CA2103570C - Elliptical waveguide - Google Patents
Elliptical waveguide Download PDFInfo
- Publication number
- CA2103570C CA2103570C CA002103570A CA2103570A CA2103570C CA 2103570 C CA2103570 C CA 2103570C CA 002103570 A CA002103570 A CA 002103570A CA 2103570 A CA2103570 A CA 2103570A CA 2103570 C CA2103570 C CA 2103570C
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- Prior art keywords
- waveguide
- elliptical
- strip
- edge portions
- viewed
- 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.)
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P11/00—Apparatus or processes specially adapted for manufacturing waveguides or resonators, lines, or other devices of the waveguide type
- H01P11/001—Manufacturing waveguides or transmission lines of the waveguide type
- H01P11/002—Manufacturing hollow waveguides
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P3/00—Waveguides; Transmission lines of the waveguide type
- H01P3/12—Hollow waveguides
- H01P3/127—Hollow waveguides with a circular, elliptic, or parabolic cross-section
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P3/00—Waveguides; Transmission lines of the waveguide type
- H01P3/12—Hollow waveguides
- H01P3/14—Hollow waveguides flexible
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- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Waveguides (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
Elliptical waveguide is formed by feeding an electrically conductive strip (1) through a forming toot (2) and pressing the formed strip onto a mandrel (5) in a helical configuration. The adjacent edges of the strip are mechanically interlocked by folding over each other to impart flexible and twistable properties to the waveguide.
A seaming wire may be interposed in the folds to re-duce escape of electromagnetic energy. The edges may also be soldered to form flexible waveguide.
A seaming wire may be interposed in the folds to re-duce escape of electromagnetic energy. The edges may also be soldered to form flexible waveguide.
Description
~, ~. ~ 3'~ ~' ~
ELLIPTICAL WAVEGUIDE
TECHNICAL FIELD OF THE INVENTION
This invention relates to the manufacture of flexible or flexible and twistable elliptical waveguide.
BACKGROUND
Waveguides are widely used for the transmission of electromagnetic energy in the RF, microwave and millimetric wavelength range. Such transmission can take place within the confines of the conductive wall of the waveguidE~, with a minimum of loss, reflection and distortion of the signal.
Standard waveguides are formed of extruded rigid metal tubing which is available in approximately 4.5 metre straight lengths which can then be bent or twisted to shape using specialist manufacturing equipment. Longer lengths are attained by joining shorter lengths together using atandard or custom made flanges. In microwave systems it is common for the waveguide runs to require several bends and twists to enable the waveguide to avoid various obstacles in its path. The use of standard :rigid waveguides therefore requires the production of a series of detailed manufacturing drawings to accurately define the shape of the required waveguide. This adds to the cost of the system, as does the operation of forming the waveguide into shape SUBSTITUTc SHEET
_ 2~.~~~~~ ;13 MAY 1993 and the subsequent inspection and fitting of the waveguide. Ret ro-fitting and replacement of rigid waveguides is also a potentially expensive operation, especially in more complex systems.
An important tape of waveguide is elliptical cross section waveguide. This has a lower microwave loss when operating in the a TE 11 mode than the equivalent comparable standard rectangular waveguide. Elliptical waveguide is also capable of transmitting higher microwave power than the equivalent rectangular waveguide operating in the H 10 mode. Since the wall of elliptical wavec~uide is convexly curved in all areas, the external compressive strength of such waveguide is greater than that of rectangular or double ridged waveguide desigr.~ed to operate within the same frequency range. This increased resistance to deformation is of importance in adverse mechanical or environmental conditions.
Flexible elliptical waveguide is currently manufactured in two halves, each of which is pressed to form a series of transversely extending shallow corrugations. The two halves are then axially soldered, brazed or welded to form the compleite waveguide. In general however, this form of waveguide is very stiff to bend by hand and is not, to any significant extent, twistable. In addition, such elliptical waveguide is expensive to manufacture, and can only be manufactured in certain fixed sizes for which tools are available, and in fixed lengths.
SUMMARY OF THE ~LNVENTION
ur,~;E;a ~c;: ~~~tom a~-:~--: ~tt;cg - SUBSTITUTE ~HE~T
PCT irae~vliona~ A -: ~; ;v.ian According to the present invention there is provided tubular waveguide having a wall which, when viewed in longitudinal section, is formed in a series of external ribs separated by grooves, in which said wall comprises an electrically conductive metal strip formed in a generally helical configuration with adjacent edge portions of adjacent turns of the strip mechanically interlocked by being folded over each other, and in which said interlocked edge portions are disposed on the crest of said ribs, wherein when viewed in transverse cross section said waveguide is of substantially elliptical shape without straight regions, and when viewed in longitudinal section said interlocked edge portions comprise straight regions extending substantially parallel to the longitudinal direction of the waveguide for a major part of the length of said edge portions, and the bottom of the grooves are also substantially straight extending substanti<~lly parallel to the longitudinal direction of the waveguide.
