EP1389353A1 - Übertragungsleitung - Google Patents

Übertragungsleitung

Info

Publication number
EP1389353A1
EP1389353A1 EP02745389A EP02745389A EP1389353A1 EP 1389353 A1 EP1389353 A1 EP 1389353A1 EP 02745389 A EP02745389 A EP 02745389A EP 02745389 A EP02745389 A EP 02745389A EP 1389353 A1 EP1389353 A1 EP 1389353A1
Authority
EP
European Patent Office
Prior art keywords
conductive sheet
slots
conductor portion
another
slotted
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
Application number
EP02745389A
Other languages
English (en)
French (fr)
Other versions
EP1389353B1 (de
Inventor
Francisco Javier Vazquez Sanchez
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.)
ERA Patents Ltd
Original Assignee
ERA Patents Ltd
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
Application filed by ERA Patents Ltd filed Critical ERA Patents Ltd
Priority to EP02745389A priority Critical patent/EP1389353B1/de
Publication of EP1389353A1 publication Critical patent/EP1389353A1/de
Application granted granted Critical
Publication of EP1389353B1 publication Critical patent/EP1389353B1/de
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • 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
    • H01Q13/10Resonant slot antennas
    • H01Q13/106Microstrip slot antennas
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/2013Coplanar line filters
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P3/00Waveguides; Transmission lines of the waveguide type
    • H01P3/003Coplanar lines

