CN114256576B - D-band Tesla node coupling structure - Google Patents
D-band Tesla node coupling structure Download PDFInfo
- Publication number
- CN114256576B CN114256576B CN202111527391.9A CN202111527391A CN114256576B CN 114256576 B CN114256576 B CN 114256576B CN 202111527391 A CN202111527391 A CN 202111527391A CN 114256576 B CN114256576 B CN 114256576B
- Authority
- CN
- China
- Prior art keywords
- tesla
- arc
- conduction band
- metal conduction
- band
- 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.)
- Active
Links
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P5/00—Coupling devices of the waveguide type
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/201—Filters for transverse electromagnetic waves
- H01P1/203—Strip line filters
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P1/00—Auxiliary devices
- H01P1/20—Frequency-selective devices, e.g. filters
- H01P1/207—Hollow waveguide filters
-
- 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
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
本发明涉及微波技术,具体为一种D波段特斯拉结耦合结构。本发明仅采用一个带状线腔体结构,通过传统带状线与特斯拉结结合的方式,利用这种结构的特殊性即电磁波达到特斯拉结两个结点的相位差不同,通过带线中心导带结构的变化来实现带阻的滤波效果,具有体积小的优势。当三个结间距不同,即结之间的耦合不同,所呈现的滤波效果不同。为解决现有耦合结构体积相对较大不利于集成的问题提供了一种新的途径。
The invention relates to microwave technology, in particular to a D-band Tesla junction coupling structure. The present invention only adopts one stripline cavity structure, and by combining the traditional stripline with the Tesla junction, the speciality of this structure is used, that is, the phase difference between the two nodes of the electromagnetic wave reaching the Tesla junction is different, and the The change of the central conduction band structure of the strip line can achieve the filtering effect of the band rejection, which has the advantage of small size. When the distance between the three junctions is different, that is, the coupling between the junctions is different, the filtering effect presented is different. It provides a new way to solve the problem that the existing coupling structure is relatively large and unfavorable for integration.
Description
技术领域technical field
本发明涉及微波技术,具体为一种D波段特斯拉结耦合结构。The invention relates to microwave technology, in particular to a D-band Tesla junction coupling structure.
背景技术Background technique
D波段为:110-170GHz,位于太赫兹频段。带状线作为微波传输线,广泛应用于滤波器的设计中。传统的带线结构的滤波效果是通过腔体与腔体之间的耦合,或中心导带间的耦合实现的,因而其整体体积相对较大,不利于当前行业集成化的小体积需求。The D-band is: 110-170GHz, located in the terahertz band. Striplines are widely used in the design of filters as microwave transmission lines. The filtering effect of the traditional stripline structure is achieved by the coupling between the cavity and the cavity, or the coupling between the central conduction bands, so the overall volume is relatively large, which is not conducive to the small volume requirements of the current industry integration.
发明内容SUMMARY OF THE INVENTION
针对上述存在问题或不足,为解决现有耦合结构体积相对较大不利于集成的问题,本发明提供了一种D波段特斯拉结耦合结构,为带状线耦合结构。In view of the above-mentioned problems or deficiencies, in order to solve the problem that the existing coupling structure is relatively bulky and unfavorable for integration, the present invention provides a D-band Tesla junction coupling structure, which is a stripline coupling structure.
本发明的技术方案如下:The technical scheme of the present invention is as follows:
一种D波段特斯拉结耦合结构,包括:高介电常数的介质基板(9-14)、金属导带和特斯拉结。A D-band Tesla junction coupling structure comprises: a high dielectric constant dielectric substrate (9-14), a metal conduction band and a Tesla junction.
所述介质基板的介电常数为9-14。The dielectric constant of the dielectric substrate is 9-14.
所述金属导带(铜)设置于沿介质基板中电磁波传播方向的中心位置;The metal conduction band (copper) is arranged at the center position along the propagation direction of the electromagnetic wave in the dielectric substrate;
所述特斯拉结有三个,三个特斯拉结相同,且位于金属导带的同一侧并与金属导带相连接,特斯拉结的材质与金属导带相同;三个特斯拉的位置关系为:1号结位于金属导带正中,以1号结为基准,沿着金属导带长度方向分别前后移动相同距离d3得到2号与3号结,d3=0.7~0.96mm。There are three Tesla junctions. The three Tesla junctions are the same and are located on the same side of the metal conduction band and are connected to the metal conduction band. The material of the Tesla junction is the same as that of the metal conduction band; The positional relationship is as follows: No. 1 knot is located in the middle of the metal conduction band, with No. 1 knot as the benchmark, move the same distance d3 back and forth along the length of the metal conduction strip to obtain No. 2 and No. 3 knots, d3 = 0.7 ~ 0.96mm.