It should be understood that the term "elliptical" as used herein is intended to cover other non-circular and substantially ellip;~e-like shapes such as ovals.
An electrically conductive element is preferably interposed between t:he folded edges to reduce electromagnetic leakage. In flexible and twistable waveguide there will usually be just a non-rigid mechanical interlock between adjacent turns, but flexible and non-twistable waveguides may be manufactured by rigidly securing they adjacent turns to each other, e.g.
by soldering, brazing or welding.
3A.
There is also disclosed a method of manufacturing tubular waveguide of substantially elliptical cross section, said waveguide having a wall which, when viewed in longitudinal section, is formed in a series of ribs separated by intervening grooves, said method comprising:
- continuously winding a pre-formed electrically conductive metal strip about a rotating mandrel of PCTlsB~2ioo2so _. ~~~~~~~~ X13 MAY 1993 substantially elliptical cross section in a generally helical configuration such that adjacent edge portions of adjacent turns of the strip are interengaged, the strip being wound onto the mandrel together with a support element: for supporting the interengaged edge portions of the strip, and - performing a secondary forming operation on said edge portions, whilst said edge portions are supported by the support element on the mandrel, so that said edge portions become folded over each other and form a mechanical interlock between said adjacent turns with said interlocked edge portions extending along the crest of said ribs.
BRIEF DESCRIPTION OF THE DRAWINGS
The invention is exemplified in the accompanying drawings, in which:
Fi ure 1 is a perspective view of waveguide of the invention in the process of manufacture, FiQUre la is an end view of the waveguide of Fig. 1 whilst wound on the mandrel, Fi ure 2 is a longitudinal section through a wall portion of the waveguide, Fi ure 3 is a further longitudinal section through a wall portion of a different waveguide of the invention ,, - r w ., y -- -_. _ ..___ _- ~-_-1 ' ,.J ,J
PC~10~~2/00~~~0 ~1~~~.~~~ '13 MAY 1993 FiQUre: 4 is a side view of a joint between two lengths of waveguide of the invention, FiQUrea 5 and 6 show an adaptor connected to an end of the waveguide in perspective view and longitudinal section respectively, and FiQUrea 7 to 9 are longitudinal sections through different forms of the adaptor.
DETAILED DESCRIPTION OF THE DRAWINGS
Hy way of example, the waveguide of the present invention may be manufactured from a thin (e. g. 0.106 mm) strip of brass, metal-plated brass (e.g. plated with a 3 to 4 um layer of silver, tin, gold, nickel or palladium nickel), or other metallic or conductive material (e. g. solid silver). The strip may typically be 5.715 mm wide:.
Referring to Fi.g. 1, the strip 1 is passed through formers 2 (e.g. rollers) which form the strip into the required cross-;sectional profile at 3. The profiled strip 3 is then fed through a forming tool 4 which feeds the strip aroundl a rotating elliptical arbour (mandrel) 5 of the required major and minor dimensions (e. g. 14.71 mm by 8.29 mm) such that adjacent turns 6 of the resulting helix 7 form a mechanical interlock with each other. Hy pre;ssing against the profiled strip, the forming tool 4 performs a final forming operation on the strip 3 so that 'the f final waveguide includes a series of angular helical ribs 6 of substantially square or '''~??-! ~ ~~ra~ic~:~;~~ _~d?~-roe ~.. ",. ~
,.r- ...~".,. , , . , , ~'~7:1~p26!~
~~~3~ ~o) ~13 MAY 1993 rectangular cross section separated by intervening grooves. As thE~ waveguide is formed it is pushed along the arbour 5 in direction 12 so that a continuous length of waveguide passes off the end of the arbour 5. The cross sectional size of the waveguide can easily be changed simply by changing the size of the arbour.
Figure 2 shows a mechanical interlock 8 which can be used to form flexible and twistable waveguide. The profiled strip 3 is wound onto the arbour 5 together with a support element 9 which supports the ribs 6 to prevent their collapse and also supports the interlock 8 during final engagement. The adjacent edges of the turns are folded back upon each other by the forming tool 4 to compleae the mechanical interlock 8, which is supported by th.e element 9 during manufacture of the waveguide. The element 9 may be an aluminium wire or a nylon filament, having a diameter of 0.91 mm for example.
