This application is a 35 U.S.C. §371 National Phase Entry Application from PCT/EP2010/055609, filed Apr. 27, 2010, designating the United States, the disclosure of which is incorporated herein in its entirety by reference.
The present invention relates to a waveguide E-plane filter component comprising a first main part and a second main part, each part in turn comprising a corresponding first and second waveguide section part. The main parts are arranged to be mounted to each other, each waveguide section part comprising a bottom wall, corresponding side walls and an open side. The open side of the first waveguide section part is arranged to face the open side of the second waveguide section part. The waveguide E-plane filter component further comprises at least one electrically conducting foil that is arranged to be placed between the first main part and the second main part when the main parts are mounted to each other, said foil comprising a filter part that is arranged to run between the waveguide section parts, the filter part comprising apertures in the foil.
When designing microwave circuits, transmission lines and waveguides are commonly used. A transmission line is normally formed on a dielectric carrier material. Due to losses in the dielectric carrier material, it is sometimes not possible to use any transmission lines. When there for example is a filter component in the layout, it may have to be realized in waveguide technology. Waveguides are normally filled with air or other low-loss materials.
Despite quite impressive progress demonstrated in the last few decades in the microwave engineering area, the important role of waveguide components remains undisputed, this is due to their low loss and high power capability performance.
A waveguide E-plane filter component normally comprises two main parts, a first main part comprising a first waveguide section part and a second main part comprising a second waveguide section part. Each waveguide section part comprises three walls; a bottom and corresponding sides.
The first main part and the second main part are arranged to be mounted together such that the first waveguide section part and the second waveguide section part face each other, and together constitute a resulting waveguide section part. This means that each main part comprises a half-height waveguide section part where, when mounted together, the resulting waveguide section part constitutes a full-height waveguide section part.
The electromagnetic field propagates parallel to the intersection. Since the waveguide section part normally have equal sizes, and thus the same height of the corresponding sides, the dominant TE10 mode of the electromagnetic field has its maximum magnitude at said intersection.
Between the main parts, at the intersection, an electrically conducting foil is placed, having a filter part comprising full height or partial-height apertures. The filter part runs between the waveguide section parts.
In order to improve the spectral selectivity and stop-band attenuation, a class of filters for which an amplitude transfer function has attenuation poles at finite frequencies is used. The transmission zeros, attenuation poles, at finite frequencies can be introduced by cross-coupling resonant cavities. Since this solution is not always realizable, the transmission zeroes at the finite frequencies can by introduced using band-stop resonators. Each band-stop resonator allows one to realize one transmission zero either below or above the pass-band of the filter. An E-plane band-stop resonator is usually realized in the form of a T-junction with one port being short-circuited. Such a T-junction is comprised in the main parts with the conductive foil disposed in between the main parts, realizing the coupling between the band-stop cavity and the rest of the E-plane filter.
These T-junctions constitute so-called extracted cavities, allowing realization of said transmission zeroes. These extracted cavities are constituted by relatively small confined openings.
Generally, the benefit of an E-plane filter is that the same main parts can be used for the filters working at different center frequencies and/or covering different bandwidths at different frequency bands. This may be achieved by using the same main parts and change the electrically conducting foil to one having the aperture configuration that provides the desired frequency characteristics.
However, when a waveguide filter design based on E-plane technology is concerned, the relative positions of extracted cavities in the form of said T-junction need to be fixed. The distance between a common port of the waveguide filter and an extracted cavity thus needs to be fixed for a given frequency characteristic of the waveguide filter. This limits the possibility of having the same main parts and replacing the conductive foil disposed between the main parts to realize different filter characteristic.
There is thus a desire to obtain a microwave waveguide E-plane filter structure, where the structure may be used for different center frequencies and/or frequency bands by only changing the electrically conducting foil according to the above.
The object of the present invention is to present a microwave waveguide E-plane filter structure, where the structure may be used for different center frequencies and/or frequency bands by only changing an electrically conducting foil.
This object is obtained by means of a waveguide E-plane filter component comprising a first main part and a second main part, each part in turn comprising a corresponding first and second waveguide section part. The main parts are arranged to be mounted to each other, each waveguide section part comprising a bottom wall, corresponding side walls and an open side. The open side of the first waveguide section part is arranged to face the open side of the second waveguide section part. The waveguide E-plane filter component further comprises at least one electrically conducting foil that is arranged to be placed between the first main part and the second main part when the main parts are mounted to each other, said foil comprising a filter part that is arranged to run between the waveguide section parts, the filter part comprising apertures in the foil. The filter part at least partly comprises at least one foil loop constituted by a foil conductor having a starting point and an end point, said foil conductor at least partly running in a corresponding further aperture in said foil, dividing said corresponding aperture in a first part and a second part.
According to an example, the first part is U-shaped and the second part is positioned at least partly inside the U-shape, where the second part may have a round shape.
According to another example, the waveguide section parts have corresponding at least two branches, where each branch comprises a foil.
Other examples are evident from the dependent claims.
A number of advantages are obtained by means of the present invention, for example
The present invention will now be described more in detail with reference to the appended drawings, where:
With reference to
As shown in
With reference to
The waveguide section part 3 further comprises a first branch 16 and a second branch 17, these branches 16, 17 being combined to a third branch 18. Corresponding branches constitute the second waveguide section part 5, a corresponding third branch 19 is shown in
With reference to
With reference also to
When the first main part 2 and the second main part 4 are mounted, as shown in
According to the present invention, with reference to
By means of the foil loop 13, there is no need for “extracted cavities” in the diplexer, which means that the same main parts 2, 4 may be used for different frequency bands, and where only the electrically conducting foils 10, 11 will have to be changed for the desired frequency band, and where the electrically conducting foils 10, 11 thus are electrically matched for a certain frequency band.
The foil loop 13 shown in
The further aperture 15a, 15b may have many different forms, one example is illustrated in
The present invention is not limited to the examples above, but may vary freely within the scope of the appended claims. For example, the diplexer shown is only on example of a waveguide E-plane filter component that is suitable for the present invention. Other types are easily conceivable for the skilled person, and may for example be single filters, having only one branch or triplexers.
Each electrically conducting foil 10, 11 may have any number and shape of apertures 12a, 12b, 12c, and more than one of the further apertures 15a, 15b comprising the foil loop according to the present invention.
The conducting foil 10, 11 may be made in any suitable material such as copper, gold or aluminium.
The main parts 2, 4 may be made in any suitable material such as aluminium or plastics covered with an electrically conducting layer.
Of course the present invention may not only be used for changing frequencies for an E-plane waveguide filter in an easy and cost-effective manner, but many other filter characteristics may also be changed by means of the present invention, such as the number of poles.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2010/055609 | 4/27/2010 | WO | 00 | 10/26/2012 |
Publishing Document | Publishing Date | Country | Kind |
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WO2011/134497 | 11/3/2011 | WO | A |
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Number | Date | Country |
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0274859 | Jul 1988 | EP |
03065496 | Aug 2003 | WO |
Entry |
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Young et al. “Integrated E-Plane Fitters with Finite Frequency Transmission Zeros” Microwave Conference, 1994, 24th European, IEEE, Sep. 5, 1994, XP031604994, pp. 460-465. |
Number | Date | Country | |
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20130038407 A1 | Feb 2013 | US |