阅读说明：本技术 一种同轴腔体双通带滤波器 (Coaxial cavity dual-passband filter ) 是由 高浩洋 陈健 于 2018-07-16 设计创作，主要内容包括：本发明揭示了一种同轴腔体双通带滤波器,包括一封闭式的滤波腔、若干个通带谐振器、若干个零点谐振器和加载板,其中,零点谐振器设置于加载板上,加载板和通带谐振器均设置于滤波腔内,加载板上的零点谐振器与通带谐振器位置对应设置,且位置对应的通带谐振器和零点谐振器之间形成电耦合连接。本发明可以降低滤波器的加工和组装成本,且减小滤波器的体积。(The invention discloses a coaxial cavity dual-passband filter which comprises a closed filter cavity, a plurality of passband resonators, a plurality of zero resonators and a loading plate, wherein the zero resonators are arranged on the loading plate, the loading plate and the passband resonators are arranged in the filter cavity, the zero resonators on the loading plate are arranged corresponding to the passband resonators in position, and the passband resonators and the zero resonators in corresponding positions are in electric coupling connection. The invention can reduce the processing and assembling cost of the filter and reduce the volume of the filter.)

1. A coaxial cavity dual-passband filter is characterized by comprising a cavity and a loading plate, wherein a plurality of linearly arranged passband resonators are integrally formed in the cavity, and adjacent passband resonators are coupled; the loading plate is fixed in the cavity and positioned above the passband resonators, and a plurality of zero resonators corresponding to the positions of the passband resonators in the cavity are formed on the loading plate; and the passband resonator and the zero resonator which correspond to the upper position and the lower position form electric coupling connection.

2. The coaxial cavity dual-passband filter of claim 1, wherein each of the passband resonator and the null resonator has an open end and a short end opposite to each other, and the short end of the null resonator is disposed adjacent to the open end of the corresponding passband resonator.

3. The coaxial cavity dual-passband filter of claim 2, wherein one end of the passband resonator is integrally formed with the inner wall of the cavity to form the short-circuited end thereof, and the other end is not in contact with the inner wall of the cavity to form the open-circuited end thereof; one end of the zero resonator is integrally formed with the loading plate to form the short-circuit end, and the other end of the zero resonator is not in contact with the loading plate to form the open-circuit end.

4. The coaxial cavity dual-passband filter according to claim 1 or 2, wherein a separation distance exists between the loading plate and the passband resonator, and the greater the separation distance is, the weaker the electric coupling strength between the passband resonator and the zero resonator is; the stronger the opposite.

5. The coaxial cavity dual-passband filter according to claim 1 or 2, wherein the zero resonators are isolated from each other by a metal isolation strip.

6. The coaxial cavity dual bandpass filter according to claim 1, wherein each of the zero resonators is a segment of metal strip line formed on a load plate.

7. The coaxial cavity dual bandpass filter according to claim 1, wherein the load plate is fixed in the cavity by fastening screws or welded in the cavity.

8. The coaxial cavity dual passband filter of claim 1, further comprising a metallic tuning screw extending into the resonant cavity of the passband resonators from the side of the cavity, one metallic tuning screw for each passband resonator.

9. The coaxial cavity dual bandpass filter of claim 1, wherein the filter further comprises an input port and an output port, the input port and the output port are respectively disposed on two opposite outer lateral surfaces of the cavity.

10. The dual bandpass filter of claim 1, further comprising an upper cover plate and a lower cover plate respectively covering and fixing the upper and lower end surfaces of the cavity.

Technical Field

The invention relates to a dual-passband filter, in particular to a coaxial cavity dual-passband filter.

Background

The radio frequency dual-passband filter is an indispensable key device in a radio frequency system, can effectively filter interference signals in a wireless system, reduces interference among all channels, and ensures normal communication of all frequency bands.

In recent years, a method of designing a dual bandpass filter based on frequency transformation has become a focus of research. The double-passband filter designed by the method mainly comprises a plurality of passband resonators and zero resonators, and the passband resonators are connected through an electric coupling or magnetic coupling structure to form the passband of the filter. The zero point resonators are independently connected with the corresponding passband resonators through electric coupling or magnetic coupling structures, and no coupling structure exists among the zero point resonators.