特斯拉结内外侧均由勒洛三角形的一条弧线边和一条半圆弧衔接构成;勒洛三角形的弧线边一端接金属导带的一侧边,另一端接半圆弧的一端,半圆弧的另一端接金属导带侧边,勒洛三角形的弧线边和半圆弧所接的金属导带侧边为相同侧,以此构成特斯拉结内外侧弧线;特斯拉结内弧线和外弧线的所属勒洛三角形的中心点相重合,且与所在金属导带侧边的中点重合。所述特斯拉结的内外侧弧线中,勒洛三角形对应的正三角形边长的一半为相应半圆弧的直径。特斯拉结外侧弧线对应的正三角形垂线的一半为L1,内侧弧线对应的正三角形垂线的一半为L2,L1=0.28~0.3mm,L2=0.19~0.22mm。The inner and outer sides of the Tesla knot are formed by connecting an arc edge and a semi-circular arc of the Leroy triangle; one end of the arc edge of the Leroy triangle is connected to one side of the metal conduction band, and the other end is connected to one end of the semi-circular arc. The other end of the semicircular arc is connected to the side of the metal conduction band, and the arc edge of the Leroy triangle and the side of the metal conduction band connected to the semicircular arc are the same side, thus forming the inner and outer arcs of the Tesla junction; The center points of the Leroy triangles of the inner arc and the outer arc of the tie-knot coincide with the center points of the sides of the metal conduction band where they are located. In the inner and outer arcs of the Tesla knot, half of the side length of the equilateral triangle corresponding to the Leroy's triangle is the diameter of the corresponding semicircular arc. The half of the equilateral triangle vertical line corresponding to the outer arc of the Tesla knot is L1, and the half of the equilateral triangle vertical line corresponding to the inner arc is L2, L1=0.28~0.3mm, L2=0.19~0.22mm.
上述D波段特斯拉结耦合结构的设计方法,包括以下步骤:The design method of the above-mentioned D-band Tesla junction coupling structure includes the following steps:
步骤1、设计一个适合D波段传输的传统带状线结构,包括介质基板的介电常数ε、宽度w1、厚度t1、中心金属导带的宽度w,厚度t。
步骤2、在步骤1设计的带状线结构中构建1号特斯拉结。
首先,以金属导带一侧边的中点为正三角形的中心点,构建特斯拉结的外侧弧线,包括与该正三角形边长相应的勒洛三角形一条弧线边和半圆弧,勒洛三角形的弧线边一端接金属导带的一侧边,另一端接半圆弧的一端,半圆弧的另一端接金属导带侧边,勒洛三角形的弧线边和半圆弧所接的金属导带侧边为相同侧;并确保特斯拉结内外弧线的所属勒洛三角形的中心点相重合,且与所在金属导带侧边的中点重合;特斯拉结外侧弧线对应的正三角形垂线的一半为L1,L1=0.28~0.3mm。First, taking the midpoint of one side of the metal conduction band as the center point of the equilateral triangle, construct the outer arc of the Tesla knot, including an arc side and a semicircle of the Leroy triangle corresponding to the side length of the equilateral triangle, One end of the arc edge of the Leroy triangle is connected to one side of the metal conduction band, the other end is connected to one end of the semicircular arc, and the other end of the semicircular arc is connected to the side edge of the metal conduction band. The sides of the connected metal conduction band are the same side; and ensure that the center points of the Leroy triangle of the inner and outer arcs of the Tesla junction coincide, and the midpoint of the side of the metal conduction band where they are located; the outer side of the Tesla junction The half of the equilateral triangle vertical line corresponding to the arc is L1, and L1=0.28~0.3mm.
然后,通过缩小外弧线所属正三角形的边长,获得特斯拉结内侧弧线的勒洛三角形弧线边和半圆弧尺寸,从而确定1号特斯拉结的尺寸;特斯拉结内侧弧线对应的正三角形垂线的一半为L2,L2=0.19~0.22mm。Then, by reducing the side length of the equilateral triangle to which the outer arc belongs, the dimensions of the Leroy triangle arc side and semicircle arc of the inner arc of the Tesla knot are obtained, so as to determine the size of the No. 1 Tesla knot; The half of the equilateral triangle vertical line corresponding to the inner arc is L2, and L2=0.19~0.22mm.
