE468045A (en) 1942-07-30
NL73887D NL73887C (en) 1942-07-30
GB22914/45A GB578617A (en) 1942-07-30 1943-11-05 Improvements in or relating to systems for transmitting guided electromagnetic waves
GB18433/43A GB578597A (en) 1942-07-30 1943-11-05 Improvements in or relating to systems for transmitting guided electromagnetic waves
US610957A US2434645A (en) 1942-07-30 1945-08-17 Wave guide bend
US610956A US2607850A (en) 1942-07-30 1945-08-17 Wave guide impedance element
US612681A US2422191A (en) 1942-07-30 1945-08-25 Impedance transformer for wave guides
US612680A US2503549A (en) 1942-07-30 1945-08-25 Impedance matching in wave guides
US614937A US2434646A (en) 1942-07-30 1945-09-07 Wave guide branching arrangement
US614936A US2530691A (en) 1942-07-30 1945-09-07 Wave filter
US614935A US2432094A (en) 1942-07-30 1945-09-07 Impedance transformer for wave guides
CH265036D CH265036A (en) 1942-07-30 1946-09-12 Filter for guided electromagnetic waves.
FR938693D FR938693A (en) 1942-07-30 1946-10-24 System for the transmission of guided electromagnetic waves
US789811A US2588226A (en) 1942-07-30 1947-12-05 Wave filter
DEP28888A DE818384C (en) 1942-07-30 1948-12-31 Filter for the transmission of a band in waveguides of guided electrical micro waves
US266179A US2740094A (en) 1942-07-30 1952-01-12 Wave-guide impedance elements

Applications Claiming Priority (7)

Application Number Priority Date Filing Date Title
US452851A US2432093A (en) 1942-07-30 1942-07-30 Wave transmission network
US610956A US2607850A (en) 1942-07-30 1945-08-17 Wave guide impedance element
US612680A US2503549A (en) 1942-07-30 1945-08-25 Impedance matching in wave guides
US614937A US2434646A (en) 1942-07-30 1945-09-07 Wave guide branching arrangement
US614936A US2530691A (en) 1942-07-30 1945-09-07 Wave filter
US789811A US2588226A (en) 1942-07-30 1947-12-05 Wave filter
US266179A US2740094A (en) 1942-07-30 1952-01-12 Wave-guide impedance elements

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US2530691A true US2530691A (en) 1950-11-21

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US610956A Expired - Lifetime US2607850A (en) 1942-07-30 1945-08-17 Wave guide impedance element
US612680A Expired - Lifetime US2503549A (en) 1942-07-30 1945-08-25 Impedance matching in wave guides
US614936A Expired - Lifetime US2530691A (en) 1942-07-30 1945-09-07 Wave filter
US614937A Expired - Lifetime US2434646A (en) 1942-07-30 1945-09-07 Wave guide branching arrangement
US789811A Expired - Lifetime US2588226A (en) 1942-07-30 1947-12-05 Wave filter
US266179A Expired - Lifetime US2740094A (en) 1942-07-30 1952-01-12 Wave-guide impedance elements

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US610956A Expired - Lifetime US2607850A (en) 1942-07-30 1945-08-17 Wave guide impedance element
US612680A Expired - Lifetime US2503549A (en) 1942-07-30 1945-08-25 Impedance matching in wave guides

Family Applications After (3)

Application Number Title Priority Date Filing Date
US614937A Expired - Lifetime US2434646A (en) 1942-07-30 1945-09-07 Wave guide branching arrangement
US789811A Expired - Lifetime US2588226A (en) 1942-07-30 1947-12-05 Wave filter
US266179A Expired - Lifetime US2740094A (en) 1942-07-30 1952-01-12 Wave-guide impedance elements

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US (6) US2607850A (en)
BE (1) BE468045A (en)
CH (1) CH265036A (en)
DE (1) DE818384C (en)
FR (1) FR938693A (en)
GB (1) GB578597A (en)

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RU2745591C1 (en) * 2020-08-17 2021-03-29 федеральное государственное бюджетное образовательное учреждение высшего образования "Национальный исследовательский университет "МЭИ" (ФГБОУ ВО "НИУ "МЭИ") Device for measuring the inherent quality of a dielectric resonator

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Also Published As

Publication number Publication date
GB578597A (en) 1946-07-04
BE468045A (en)
US2588226A (en) 1952-03-04
US2434646A (en) 1948-01-20
US2740094A (en) 1956-03-27
DE818384C (en) 1951-10-25
US2503549A (en) 1950-04-11
US2607850A (en) 1952-08-19
FR938693A (en) 1948-10-21
CH265036A (en) 1949-11-15

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