The mechanical :interlock 8 of Fig. 2 also incorporates an electrically conductive seaming wire 10 which is wound onto the elliptical arbour 5 together with the profiled strip 3 and is interposed between the folded-back edges of adjacent turns 6. This seaming wire 10 may for example be of 0.21 mm thick copper wire plated with tin or silver. The seaming wire 10 enhances the mechanical performance of the waveguide and reduces microwave leakage from the waveguide.
The mechanical :interlock 8 which is shown in Fig. 3 is similar to that of Fi,g. 2 but is suitable for flexible and non-twistable waveguide. A support element 9 is United K:~gdom P-~~~L-~ ~~~ce SUBSTI~TUT~ ~H~~'T' PCZ~ ~aterr;a:;~~! A~:;~.:c~~ian PCT/~~~32/00261( _ ~~~~~~~~ ~j3 MAY 1993 again included, but the seaming wire 10 is replaced by a length of solder wire 11 of e.g. 0.23 mm diameter.
After formation of the helical waveguide as described, the waveguide is heated to melt the solder 11 which is then allowed to cool so that the adjacent turns 6 become rigidly bonded l.ogether in the region of the interlock 8.
Long lengths of the waveguide can be manufactured by joining shorter lengths using a jointing flange 15 ( Fig.
4) which is soldered, brazed or welded to the adjacent ends of the two lengths of waveguide. Another method is to join a new si.rip 3 onto the end of a previous strip 3 prior to application to the mandrel, by soldering brazing or welding or by other suitable means, so that the resulting waveguide is of a substantially continuous form with less-obvious joints.
The helix 7 ma5r be covered by a protective layer of elastomer, heat-shrunk polymer, organic or metallic braid, or the hike, to provide added environmental and mechanical protection. Flexible and twistable versions can have a further covering of an electrically conductive elasitomer for example, in order to provide improved electromagnetic screening and isolation properties.
Another version of the waveguide may be manufactured so that the screening effectiveness is deliberately very low, thus formir.~g a "leaky feeder" waveguide. This can be achieved by forming the waveguide with a loose, non-rigid interlocH: between adjacent turns, and/or by omitting the seeuning wire 10.
~id.a ~;;?C~t~Gttl1 ~dr~llt ~Jf~~f~ ~.,.,".~.-.r ~-~r~y ;nterng~tiona! Apolicat~on ~~~~' ~ ~ : ~~ i ~ ~i ~~==:~T
~~3 MAY 1993 s In order to electrically connect and match the elliptical waweguide to a different microwave transmission link, e.g. a standard rectangular waveguide, a spe~~ial elliptical-to-rectangular waveguide flanged adaptor is required. This can be soldered, clamped or attached by other suitable means onto the end of the elliptical waveguide. A suitable adaptor 20 is shown in Fig s 5 and 6, and comprises a rectangular-section waveguide part 21 which terminates in a flange interface 22. The opposite end of the rectangular part 21 is joined to an elliptical section 23, the internal dimensions of which are similar to those of the elliptical wavec~uide 7. The free end of the elliptical section 23 is provided with an internal annular recess 24 to receive the elliptical waveguide, which is soldered, mechanically fixed, adhesively bonded or otherwise secured therein. An internal step 25 is formed between 'the rectangular and elliptical sections 21 and 23. A set of tuning screws 26 are inserted through the wall of the rectangular and elliptical sections, and these screws are placed one eighth of a wavelength apart: so that by screwing them in and out of the adaptor theft can be tuned to match the rectangular and elliptical sections.
Instead of the step 25 the elliptical section of the adaptor 20 can t>e tapered, as shown in Fig. 7. In each case the tuning screws can be located in both of the wider walls of t:he waveguide or omitted altogether.
The adaptors of Fig. s 5 to 7 may be of brass, copper, aluminium, stainless steel, titanium, alloy or polymer.
The inner surface oflthe recess 24 may be plated with ~,~~:fd'e~~~o~&~ ~p~~ICca'~~(7 7 ~ "-~',~ ..::~.r 3 i i ~' i !'~
~ i ~ _ _ PCTIGBs2~oo2so silver, tin or cold for example, to aid soldering to the elliptical wave~~uide.
The waveguide o:E the invention could also be interfaced to other forms of transmission line via a similar matching adaptor of suitable design, for example circular, double ridge, single ridge, and quad ridged dielectric wave;guides, or elliptical waveguide of a different size or orientation. Fig. 8 shows an adaptor for matching :into coaxial transmission lines, the adaptor including a launching probe 28 and tuning screws 29.