For example, the existing Chinese patent application numbers are: 200620172678.9 discloses an asymmetric dual passband cavity filter, and the existing chinese patent application No.: 200620172678.9 discloses a dual-passband SIR coaxial cavity filter, which is designed by frequency conversion.

However, the following drawbacks exist in both of the above patents: 1. the zero resonator and the passband resonator are realized by adopting coaxial cavities, so that the whole structure of the filter is not compact enough and the size is large; 2. the zero resonator and the pass-band resonator are connected through a magnetic coupling structure, so that the structure wastes space and further increases the volume of the filter; 3. the zero resonator needs to be separately processed and assembled, so that the overall processing cost of the filter is increased, and the assembly and debugging difficulty is high.

Therefore, a novel dual-passband filter is needed to solve the defects of the dual-passband filter, such as non-compact structure, large volume, high processing cost, and high difficulty in assembly and debugging.

Disclosure of Invention

The invention aims to overcome the defects of the prior art and provides a coaxial cavity dual-passband filter which is compact in structure and reduces the assembly and debugging difficulty.

In order to achieve the purpose, the invention provides the following technical scheme: a coaxial cavity dual-passband filter comprises a cavity and a loading plate, wherein a plurality of linearly arranged passband resonators are integrally formed in the cavity, and adjacent passband resonators are coupled and connected; the loading plate is fixed in the cavity and positioned above the passband resonators, and a plurality of zero resonators corresponding to the positions of the passband resonators in the cavity are formed on the loading plate; and the passband resonator and the zero resonator which correspond to the upper position and the lower position form electric coupling connection.

Preferably, each of the pass-band resonators and the zero resonator has an open end and a short end opposite to each other, and the short end of the zero resonator is disposed close to the open end of the corresponding pass-band resonator.

Preferably, one end of the passband resonator is integrally formed with the inner wall of the cavity to form the short-circuit end thereof, and the other end of the passband resonator is not in contact with the inner wall of the cavity to form the open-circuit end thereof; one end of the zero resonator is integrally formed with the loading plate to form the short-circuit end, and the other end of the zero resonator is not in contact with the loading plate to form the open-circuit end.

Preferably, a separation distance exists between the loading plate and the pass-band resonator, and the greater the separation distance is, the weaker the electric coupling strength between the pass-band resonator and the zero-point resonator is; the stronger the opposite.

Preferably, the zero resonators are isolated from each other by metal isolation strips.

Preferably, each zero resonator is a section of metal strip line formed on the loading plate.

Preferably, the loading plate is fixed in the cavity by fastening screws or is fixed in the cavity by welding.

Preferably, the filter further comprises a metal tuning screw, the metal tuning screw extends into the resonant cavity of the pass-band resonator from the side surface of the cavity, and each pass-band resonator corresponds to one metal tuning screw.

Preferably, the filter further includes an input port and an output port, and the input port and the output port are respectively disposed on two opposite outer side surfaces of the cavity.

Preferably, the filter further comprises an upper cover plate and a lower cover plate which are respectively fixed on the upper end surface and the lower end surface of the cavity in a covering manner.

The invention has the beneficial effects that:

1. a plurality of zero resonators are manufactured into a whole through a loading plate, the whole processing time of the filter can be greatly reduced, the procedures are simplified, the cost is saved, and the whole assembly and debugging difficulty of the filter is reduced.

2. The zero resonator and the pass-band resonator are connected through the electric coupling structure, so that the distance between the zero resonator and the pass-band resonator can be greatly reduced, and the simple and reliable filter structure is realized.

3. The loading plate is directly assembled in the passband resonator, so that the filter structure is more compact, and the size of the filter is greatly reduced.