步骤3、以1号特斯拉结为基准,沿着金属导带长度方向分别前后移动相同距离d3得到2号与3号结,d3=0.7~0.96mm。Step 3. Taking the No. 1 Tesla knot as the benchmark, move the same distance d3 back and forth along the length of the metal conduction band to obtain the No. 2 and No. 3 knots, d3=0.7~0.96mm.
步骤4、调整L1、L2和/或d3优化整体参数性能,并确保整个耦合结构呈现带阻效果。Step 4. Adjust L1, L2 and/or d3 to optimize the overall parameter performance and ensure that the entire coupling structure exhibits a band-stop effect.
综上所述,本发明仅采用一个带状线腔体结构,通过传统带状线与特斯拉结结合的方式,利用这种结构的特殊性即电磁波达到特斯拉结两个结点的相位差不同,通过带线中心导带结构的变化来实现带阻的滤波效果,具有体积小的优势。当三个结间距不同,即结之间的耦合不同,所呈现的滤波效果不同。为解决现有耦合结构体积相对较大不利于集成的问题提供了一种新的途径。To sum up, the present invention only adopts a stripline cavity structure, and through the combination of traditional stripline and Tesla junction, the particularity of this structure is used, that is, electromagnetic waves reach the two nodes of Tesla junction. The phase difference is different, and the band-stop filtering effect is achieved through the change of the central conduction band structure of the strip line, which has the advantage of small size. When the distance between the three junctions is different, that is, the coupling between the junctions is different, the filtering effect presented is different. It provides a new way to solve the problem that the existing coupling structure is relatively large and unfavorable for integration.
附图说明Description of drawings
图1是本发明D波段特斯拉结耦合结构的立体结构示意图;Fig. 1 is the three-dimensional structure schematic diagram of D-band Tesla junction coupling structure of the present invention;
图2是本发明D波段特斯拉结耦合结构的局部参数示意图;Fig. 2 is the local parameter schematic diagram of the D-band Tesla junction coupling structure of the present invention;
图3是实施例D波段特斯拉结耦合结构的带阻效果所对应的s参数图;3 is an s-parameter diagram corresponding to the band-stop effect of the D-band Tesla junction coupling structure of the embodiment;
图4是实施例D波段特斯拉结耦合结构的d3为0.7mm所对应的s参数图;4 is a s-parameter diagram corresponding to d3 of the D-band Tesla junction coupling structure of the embodiment being 0.7 mm;
图5是实施例D波段特斯拉结耦合结构的d3为0.82mm所对应的s参数图;5 is a s-parameter diagram corresponding to d3 of the D-band Tesla junction coupling structure of the embodiment being 0.82 mm;
图6是实施例D波段特斯拉结耦合结构的d3为0.92mm所对应的s参数图。FIG. 6 is an s-parameter diagram corresponding to the d3 of the D-band Tesla junction coupling structure of the embodiment being 0.92 mm.
具体实施方式Detailed ways
下面结合附图和实施例对本发明做进一步的详细说明。The present invention will be further described in detail below with reference to the accompanying drawings and embodiments.
一种D波段特斯拉结耦合结构的设计,包括以下步骤:A design of a D-band Tesla junction coupling structure includes the following steps:
步骤1、设计一个适合D波段传输的传统带状线结构。包括介质基板的介电常数ε、宽度w1、厚度t1、中心金属导带的宽度w,厚度t。最终确定介质基板的介电常数ε=10、宽度w1=1.6mm、厚度t1=0.25mm、中心金属导带的宽度w=0.1mm,厚度t=0.03mm。由于带线的宽度限制了特斯拉结环的大小,因此根据数学知识,初步确定带线长度L=3mm。
步骤2、在步骤1设计的带状线中增加1号特斯拉结。
具体以金属导带上侧边的中心点为正三角形的中心点,为了方便建模,以该正三角形的垂直线的一半为变量L1,垂直线沿着电磁波传播方向位于金属导带上侧边,从而确定1号特斯拉结外弧线的大小,包括与该正三角形边长相应的勒洛三角形一条弧线边和半圆弧,勒洛三角形的弧线边一端接金属导带的一侧边,另一端接半圆弧的一端,半圆弧的另一端接金属导带侧边,勒洛三角形的弧线边和半圆弧所接的金属导带侧边为相同侧。并确保特斯拉结内外弧线的所属勒洛三角形的中心点相重合,且与所在金属导带侧边的中点重合。L1=0.28~0.3mm,外弧线中半圆弧的直径d1为该正三角形边长的一半。Specifically, the center point of the upper side of the metal conduction band is the center point of the equilateral triangle. For the convenience of modeling, the half of the vertical line of the equilateral triangle is used as the variable L1, and the vertical line is located on the upper side of the metal conduction band along the electromagnetic wave propagation direction. , so as to determine the size of the arc outside the No. 1 Tesla node, including an arc side and a semicircular arc of the Leroy triangle corresponding to the side length of the equilateral triangle, and one end of the arc side of the Leroy triangle is connected to a The side, the other end is connected to one end of the semi-circular arc, the other end of the semi-circular arc is connected to the side of the metal conduction band, and the arc edge of the Leroy triangle and the side of the metal conduction band connected to the semi-circle arc are the same side. And ensure that the center points of the Leroy triangle belonging to the inner and outer arcs of the Tesla knot coincide, and the center points of the sides of the metal conduction band where it is located. L1=0.28~0.3mm, the diameter d1 of the semicircular arc in the outer arc is half of the side length of the equilateral triangle.