The waveguide can also be coupled to surface propagating microwave lines, such as strip line, microstrip line and finline. Fig. 9 shows an adaptor for matching into microstrip line 30, incorporating a matching waveguide ridge 31 and turning screws 32.
The waveguide is used to conduct electromagnetic wave energy from an electromagnetic generator. The performance of the waveguide of the invention is superior to that of flexible rectangular waveguide designed to operate at the same frequency. For example, the microwave attenuation of rectangular flexible waveguide type 'WG19 from 16 to 20 GHz is 0.9 dH/metre whereas the microwave attenuation of the equivalent waveguide of thE: invention is less than 0.4 dB/metre.
The maximum microwave power handling of the waveguide of the invention i:; also superior to standard waveguides.
For example, from 16 to 20 GHz the maximum power handling capability of rectangular flexible waveguide ~rPt~...~
d .:, ~ ' ~. . ;~~;j..~~~, a S~t~~~t'fF ~~"~~~'~
~'C~' f~~.ernatic~ai A ~ icat,op :__,:;~ ~; v~~~' ~13 MAY 1993 to type WG19 is 0.21 KW whereas the figure for the equivalent waveguide of the invention is 0.5 KW, with the waveguides filled with air at ambient temperature and pressure, and dry.
The return loss of the waveguide of the invention to elliptical transitions at each end depends upon its length and size. By way of example, a one metre length of the waveguide described above has a return loss of better than 27d13 within its operating band.
The minimum bend radius in the E plane for the waveguide of the invention is better than for other forms of elliptical waveguide. For a typical waveguide of the kind described., the minimum bend radius whilst maintaining the microwave specification is 25 mm in the E plane and 62 mm in the H plane. The minimum bend radius for other kinds of flexible elliptical waveguide is typically 150 mm in the E plane and 380 mm in the H
plane.
A further advantage of the flexible and twistable form of waveguide of the present invention is the high degree of twisting which can be achieved without degrading the performance of the waveguide beyond the permitted specification. The maximum amount of twist is typically 360o per metre. The maximum twist for other forms of flexible elliptical waveguide is typically only 6o per metre.
A given wavegu:ide of the present invention operates effectively within a relatively small frequency band, for example 15 t.o 20 GHz. However, a range of different "~3~ ~m~ ors t~aie~,t d~~a~ $U~S"p'lTt _~'C'~' ~~~ar~arlc~nai r~pplicat3pl~
P~~1~8 ~ 2 / 0 0 2 ~ ~Q
~. .# ~ ~- r( ~ ~1~3 MAY 1993 2~~~~~~J
sizes can be manufactured to cover a typical range of, but not limited to, 0.50 GHz to 50GHz.
-, ~-.: ..
'"."' ' . . F~i~a- ..Qt~..z .rlffirA
f~~~' ;z~':a~'~~t;cnal ~lpplicatEsy
ELLIPTICAL WAVEGUIDE
TECHNICAL FIELD OF THE INVENTION
This invention relates to the manufacture of flexible or flexible and twistable elliptical waveguide.
BACKGROUND
Waveguides are widely used for the transmission of electromagnetic energy in the RF, microwave and millimetric wavelength range. Such transmission can take place within the confines of the conductive wall of the waveguidE~, with a minimum of loss, reflection and distortion of the signal.
Standard waveguides are formed of extruded rigid metal tubing which is available in approximately 4.5 metre straight lengths which can then be bent or twisted to shape using specialist manufacturing equipment. Longer lengths are attained by joining shorter lengths together using atandard or custom made flanges. In microwave systems it is common for the waveguide runs to require several bends and twists to enable the waveguide to avoid various obstacles in its path. The use of standard :rigid waveguides therefore requires the production of a series of detailed manufacturing drawings to accurately define the shape of the required waveguide. This adds to the cost of the system, as does the operation of forming the waveguide into shape SUBSTITUTc SHEET
_ 2~.~~~~~ ;13 MAY 1993 and the subsequent inspection and fitting of the waveguide. Ret ro-fitting and replacement of rigid waveguides is also a potentially expensive operation, especially in more complex systems.
An important tape of waveguide is elliptical cross section waveguide. This has a lower microwave loss when operating in the a TE 11 mode than the equivalent comparable standard rectangular waveguide. Elliptical waveguide is also capable of transmitting higher microwave power than the equivalent rectangular waveguide operating in the H 10 mode. Since the wall of elliptical wavec~uide is convexly curved in all areas, the external compressive strength of such waveguide is greater than that of rectangular or double ridged waveguide desigr.~ed to operate within the same frequency range. This increased resistance to deformation is of importance in adverse mechanical or environmental conditions.
