GB2218855A - Waveguide apparatus - Google Patents
Waveguide apparatus Download PDFInfo
- Publication number
- GB2218855A GB2218855A GB8911532A GB8911532A GB2218855A GB 2218855 A GB2218855 A GB 2218855A GB 8911532 A GB8911532 A GB 8911532A GB 8911532 A GB8911532 A GB 8911532A GB 2218855 A GB2218855 A GB 2218855A
- Authority
- GB
- United Kingdom
- Prior art keywords
- mode
- waveguide
- signal
- signals
- aperture
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/16—Auxiliary devices for mode selection, e.g. mode suppression or mode promotion; for mode conversion
- H01P1/163—Auxiliary devices for mode selection, e.g. mode suppression or mode promotion; for mode conversion specifically adapted for selection or promotion of the TE01 circular-electric mode
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/06—Movable joints, e.g. rotating joints
- H01P1/062—Movable joints, e.g. rotating joints the relative movement being a rotation
- H01P1/066—Movable joints, e.g. rotating joints the relative movement being a rotation with an unlimited angle of rotation
- H01P1/067—Movable joints, e.g. rotating joints the relative movement being a rotation with an unlimited angle of rotation the energy being transmitted in only one line located on the axis of rotation
Description
1 2n18855 4 DRAFT I/7578/MRC WAVEGUIDE APPARATUS This invention relates to
waveguide apparatus and more particularly, but not exclusively, to apparatus for transforming signals between the TE 10 mode and the TE 01 mode.
In arrangements in which it is desired to transmit microwave radiation over an appreciable distance, for example to a remote antenna, the energy is often transmitted along a circular waveguide in the TE 01 mode. The TE 01 mode, which is illustrated in Figure 1, is one in which the electric field lines are circumferential and thus power losses tend to be small because they do not intercept the walls of the waveguide. The energy to be transmitted along the waveguide is normally generated in the TE 10 mode, as shown in Figure 2, which exists in rectangular waveguides and in which the electric field lines are generally parallel to the short sides of the waveguide. A transition section must be included to convert signals from the TE 10 mode into the TE 01 mode and consists of a tapered section in which the cross-section of the waveguide gradually changes from the rectangular shape to a circular section. The transition section must be relatively long in order to obtain a final signal having good mode purity, being typically of the order of one metre for signal frequencies of 6Ghz.
The present invention arose from an attempt to 2 - provide a more compact waveguide apparatus for transforming signals between the TE 10 and TE 01 modes.
- Acccording to the invention there is provided waveguide apparatus for transforming signals between the TE 10, mode and a circular waveguide mode comprising a Magic-T having its output ports arranged adjacent to one another and means for transmitting a signal via its E plane port and signals via its output port, such that a signal in the TE 10 mode applied to the E-plane port results in signals at the outputs which form a signal in the TE 20 mode, and means for using the signal in the TE 20 mode alone to produce the circular waveguide mode. By using apparatus in accordance with the invention, the circular mode can be produced from a signal in the TE 10 mode using a relatively small transition section which may be, for example, of the order of five times shorter than a conventional transition section. Preferably, the circular mode is the TE 01 mode. Normally, the input to a Magic-T is applied via its H-plane port and the E-plane port is connected to a load for matching purposes. By terminating the H-plane port and applying the input signal to the E plane port, the signals at the two outputs of the Magic-T are in the TE 10 mode in opposite senses. Thus, by arranging the outputs adjacent to one another, the two, opposite TE 10 modes combine to form a TE 20 mode, as shown in Figure 3, where the reference 1 indicates one of the Magic-T outputs and reference 2 the other. The 1 9 i production of the TE 20 mode is an intermediate point in the eventual transformation of the signal into the TE 01 mode or other circular mode. Apparatus in accordance with the invention may thus be made less bulky than conventional transition sections, which makes i t particularly advantageous for arrangements in which the waveguide is required to move, for example in a rotating joint. Of course, the Magic-T is a symmetrical device such that in apparatus in accordance with the invention, when a signal in the TE 20 mode is applied to the outputs of the Magic-T, a signal is derived from the E-plane port which is in the TE 10 mode. Thus, the waveguide apparatus may act to transform signals from the TE 10 mode into the TE 01 mode and vice-versa. Although apparatus in accordance with the invention may tend to have reduced bandwidth capability and mode purity compared to a conventional transition section, it has good matching characteristics and offers sufficiently good performance for its use to be advantageous in a number of applications.