Drawings

FIG. 1 is a schematic illustration of an explosive structure according to the present invention;

FIG. 2 is a schematic cross-sectional view of the resonator-mounted cavity of the present invention;

FIG. 3 is a schematic top view of the chamber of the present invention;

FIG. 4 is a schematic view of the present invention load plate screw secured in the cavity;

FIG. 5 is a schematic view of another alternative embodiment of the present invention with a load plate welded into the cavity;

fig. 6 is a schematic diagram of the frequency response curve of the dual bandpass filter of the present invention.

Reference numerals:

1. the device comprises a passband resonator, 2, a zero resonator, 3, a loading plate, 4, a cavity, 5, an upper cover plate, 6, a lower cover plate, 7, a fastening screw, 8, an input port, 9, an output port, 10, a metal adjusting screw, 11, a resonant cavity, 12, a metal isolation strip, 13, a mounting boss, 14 and a second mounting hole.

Detailed Description

The technical solution of the embodiment of the present invention will be clearly and completely described below with reference to the accompanying drawings of the present invention.

As shown in fig. 1, the coaxial cavity dual-passband filter disclosed by the present invention has an overall structure disposed in a closed metal cavity, and the filter includes a closed filter cavity, a plurality of passband resonators 1, a plurality of zero resonators 2, and a loading plate 3, wherein the zero resonator 2 is disposed on the loading plate 3, the loading plate 3 and the passband resonators 1 are both disposed in the filter cavity, the zero resonator 2 on the loading plate 3 is disposed corresponding to the passband resonators 1, and the corresponding passband resonators 1 and zero resonators 2 are electrically coupled.

Specifically, in this embodiment, as shown in fig. 1, the filter cavity includes a cavity 4, an upper cover plate 5 and a lower cover plate 6, wherein the upper cover plate 5 and the lower cover plate 6 are respectively fixed on the upper and lower end surfaces of the cavity 4 in a covering manner, so that the filter cavity is integrally formed into a sealed cavity. In practice, the upper cover plate 5 and the lower cover plate 6 can be fixed with the corresponding end surfaces of the cavity 4 through fastening screws 7, and the filter cavity can be a metal cavity.

As shown in fig. 1 to 5, two opposite outer side surfaces of the cavity 4 are respectively provided with a signal port 8, 9 for signal access. In this embodiment, an input port 8 and an output port 9 are respectively disposed on the left and right opposite side surfaces of the cavity 4, both the two ports 8 and 9 are communicated with the cavity 4, that is, a signal enters the cavity 4 for filtering after being input from the input port 8, and the filtered signal is output through the output port 8 to complete filtering.

As shown in fig. 1 and 3, the passband resonator 1 is directly machined into the cavity 4, integrally formed with the cavity 4 to form a whole, and cooperates with the cavity 4 to form the passband of the filter. Specifically, in the present embodiment, the direction of the passband resonator 1 in the cavity is perpendicular to the direction of the two signal ports 8 and 9, that is, in the present embodiment, a single passband resonator 1 is longitudinally disposed in the cavity 4, and a plurality of passband resonators 1 are linearly arranged in the cavity 4 in the transverse direction (i.e., in the direction perpendicular to the direction of the single passband resonator 1).

One end of each passband resonator 1 (the bottom end of the passband resonator 1 in this embodiment) is integrally formed with the inner wall of the cavity (in this embodiment, the inner wall of the cavity, i.e., the inner wall of the front side of the cavity), to form a short-circuited end thereof; the other end (the top end of the passband resonator 1 in this embodiment) is not in contact with the inner wall of the cavity (i.e., has a certain space), and forms an open end. In the pass-band resonator 1, the open end is a region where the electric field is strongest, and the short end is a region where the magnetic field is strongest.

In addition, as shown in fig. 3, two adjacent pass-band resonators 1 are coupled to each other, and may be electrically coupled to each other, magnetically coupled to each other, or electromagnetically mixed.

Preferably, as shown in fig. 2, the dual-passband filter of the present invention further includes a plurality of tuning metal screws 10, and the tuning metal screws 10 extend into the passband resonator 1 to adjust the resonant frequency thereof. Specifically, in this embodiment, a resonant cavity 11 is formed in each passband resonator 1, the metal tuning screw 10 penetrates through the outer side surface of the cavity and extends into the resonant cavity 11, and each metal tuning screw 10 corresponds to one passband resonator 1.