Flexible elliptical waveguide is currently manufactured in two halves, each of which is pressed to form a series of transversely extending shallow corrugations. The two halves are then axially soldered, brazed or welded to form the compleite waveguide. In general however, this form of waveguide is very stiff to bend by hand and is not, to any significant extent, twistable. In addition, such elliptical waveguide is expensive to manufacture, and can only be manufactured in certain fixed sizes for which tools are available, and in fixed lengths.
SUMMARY OF THE ~LNVENTION
ur,~;E;a ~c;: ~~~tom a~-:~--: ~tt;cg - SUBSTITUTE ~HE~T
PCT irae~vliona~ A -: ~; ;v.ian According to the present invention there is provided tubular waveguide having a wall which, when viewed in longitudinal section, is formed in a series of external ribs separated by grooves, in which said wall comprises an electrically conductive metal strip formed in a generally helical configuration with adjacent edge portions of adjacent turns of the strip mechanically interlocked by being folded over each other, and in which said interlocked edge portions are disposed on the crest of said ribs, wherein when viewed in transverse cross section said waveguide is of substantially elliptical shape without straight regions, and when viewed in longitudinal section said interlocked edge portions comprise straight regions extending substantially parallel to the longitudinal direction of the waveguide for a major part of the length of said edge portions, and the bottom of the grooves are also substantially straight extending substanti<~lly parallel to the longitudinal direction of the waveguide.
It should be understood that the term "elliptical" as used herein is intended to cover other non-circular and substantially ellip;~e-like shapes such as ovals.
An electrically conductive element is preferably interposed between t:he folded edges to reduce electromagnetic leakage. In flexible and twistable waveguide there will usually be just a non-rigid mechanical interlock between adjacent turns, but flexible and non-twistable waveguides may be manufactured by rigidly securing they adjacent turns to each other, e.g.
by soldering, brazing or welding.
3A.
There is also disclosed a method of manufacturing tubular waveguide of substantially elliptical cross section, said waveguide having a wall which, when viewed in longitudinal section, is formed in a series of ribs separated by intervening grooves, said method comprising:
- continuously winding a pre-formed electrically conductive metal strip about a rotating mandrel of PCTlsB~2ioo2so _. ~~~~~~~~ X13 MAY 1993 substantially elliptical cross section in a generally helical configuration such that adjacent edge portions of adjacent turns of the strip are interengaged, the strip being wound onto the mandrel together with a support element: for supporting the interengaged edge portions of the strip, and - performing a secondary forming operation on said edge portions, whilst said edge portions are supported by the support element on the mandrel, so that said edge portions become folded over each other and form a mechanical interlock between said adjacent turns with said interlocked edge portions extending along the crest of said ribs.
BRIEF DESCRIPTION OF THE DRAWINGS
The invention is exemplified in the accompanying drawings, in which:
Fi ure 1 is a perspective view of waveguide of the invention in the process of manufacture, FiQUre la is an end view of the waveguide of Fig. 1 whilst wound on the mandrel, Fi ure 2 is a longitudinal section through a wall portion of the waveguide, Fi ure 3 is a further longitudinal section through a wall portion of a different waveguide of the invention ,, - r w ., y -- -_. _ ..___ _- ~-_-1 ' ,.J ,J
PC~10~~2/00~~~0 ~1~~~.~~~ '13 MAY 1993 FiQUre: 4 is a side view of a joint between two lengths of waveguide of the invention, FiQUrea 5 and 6 show an adaptor connected to an end of the waveguide in perspective view and longitudinal section respectively, and FiQUrea 7 to 9 are longitudinal sections through different forms of the adaptor.
DETAILED DESCRIPTION OF THE DRAWINGS
Hy way of example, the waveguide of the present invention may be manufactured from a thin (e. g. 0.106 mm) strip of brass, metal-plated brass (e.g. plated with a 3 to 4 um layer of silver, tin, gold, nickel or palladium nickel), or other metallic or conductive material (e. g. solid silver). The strip may typically be 5.715 mm wide:.
Referring to Fi.g. 1, the strip 1 is passed through formers 2 (e.g. rollers) which form the strip into the required cross-;sectional profile at 3. The profiled strip 3 is then fed through a forming tool 4 which feeds the strip aroundl a rotating elliptical arbour (mandrel) 5 of the required major and minor dimensions (e. g. 14.71 mm by 8.29 mm) such that adjacent turns 6 of the resulting helix 7 form a mechanical interlock with each other. Hy pre;ssing against the profiled strip, the forming tool 4 performs a final forming operation on the strip 3 so that 'the f final waveguide includes a series of angular helical ribs 6 of substantially square or '''~??-! ~ ~~ra~ic~:~;~~ _~d?~-roe ~.. ",. ~
,.r- ...~".,. , , . , , ~'~7:1~p26!~
~~~3~ ~o) ~13 MAY 1993 rectangular cross section separated by intervening grooves. As thE~ waveguide is formed it is pushed along the arbour 5 in direction 12 so that a continuous length of waveguide passes off the end of the arbour 5. The cross sectional size of the waveguide can easily be changed simply by changing the size of the arbour.