In one embodiment of the invention a taper section is included which has an aperture therethrough, the transverse section of which is substantially rectangular at one end and substantially cruciform at its other end, the taper section being arranged such that signals from the Magic-T outputs are applied to the rectangular section part of the aperture. By using a taper section, the mode purity of the resultant signal in the TE 01 mode may be improved over what would otherwise be obtainable.
In another, particularly advantageous embodiment of the invention, a taper section is included having an aperture therethrough, the transverse section of the aperture being substantially rectangular at one end of the taper section and, at its other end, having two substantially concave sides which are joined by four substantially straight sides, the width of the.aperture being larger at the concave sides than at its centre, the taper section being arranged such that signals from the Magic-T outputs are applied to the part of the aperture having rectangular section.
It is further preferred that an iris is included, the iris "having a cruciform aperture therein via which signals from and to the Magic-T outputs are arranged to pass. The cruciform aperture is preferably arranged to overlap the non-rectangular end of the taper section. Again, the non-rectangular end of the taper section and the iris are also of use in transforming a signal in the TE 01 mode to the TE 10 mode.
I-t may be preferred that a waveguide rotating joint is included which is capable of transmitting two signals across the joint in respective different waveguide modes. Thus only one rotating joint is required for the transmission of two signals between relatively rotating members, whereas using previously known apparatus, a - f 2 4 d r separate rotating joint would have been required for each signal. The size of waveguide apparatus can therefore be reduced which is particularly important for example, in applications such as satellite communication equipment and in radar apparatus. The waveguide modes chosen must be such that there is little or no coupling between them. It is preferred that the two signals are at respective different frequencies. These frequencies might be, for example, 4 GHz and 6 GHz which are typical frequency bands for satellite communication down and up paths. By using widely spaced frequency bands for the two signals, any coupling between them tends to be further reduced.
It is preferred that the waveguide at the joint is circular, and that one mode is the TM 01 mode and the other is the TE 01 mode. When a signal in one of these modes is imposed on another signal in the other mode, the electric field lines of the two modes are orthogonal and there is substantially no coupling between them. Another advantage in employing these two modes is that there is only a very small electric field along the longitudinal axis in the TE 01 modes so that, for example, a cable may be positioned along it.
Some ways in which the invention may be performed is now described by way of example with reference to the accompanying drawings, in which:
Figure 4 is a schematic perspective view of a waveguide rotating joint which includes apparatus in accordance with the invention; Figure 5 is a schematic sectional view of the apparatus shown in Figure 4; Figure 6 is an explanatory diagram relating to the operation of the apparatus shown in Figure 4; Figure 7 is an exploded view of part of the rotating joint shown in Figure 4; Figure 8 shows part of another apparatus in accordance with the invention.
With reference to Figures 4 and 5, apparatus in accordance with the invention includes two circular waveguide sections 3 and 4 which are relatively rotatable at a rotating joint 5 about axis X-X. Two ports 6 and 7 are included for transmission of microwave energy across the rotating joint 5 in the TM 01 W. aveguide mode, which has radial electrical field lines as shown in Figure 6. Power in the TE 01 mode can also be transmitted across the rotating joint 5 via ports 8 and 9, between which the TM 01 ports 6 and 7 are located. The frequency of the TE 01 mode signal is different from that of the TM 01 mode signal.
TEO, port 8 is the E-plane input port of a Magic-T 10, the H-plane input port having a termination 11. As is more clearly shown in Figure 7, the two output ports 12 and 13 of the Magic-T 10 are arranged adjacent one another. Microwave energy applied in the TE10 mode to the port 8 reaches one of the outputs 12 in the TE 10 mode, as illustrated by the arrows, and the other output port 13 in v i 1.