Definitions

  • the present invention relates to electromagnetic transmission lines.
  • Microstrip, stripline and coplanar transmission lines have been developed as planar structures to guide electromagnetic energy. These planar structures can be used to implement circuits with surface mounted components and beamforming networks for planar antennas .
  • Transmission lines of this type typically require a continuous dielectric substrate or periodic spacers to maintain the correct separation between the transmission line conductors. Most commonly they are fabricated on dielectric substrates using low cost photolithographic techniques.
  • dielectric materials introduce additional losses which degrade the performance of the transmission lines.
  • the choice of suitable dielectric materials is limited, since any material must have low electrical losses and must comply with often stringent mechanical, chemical and thermal requirements. In some applications which involve particularly harsh environments, for example, space, aircraft, military, etc., dielectric materials cannot be used at all . Power handling is also limited due to electrical breakdown of the dielectric materials in the presence of high electromagnetic fields. Mechanically rigid, chemically stable dielectric materials with low losses at microwave and millimetre wave frequencies are expensive, becoming a limiting factor in the reduction of the cost of antenna and microwave technology.
  • planar array antennas eg for Ku-Band TVRO applications
  • the development of large planar array antennas has largely been limited by the losses in low cost dielectric substrates, since the gain of array antennas is physically limited by the insertion losses of the beamforming network.
  • the need to use high quality dielectrics is a major cost for planar antennas, reducing the economic advantage of using simple manufacturing techniques .
  • the suspended stripline concept was developed to avoid the costs and losses associated with high quality dielectric materials used in large antenna beamformer applications, see for example US-A-4614947 and US-A- 4527165.
  • the suspended stripline concept is based on using a thin sheet, typically less than 0.15mm thick, of dielectric material to support the central conductor of the stripline. As it is very thin, the contribution to losses from the dielectric substrate is minimised. This means that lower cost dielectric materials can be used, producing acceptable line attenuation (typically 2-4dB/m at 10GHz) at an acceptable price.
  • the suspended stripline concept there are a number of problems with the suspended stripline concept. Firstly, it still employs a dielectric substrate, albeit thin. Therefore, dielectric losses are not completely removed, and they can still represent a significant proportion of total losses, typically more than 50%, particularly when low cost dielectric materials are used. Secondly, even if the cost of the dielectric sheet is minimised by selecting low cost materials such as mylar, polystyrene or kapton, it can still represent about 20-30% of the total cost of the transmission line. Thirdly, as the dielectric sheet should be kept thin, it is not rigid and therefore not self- supporting. As a result, the channel width of suspended striplines is limited by mechanical constraints to a few millimetres (typically ⁇ 10mm) . Finally, the suspended line concept is very difficult to implement in open structures such as microstrip or coplanar lines.
  • a device for transmitting electromagnetic energy comprises a conductive sheet, the conductive sheet having: a conductor portion; at least one ground plane portion; and, two parallel rows of slots formed in the conductive sheet, separating the conductor portion from the or each ground plane portion, the slots in each row being periodically spaced from one another along the row and adjacent rows of slots being shifted relative to one another in the row direction.
  • the slots are all of identical length.
  • adjacent rows of slots are shifted relative to one another by half the length of the periodic spacing of the slots within each row.
  • the conductor portion is formed centrally on the conductive sheet, extends from one edge of the conductive sheet to another and is separated from the ground plane portions by two rows of slots formed on both sides of the conductor portion. More than two rows of slots may be used to separate the conductor from the ground plane to implement a multiconductor transmission line.
  • the conductor portion does not extend from one edge of the conductive sheet to another and comprises a widened end section, which in use forms a radiating element.
  • the present invention provides a low cost alternative to existing transmission lines and radiating elements, as there is no need to use expensive dielectric material in a device according to present invention.
  • transmission lines and radiating elements according to the present invention can be more finely tuned than conventional transmission lines and radiating elements and present minimal scattering of incident electromagnetic waves .
  • an additional conductive sheet is placed in a plane parallel to the slotted conductive sheet.
  • two additional conductive sheets are placed parallel to the slotted conductive sheet, one above and one below the slotted conductive sheet .
  • a conductive channel may back or completely surround the slotted conductive sheet.
  • a filter in a second aspect of the invention, includes a device according to the first aspect of the invention, wherein the frequency response includes a passband and selective attenuation at frequencies outside the passband.
  • Figure 1 is a schematic diagram of a transmission line according to present invention
  • Figure 2 is a graph showing the transmission characteristic of the transmission line shown in Figure 1;
  • Figure 3 is a schematic showing alternative embodiments of the present invention.
  • Figure 4 is a schematic diagram of a further embodiment of the present invention.
  • the dielectric-less transmission line described with reference to Figure 1 is coplanar (one metal plane) but the present invention can be embodied as a microstrip transmission line (two metal planes) or in stripline form
  • the transmission line of Figure 1 consists of a metallic sheet 1, which is perforated by two rows of slots 3, periodically distributed in a given direction. Adjacent rows of slots are displaced relative to one another by half the periodic inter-row spacing.
  • the slots define a central metallic region 4 which acts as the conductor of the transmission line itself, two inter-slot metallic regions between adjacent rows 5, and ground planes 2 on both sides.
  • the centres of slots in each row are separated by about half a wavelength at the nominal operating frequency, and slots in adjacent rows are offset by about a quarter wavelength.
  • a TEM type wave periodically loaded, is supported by the structure and it can be used to guide electromagnetic energy between the central conductor 4 and the two outer ground planes 2.
  • the conductor can be formed at the edge of a conductive sheet, with two rows of slots separating the conductor from the rest of the sheet.
  • the structure can be seen as a multi-conductor transmission line in which the conductors are short- circuited at alternated periodic intervals.
  • two possible symmetrical TEM waves are supported by the structure .
  • One TEM mode (Ml "resonating mode") is defined between the outer ground plane 2 and the central conductor 4, with the intermediate conductors at the same potential as the ground plane .
  • a second TEM mode (M2 "propagating mode") is defined when the intermediate conductors are at the mean potential between the central conductor 4 and the ground plane 2.
  • the structure can be seen as a transmission line supporting symmetrical mode M2, loaded periodically with short circuited stubs of line supporting the mode Ml.
  • the length of those stubs is half of the slot length and its period is the same as the slots 3.
  • the separation of the slots within each row is less than a tenth of the wavelength of the highest frequency of operation.
  • the separation between adjacent rows is about half the pitch of the slots.
  • the frequency response of the dielectric-less line is similar to some types of bandpass filter based on periodic loading of transmission lines with ⁇ resonating stubs .
  • the transmission line propagates energy in the frequency bands where the length of the slots 3 is close to n ⁇ /2 (n is an integer) .
  • the line provides selective filtering of signals outside the primary operating band of the transmission line.
  • a typical frequency response is shown in Figure 2.
  • the width of the transmission band can be controlled using the slot width and separation, as these parameters define the characteristic impedance of the resonating mode Ml.
  • the width of the central region can be used to control the impedance of the line since it defines characteristic impedance of the propagating mode M2.
  • Very large transmission bands typically up to 80%, can be achieved through proper design of the line.
  • the line characteristic impedance and propagation constant change with frequency, especially at the edges of the transmission band. In the central part of the band the line exhibits very low dispersion.
  • Multiple transmission lines can be formed on a single conductive sheet, with adjacent conductor portions separated by a common ground plane portion.
  • solder stripline shown in Figure 3c, or coaxial type, not shown
  • a metallic channel encloses the central metallic region.
  • the walls of the metallic channel are connected to the outer coplanar ground plane.
  • the dielectric-less lines can be used to implement power dividers, couplers and other passive devices typically used in microwave networks.
  • the lines may be curved by bending the slots accordingly whilst maintaining the slot period and length as constant as possible.
  • Power dividers for example T-splitters
  • T-splitters can also be implemented by bending the slots of the input line at the junction of the lines.
  • the central conductor width is used to control the impedance of the lines.
  • Impedance transformers can also be implemented by stepping the width of the central conductor at the mid-point of adjacent slots. The width of the slot should be also properly modified.
  • Radiating elements can also be directly implemented using dielectric-less lines.
  • the slots are excited by the TEM mode M2 as it propagates in the structure.
  • the line radiates energy which introduces additional line losses. This radiation is minimised when the width of the transmission line is much smaller than the wavelength.
  • the slots can be separated and enlarged to radiate energy.
  • a radiating slot can be directly fed from a dielectric-less line just by bending the adjacent slots 90° and widening them to obtain adequate impedance level and bandwidth.
  • Microstrip-like patch radiators can also be implemented from a dielectric-less microstrip by enlarging the central region of the line 20, creating a resonating cavity, as shown in Figure 4.
  • the slots surrounding the metallic central patch 21 form an array of radiators that drive the fields inside the cavity into the open space.
  • a key benefit of the present invention is the use of low cost manufacturing techniques for the implementation of the dielectric-less transmission line structures. Possible techniques for the manufacture of the central conductor include: sheet metal stamping or pressing, chemical etching, laser cutting, aluminium casting, plastic or metal injection moulding, and metallisation.
  • channelised microstrip or suspended stripline multilayer sheet metal structures, in which the intermediate layers are profiled to form channels, sheet metal pressing, aluminium casting, plastic or metal injection moulding, and metallisation.
  • an antenna according to the present invention may be desirable to include a layer of dielectric material in a transmission line or radiating element according to the present invention, in order to improve the mechanical characteristics of the structure.
  • a layer of dielectric material may be too flexible for a particular application. Insertion of a layer of dielectric material provides additional rigidity. Although this increases the expense of the antenna to that of a conventional antenna, it has benefits over a conventional antenna in that it is more highly tuned and hence is less susceptible to electromagnetic interference from outside the operating band of the antenna.
  • an antenna according to the present invention presents minimal scattering of incident electromagnetic waves.