Figure 2 shows a mechanical interlock 8 which can be used to form flexible and twistable waveguide. The profiled strip 3 is wound onto the arbour 5 together with a support element 9 which supports the ribs 6 to prevent their collapse and also supports the interlock 8 during final engagement. The adjacent edges of the turns are folded back upon each other by the forming tool 4 to compleae the mechanical interlock 8, which is supported by th.e element 9 during manufacture of the waveguide. The element 9 may be an aluminium wire or a nylon filament, having a diameter of 0.91 mm for example.
The mechanical :interlock 8 of Fig. 2 also incorporates an electrically conductive seaming wire 10 which is wound onto the elliptical arbour 5 together with the profiled strip 3 and is interposed between the folded-back edges of adjacent turns 6. This seaming wire 10 may for example be of 0.21 mm thick copper wire plated with tin or silver. The seaming wire 10 enhances the mechanical performance of the waveguide and reduces microwave leakage from the waveguide.
The mechanical :interlock 8 which is shown in Fig. 3 is similar to that of Fi,g. 2 but is suitable for flexible and non-twistable waveguide. A support element 9 is United K:~gdom P-~~~L-~ ~~~ce SUBSTI~TUT~ ~H~~'T' PCZ~ ~aterr;a:;~~! A~:;~.:c~~ian PCT/~~~32/00261( _ ~~~~~~~~ ~j3 MAY 1993 again included, but the seaming wire 10 is replaced by a length of solder wire 11 of e.g. 0.23 mm diameter.
After formation of the helical waveguide as described, the waveguide is heated to melt the solder 11 which is then allowed to cool so that the adjacent turns 6 become rigidly bonded l.ogether in the region of the interlock 8.
Long lengths of the waveguide can be manufactured by joining shorter lengths using a jointing flange 15 ( Fig.
4) which is soldered, brazed or welded to the adjacent ends of the two lengths of waveguide. Another method is to join a new si.rip 3 onto the end of a previous strip 3 prior to application to the mandrel, by soldering brazing or welding or by other suitable means, so that the resulting waveguide is of a substantially continuous form with less-obvious joints.
The helix 7 ma5r be covered by a protective layer of elastomer, heat-shrunk polymer, organic or metallic braid, or the hike, to provide added environmental and mechanical protection. Flexible and twistable versions can have a further covering of an electrically conductive elasitomer for example, in order to provide improved electromagnetic screening and isolation properties.
Another version of the waveguide may be manufactured so that the screening effectiveness is deliberately very low, thus formir.~g a "leaky feeder" waveguide. This can be achieved by forming the waveguide with a loose, non-rigid interlocH: between adjacent turns, and/or by omitting the seeuning wire 10.
~id.a ~;;?C~t~Gttl1 ~dr~llt ~Jf~~f~ ~.,.,".~.-.r ~-~r~y ;nterng~tiona! Apolicat~on ~~~~' ~ ~ : ~~ i ~ ~i ~~==:~T
~~3 MAY 1993 s In order to electrically connect and match the elliptical waweguide to a different microwave transmission link, e.g. a standard rectangular waveguide, a spe~~ial elliptical-to-rectangular waveguide flanged adaptor is required. This can be soldered, clamped or attached by other suitable means onto the end of the elliptical waveguide. A suitable adaptor 20 is shown in Fig s 5 and 6, and comprises a rectangular-section waveguide part 21 which terminates in a flange interface 22. The opposite end of the rectangular part 21 is joined to an elliptical section 23, the internal dimensions of which are similar to those of the elliptical wavec~uide 7. The free end of the elliptical section 23 is provided with an internal annular recess 24 to receive the elliptical waveguide, which is soldered, mechanically fixed, adhesively bonded or otherwise secured therein. An internal step 25 is formed between 'the rectangular and elliptical sections 21 and 23. A set of tuning screws 26 are inserted through the wall of the rectangular and elliptical sections, and these screws are placed one eighth of a wavelength apart: so that by screwing them in and out of the adaptor theft can be tuned to match the rectangular and elliptical sections.