1 the TE 10 mode in the opposite sense. Thus, the output of the Magic-T is effectively in the TE 20 mode.
The output of the Magic-T 10 is applied to a short taper 14 which has a rectangular section aperture on the side adjacent output ports 12 and 13 which opens out into a substantially cruciform section aperture at its other face. A made is set up at the cruciform aperture face of the taper 14 as illustrated by the arrows. Signals passed via the Magic-T outputs 12 and 13 and the taper 14 are then applied via a spacer 15 to an iris 16 having a cruciform aperture 17 therein. This sets up a mode at the iris 16 as illustrated by the arrows. The iris 16 is the last stage in the transition section 18 which produces the TE 01 mode in the circular waveguide at the joint 5. A similar transition section 19 is included on the other side of the rotating joint 5 and includes the port 9, which again is the E-plane port of a Magic-T.
The taper 14, or iris 16 where this is included, is arranged to present a short circuit at 20 (as shown in Figure 5) to energy passing through ports 6 and 7 so as to. inhibit the undesirable TE 11 mode.
Figure 8 shows another short taper 21 which may be used instead of the taper 14 shown in Figure 7. The taper 21 has a rectangular aperture 22 in one face which opens out into and aperture 23 having two curved sides and four straight side between them, as shown. This configuration give particularly good mode purity.
z 1
Claims (1)
- CLAIMS 1. Waveguide apparatus for transforming signals between the TE 10mode and a circular waveguide mode comprising a Magic-T having its output ports arranged adjacent one another and means for transmitting a signal via its Eplane port and signals via its output ports, such that a signal in the TE 10 mode applied to the E-plane port results in signals at the outputs which form a signal in the TE 20 mode, and means for using the singal in the TE 20 mode alone to produce the circular waveguide mode. 2. Apparatus as claimed in claim 1 wherein the circular waveguide mode is the TE 01 mode. 3. Apparatus as claimed in claim 1 or 2 and including a taper section having an aperture therethrough, the transverse section of the aperture being substantially rectangular at one end of the taper section and substantially cruciform at its other end, the taper section being arranged such that signals from the Magic-T outputs are applied to the part of the aperture having rectangular section. 4. Apparatus as claimed in claim 1 or 2 and including a taper section having an aperture therethrough, the transverse section of the aperture being substantially rectangular at one end of the taper section and, at its other end, having two substantially concave sides which are joined by four substantially straight sides, the width of the aperture be larger at the concave sides than at its1 Y centre, the taper section being arranged such that signals from the Magic- T outputs are applied to the part of the aperture having rectangular section. 5. Apparatus as claimed in claim any preceding and including an iris having a cruciform aperture therein via which signals from and/or to the Magic-T outputs are arranged to pass. 6. Apparatus as claimed in any preceding claim and including a waveguide rotating joint capable of transmitting two signals across the joint in respective different waveguide modes. 7. Waveguide apparatus as claimed in claim 6 wherein the two signals are at respective different frequencies. 8. Waveguide apparatus as claimed in claim 6 or 7 wherein the waveguide at the j.oint is circular and one mode is the TM 01 mode and the other is the TE 01 mode. 9. Apparatus as claimed in claim 8 wherein the rotating joint includes ports for the signal in the TM 01 mode located between ports for the signal in the TE 01 mode. 10. Waveguide apparatus as claimed in claim 9 wherein the signal in the TE 01 mode is transmitted into a resonant cavity at a distance from a port for the signal in the TM 01 mode such that it acts as a short circuit for the signal in the TM 01 mode. 11. Waveguide apparatus substantially as illustrated in and described with reference to Figure 7 or 8 of the accompanying drawings.Published 1989 atThePatent Office, State House, 66171 High Holborn, London WCIR4TP- Further copies maybe obtainedfrom The Patent Office. Sales Branch, St Mary Cray, Orpington, Kent BR,5 3RD. Printed by Multiplex techniques ltd, St Mary Cray, Kent, Con. 1187