As shown in fig. 1, 2, 4, and 5, the plurality of zero resonators 2 are integrally formed on the load plate 3 and are machined to form a whole. The loading plate 3 is fixed in the cavity 4 and located above the passband resonator 1, and after the loading plate 3 is installed in the cavity 4, the position of the zero point resonator 2 on the loading plate corresponds to the position of the passband resonator 1 in the cavity 4. Specifically, in the present embodiment, the zero point resonators 2 are also linearly arranged in the lateral direction on the loading plate 3, and each zero point resonator 2 corresponds to the upper and lower positions of the pass-band resonator 1 located therebelow.

Similarly, one end of each zero resonator 2 (the bottom end of the zero resonator 2 in this embodiment) is integrally formed with the load plate 3 to form a short-circuited end thereof; the other end (the top end of the zero resonator 2 in this embodiment) is not in contact with (i.e., has a certain interval from) the load plate 3, and forms an open end thereof. In the zero resonator 2, the open end is also the region where the electric field is strongest, and the short end is the region where the magnetic field is strongest.

The loading plate 3 is installed directionally, in this embodiment, the short-circuit end (i.e., the place where the magnetic field is strongest) of the zero-point resonator 2 is arranged close to the open-circuit end (i.e., the place where the electric field is strongest) of the corresponding pass-band resonator 1, so that the two are electrically coupled; on the contrary, the open end (i.e., where the electric field is strongest) of the zero-point resonator 2 is located close to the short end (i.e., where the magnetic field is strongest) of the corresponding pass-band resonator 1. Note that the electric coupling exists only between the passband resonator 1 and the zero point resonator 2 corresponding to the two positions, and the electric coupling does not exist between the passband resonator 1 and the zero point resonator 2 not corresponding to the two positions.

In addition, there is no energy coupling between two adjacent zero point resonators 2, and as shown in fig. 1, 2, 4, and 5, in the present embodiment, two adjacent zero point resonators 2 are spaced apart from each other by a metal isolation strip 12. In addition, the main body of the zero resonator 2 in this embodiment is a section of metal strip line, and the total length of the strip line determines the resonant frequency of the zero resonator 2.

When the device is installed, as shown in fig. 4 and 5, the loading plate 3 may be fixed in the cavity 4 by a screw fastening structure, or may be fixed in the cavity 4 by a welding fixing structure. Specifically, as shown in fig. 4, when the loading plate 3 is fixed by a screw fastening structure, the outer edge of the loading plate 3 is provided with a first mounting hole (not shown), the inner wall of the cavity 4 above the passband resonator 1 is provided with a mounting boss 13, the mounting boss 13 is provided with a second mounting hole 14 corresponding to the position of the first mounting hole 13 on the loading plate 3, and the loading plate 3 can be fixed in the metal cavity 4 by fastening a screw 7 through the first mounting hole 13 and the second mounting hole 14. When the loading plate is fixed by a welding fixing structure, the loading plate 3 and the inner wall of the cavity 4 can be directly welded together as shown in fig. 5.

In addition, a certain spacing distance exists between the loading plate 3 and the pass-band resonator 1, wherein the greater the spacing distance is, the weaker the electric coupling strength between the pass-band resonator 1 and the zero-point resonator 2 is; otherwise, the stronger.

The frequency response curve of the double-passband filter of the embodiment of the invention is shown in fig. 6, and transmission zeros between two passband resonators 1 are realized by the zero resonator 2 on the loading plate 3.

In addition, the shapes of the pass-band resonator 1 and the zero-point resonator 2 of the present invention are not limited to those shown in the drawings, and may be changed accordingly according to actual needs.

Therefore, the scope of the present invention should not be limited to the disclosure of the embodiments, but includes various alternatives and modifications without departing from the scope of the present invention, which is defined by the claims of the present patent application.