Instead of the step 25 the elliptical section of the adaptor 20 can t>e tapered, as shown in Fig. 7. In each case the tuning screws can be located in both of the wider walls of t:he waveguide or omitted altogether.
The adaptors of Fig. s 5 to 7 may be of brass, copper, aluminium, stainless steel, titanium, alloy or polymer.
The inner surface oflthe recess 24 may be plated with ~,~~:fd'e~~~o~&~ ~p~~ICca'~~(7 7 ~ "-~',~ ..::~.r 3 i i ~' i !'~
~ i ~ _ _ PCTIGBs2~oo2so silver, tin or cold for example, to aid soldering to the elliptical wave~~uide.
The waveguide o:E the invention could also be interfaced to other forms of transmission line via a similar matching adaptor of suitable design, for example circular, double ridge, single ridge, and quad ridged dielectric wave;guides, or elliptical waveguide of a different size or orientation. Fig. 8 shows an adaptor for matching :into coaxial transmission lines, the adaptor including a launching probe 28 and tuning screws 29.
The waveguide can also be coupled to surface propagating microwave lines, such as strip line, microstrip line and finline. Fig. 9 shows an adaptor for matching into microstrip line 30, incorporating a matching waveguide ridge 31 and turning screws 32.
The waveguide is used to conduct electromagnetic wave energy from an electromagnetic generator. The performance of the waveguide of the invention is superior to that of flexible rectangular waveguide designed to operate at the same frequency. For example, the microwave attenuation of rectangular flexible waveguide type 'WG19 from 16 to 20 GHz is 0.9 dH/metre whereas the microwave attenuation of the equivalent waveguide of thE: invention is less than 0.4 dB/metre.
The maximum microwave power handling of the waveguide of the invention i:; also superior to standard waveguides.
For example, from 16 to 20 GHz the maximum power handling capability of rectangular flexible waveguide ~rPt~...~
d .:, ~ ' ~. . ;~~;j..~~~, a S~t~~~t'fF ~~"~~~'~
~'C~' f~~.ernatic~ai A ~ icat,op :__,:;~ ~; v~~~' ~13 MAY 1993 to type WG19 is 0.21 KW whereas the figure for the equivalent waveguide of the invention is 0.5 KW, with the waveguides filled with air at ambient temperature and pressure, and dry.
The return loss of the waveguide of the invention to elliptical transitions at each end depends upon its length and size. By way of example, a one metre length of the waveguide described above has a return loss of better than 27d13 within its operating band.
The minimum bend radius in the E plane for the waveguide of the invention is better than for other forms of elliptical waveguide. For a typical waveguide of the kind described., the minimum bend radius whilst maintaining the microwave specification is 25 mm in the E plane and 62 mm in the H plane. The minimum bend radius for other kinds of flexible elliptical waveguide is typically 150 mm in the E plane and 380 mm in the H
plane.
A further advantage of the flexible and twistable form of waveguide of the present invention is the high degree of twisting which can be achieved without degrading the performance of the waveguide beyond the permitted specification. The maximum amount of twist is typically 360o per metre. The maximum twist for other forms of flexible elliptical waveguide is typically only 6o per metre.
A given wavegu:ide of the present invention operates effectively within a relatively small frequency band, for example 15 t.o 20 GHz. However, a range of different "~3~ ~m~ ors t~aie~,t d~~a~ $U~S"p'lTt _~'C'~' ~~~ar~arlc~nai r~pplicat3pl~
P~~1~8 ~ 2 / 0 0 2 ~ ~Q
~. .# ~ ~- r( ~ ~1~3 MAY 1993 2~~~~~~J
sizes can be manufactured to cover a typical range of, but not limited to, 0.50 GHz to 50GHz.
-, ~-.: ..
'"."' ' . . F~i~a- ..Qt~..z .rlffirA
f~~~' ;z~':a~'~~t;cnal ~lpplicatEsy
Claims
1. Tubular waveguide having a wall which, when viewed in longitudinal section, is formed in a series of external ribs separated by grooves, in which said wall comprises an electrically conductive metal strip formed in a generally helical configuration with adjacent edge portions of adjacent turns of the strip mechanically interlocked by being folded over each other, and in which said interlocked edge portions are disposed on the crest of said ribs, wherein when viewed in transverse cross section said waveguide is of substantially elliptical shape without straight regions, and when viewed in longitudinal section said interlocked edge portions comprise straight regions extending substantially parallel to the longitudinal direction of the waveguide for a major part of the length of said edge portions, and the bottom of the grooves are also substantially straight extending substantially parallel to the longitudinal direction of the waveguide.