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB888812091A GB8812091D0 (en) | 1988-05-21 | 1988-05-21 | Waveguide apparatus |
Publications (3)
Publication Number | Publication Date |
---|---|
GB8911532D0 GB8911532D0 (en) | 1989-07-05 |
GB2218855A true GB2218855A (en) | 1989-11-22 |
GB2218855B GB2218855B (en) | 1992-05-27 |
Family
ID=10637333
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB888812091A Pending GB8812091D0 (en) | 1988-05-21 | 1988-05-21 | Waveguide apparatus |
GB8911532A Expired - Fee Related GB2218855B (en) | 1988-05-21 | 1989-05-19 | Waveguide apparatus |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB888812091A Pending GB8812091D0 (en) | 1988-05-21 | 1988-05-21 | Waveguide apparatus |
Country Status (2)
Country | Link |
---|---|
EP (1) | EP0343887A1 (en) |
GB (2) | GB8812091D0 (en) |
Families Citing this family (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE202009006651U1 (en) * | 2008-12-30 | 2009-07-23 | Dr. Nathrath, Trümper, Partnerschaft Ingenieure | Mirowellen swivel coupling for rectangular waveguide |
CN101789535A (en) * | 2010-03-10 | 2010-07-28 | 北京纳诺帕技术中心 | Single-mode cylindrical microwave cavity |
RU2626726C1 (en) * | 2016-07-12 | 2017-07-31 | Акционерное общество "Концерн воздушно-космической обороны "Алмаз-Антей"(АО "Концерн ВКО "Алмаз-Антей") | Compact 90-degree twisting in the rectangular waveguide |
CN106992337A (en) * | 2017-04-19 | 2017-07-28 | 桂林电子科技大学 | A kind of Ka wave bands circular waveguide TE01 mode exciters |
GB2593159A (en) * | 2020-03-12 | 2021-09-22 | Univ Lancaster | Method and apparatus for supplying electromagnetic power to a plasma vessel |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2471021A (en) * | 1944-08-15 | 1949-05-24 | Philco Corp | Radio wave guide |
US2656513A (en) * | 1949-12-29 | 1953-10-20 | Bell Telephone Labor Inc | Wave guide transducer |
US2825031A (en) * | 1951-12-15 | 1958-02-25 | Alford Andrew | Method of converting modes of wave motion for transmission from rectangular to circular wave guides |
FR1239182A (en) * | 1958-10-30 | 1960-08-19 | Thomson Houston Comp Francaise | Microwave operating mode changer |
US3100881A (en) * | 1960-10-19 | 1963-08-13 | Gen Electric | Waveguide system having mode converter for changing rectangular te10 mode into circular te01 at locus of waveguide window |
US3230484A (en) * | 1963-10-22 | 1966-01-18 | Lipetz Nathan | Waveguide transition between rectangular and circular waveguides |
FR1584009A (en) * | 1968-07-05 | 1969-12-12 | ||
US3633130A (en) * | 1970-07-15 | 1972-01-04 | Hughes Aircraft Co | Multichannel rotary joint supportive of energy in at least three mutually orthogonal circularly symmetric waveguide modes simultaneously |
US4654613A (en) * | 1985-08-02 | 1987-03-31 | Texas Instruments Incorporated | Radar rotary joint |
FR2598034B1 (en) * | 1986-04-28 | 1988-08-26 | Alcatel Espace | MICROWAVE ROTATING JOINT DEVICE |
-
1988
- 1988-05-21 GB GB888812091A patent/GB8812091D0/en active Pending
-
1989
- 1989-05-19 GB GB8911532A patent/GB2218855B/en not_active Expired - Fee Related
- 1989-05-19 EP EP89305128A patent/EP0343887A1/en not_active Withdrawn
Also Published As
Publication number | Publication date |
---|---|
EP0343887A1 (en) | 1989-11-29 |
GB8812091D0 (en) | 1988-06-22 |
GB8911532D0 (en) | 1989-07-05 |
GB2218855B (en) | 1992-05-27 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 19980519 |