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Waveguide Aerials (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)
  • Glass Compositions (AREA)
  • Addition Polymer Or Copolymer, Post-Treatments, Or Chemical Modifications (AREA)
  • Waveguides (AREA)
EP02745389A 2001-05-23 2002-05-22 Übertragungsleitung Expired - Lifetime EP1389353B1 (de)

Priority Applications (1)

Application Number Priority Date Filing Date Title
EP02745389A EP1389353B1 (de) 2001-05-23 2002-05-22 Übertragungsleitung

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
EP01304526 2001-05-23
EP01304526A EP1263077A1 (de) 2001-05-23 2001-05-23 Übertragungsleitung
PCT/EP2002/006591 WO2002095864A1 (en) 2001-05-23 2002-05-22 Transmitting line
EP02745389A EP1389353B1 (de) 2001-05-23 2002-05-22 Übertragungsleitung

Publications (2)

Publication Number Publication Date
EP1389353A1 true EP1389353A1 (de) 2004-02-18
EP1389353B1 EP1389353B1 (de) 2004-11-24

Family

ID=8181975

Family Applications (2)

Application Number Title Priority Date Filing Date
EP01304526A Withdrawn EP1263077A1 (de) 2001-05-23 2001-05-23 Übertragungsleitung
EP02745389A Expired - Lifetime EP1389353B1 (de) 2001-05-23 2002-05-22 Übertragungsleitung

Family Applications Before (1)

Application Number Title Priority Date Filing Date
EP01304526A Withdrawn EP1263077A1 (de) 2001-05-23 2001-05-23 Übertragungsleitung

Country Status (4)

Country Link
EP (2) EP1263077A1 (de)
AT (1) ATE283554T1 (de)
DE (1) DE60202061T2 (de)
WO (1) WO2002095864A1 (de)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011108725A1 (ja) * 2010-03-05 2011-09-09 日本電気株式会社 高周波伝送線路及び回路基板
RU2652169C1 (ru) 2017-05-25 2018-04-25 Самсунг Электроникс Ко., Лтд. Антенный блок для телекоммуникационного устройства и телекоммуникационное устройство
CN111129673B (zh) * 2018-11-01 2021-02-12 西安邮电大学 基于lcp工艺的超宽带带通滤波器

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4365222A (en) * 1981-04-06 1982-12-21 Bell Telephone Laboratories, Incorporated Stripline support assembly
US6198437B1 (en) * 1998-07-09 2001-03-06 The United States Of America As Represented By The Secretary Of The Air Force Broadband patch/slot antenna
JP3334680B2 (ja) * 1999-06-03 2002-10-15 株式会社村田製作所 高周波回路装置および通信装置

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
See references of WO02095864A1 *

Also Published As

Publication number Publication date
ATE283554T1 (de) 2004-12-15
DE60202061D1 (de) 2004-12-30
WO2002095864A1 (en) 2002-11-28
EP1389353B1 (de) 2004-11-24
EP1263077A1 (de) 2002-12-04
DE60202061T2 (de) 2005-04-07

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