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| GB919103067A GB9103067D0 (en) | 1991-02-13 | 1991-02-13 | Elliptical waveguides |
| PCT/GB1992/000260 WO1992015125A1 (en) | 1991-02-13 | 1992-02-13 | Elliptical waveguide |
| GB9103067.6 | 1992-02-13 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2103570A1 CA2103570A1 (en) | 1992-08-14 |
| CA2103570C true CA2103570C (en) | 2002-04-30 |
Family
ID=10689986
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002103570A Expired - Fee Related CA2103570C (en) | 1991-02-13 | 1992-02-13 | Elliptical waveguide |
Country Status (9)
| Country | Link |
|---|---|
| EP (1) | EP0571449B1 (en) |
| JP (1) | JPH06505599A (en) |
| KR (1) | KR100260585B1 (en) |
| AU (1) | AU1229792A (en) |
| CA (1) | CA2103570C (en) |
| CH (1) | CH687655A5 (en) |
| DE (1) | DE69226262T2 (en) |
| GB (3) | GB9103067D0 (en) |
| WO (1) | WO1992015125A1 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6583693B2 (en) * | 2001-08-07 | 2003-06-24 | Andrew Corporation | Method of and apparatus for connecting waveguides |
| CN108682930B (en) * | 2018-04-24 | 2024-03-26 | 中天射频电缆有限公司 | Terminating waveguide transition device |
Family Cites Families (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE892003C (en) * | 1953-08-20 | Siemens iS. Halske Aktiengesellschaft, Berlin und München | Dielectric tubular cable with a flattened cross-section for the transmission of ultra-short waves | |
| US2636083A (en) * | 1950-03-04 | 1953-04-21 | Titeflex Inc | Flexible hollow pipe wave guide |
| DE1297722B (en) * | 1962-02-01 | 1969-06-19 | Kabel Metallwerke Ghh | Method and device for producing a corrugated waveguide of elliptical cross section |
| FR1329358A (en) * | 1962-07-20 | 1963-06-07 | Radiall Soc | Electromagnetic waveguides |
| US3383895A (en) * | 1965-08-11 | 1968-05-21 | Hackethal Draht & Kabelwerk Ag | Coilable waveguide |
| DE1690310A1 (en) * | 1967-10-06 | 1971-05-13 | Telefunken Patent | Antenna feed line in the form of a corrugated tube waveguide |
| FR2528240A1 (en) * | 1982-06-04 | 1983-12-09 | Thomson Csf | Semi-rigid aluminium waveguide for microwave transmission - comprises corrugated metallic strip joined by folding and crimping and has dual flanges for clamping terminating ends. |
-
1991
- 1991-02-13 GB GB919103067A patent/GB9103067D0/en active Pending
-
1992
- 1992-02-12 GB GB929202892A patent/GB9202892D0/en active Pending
- 1992-02-13 WO PCT/GB1992/000260 patent/WO1992015125A1/en active IP Right Grant
- 1992-02-13 AU AU12297/92A patent/AU1229792A/en not_active Abandoned
- 1992-02-13 CH CH03221/92A patent/CH687655A5/en not_active IP Right Cessation
- 1992-02-13 JP JP4504178A patent/JPH06505599A/en active Pending
- 1992-02-13 GB GB9316815A patent/GB2268001B/en not_active Expired - Fee Related
- 1992-02-13 DE DE69226262T patent/DE69226262T2/en not_active Expired - Fee Related
- 1992-02-13 CA CA002103570A patent/CA2103570C/en not_active Expired - Fee Related
- 1992-02-13 KR KR1019920702540A patent/KR100260585B1/en not_active IP Right Cessation
- 1992-02-13 EP EP92904543A patent/EP0571449B1/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| DE69226262T2 (en) | 1999-04-01 |
| GB9103067D0 (en) | 1991-03-27 |
| EP0571449A1 (en) | 1993-12-01 |
| JPH06505599A (en) | 1994-06-23 |
| CA2103570A1 (en) | 1992-08-14 |
| EP0571449B1 (en) | 1998-07-15 |
| CH687655A5 (en) | 1997-01-15 |
| WO1992015125A1 (en) | 1992-09-03 |
| GB9202892D0 (en) | 1992-03-25 |
| GB9316815D0 (en) | 1993-10-20 |
| AU1229792A (en) | 1992-09-15 |
| KR100260585B1 (en) | 2000-07-01 |
| DE69226262D1 (en) | 1998-08-20 |
| GB2268001A (en) | 1993-12-22 |
| GB2268001B (en) | 1995-07-05 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EEER | Examination request | ||
| MKLA | Lapsed |