然后,通过改变L1,获得1号特斯拉结内侧弧线的勒洛三角形弧线边和半圆弧尺寸,从而形成1号特斯拉结。设1号特斯拉结内侧弧线所属正三角形的垂直线一半为L2,L2=0.19~0.22mm,相应半圆的直径为d2。Then, by changing L1, the arc sides of the Leroy triangle and the semicircular arc dimensions of the inner arc of Tesla
步骤3、以1号特斯拉结为基准,沿着金属导带长度方向分别前后移动相同距离d3得到2号与3号特斯拉结,d3=0.7~0.96mm。Step 3. Taking the No. 1 Tesla knot as the benchmark, move the same distance d3 back and forth along the length of the metal conduction band to obtain the No. 2 and No. 3 Tesla knots, d3=0.7~0.96mm.
步骤4、调整L1、L2和/或d3优化整体参数性能,并确保整个耦合结构呈现带阻效果。最终确定L1=0.28mm,L2=0.2mm,d3=0.7~0.96mm时,耦合结构呈现带阻效果,如附图3所示。Step 4. Adjust L1, L2 and/or d3 to optimize the overall parameter performance and ensure that the entire coupling structure exhibits a band-stop effect. When it is finally determined that L1=0.28mm, L2=0.2mm, and d3=0.7-0.96mm, the coupling structure exhibits a band resistance effect, as shown in FIG. 3 .
图4、5、6为L1=0.28mm,L2=0.2mm时,d3分别为0.7mm、0.82mm和0.92mm时的S参数图。Figures 4, 5, and 6 are S-parameter diagrams when L1=0.28mm, L2=0.2mm, and d3 is 0.7mm, 0.82mm, and 0.92mm, respectively.
通过上述实施例可见,本发明通过传统带状线与特斯拉结结合的方式,利用这种结构的特殊性即电磁波达到特斯拉结两个结点的相位差不同,实现带阻的滤波效果。当三个结间距不同,即结之间的耦合不同,所呈现的滤波效果不同。为解决现有耦合结构体积相对较大不利于集成的问题提供了一种新的途径。It can be seen from the above-mentioned embodiments that the present invention realizes band-stop filtering by combining the traditional strip line with the Tesla junction, utilizing the particularity of this structure, that is, the electromagnetic waves have different phase differences between the two nodes of the Tesla junction. Effect. When the distance between the three junctions is different, that is, the coupling between the junctions is different, the filtering effect presented is different. It provides a new way to solve the problem that the existing coupling structure is relatively large and unfavorable for integration.
Claims (2)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202111527391.9A CN114256576B (en) | 2021-12-14 | 2021-12-14 | D-band Tesla node coupling structure |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202111527391.9A CN114256576B (en) | 2021-12-14 | 2021-12-14 | D-band Tesla node coupling structure |
Publications (2)
Publication Number | Publication Date |
---|---|
CN114256576A CN114256576A (en) | 2022-03-29 |
CN114256576B true CN114256576B (en) | 2022-07-29 |
Family
ID=80795073
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202111527391.9A Active CN114256576B (en) | 2021-12-14 | 2021-12-14 | D-band Tesla node coupling structure |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN114256576B (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN116315548B (en) * | 2023-04-12 | 2024-03-26 | 电子科技大学 | An X-band Oralero knot circulator |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1119351A (en) * | 1993-12-27 | 1996-03-27 | 松下电器产业株式会社 | Resonator and high-frequency circuit element using the same |
WO2013147152A1 (en) * | 2012-03-29 | 2013-10-03 | 国立大学法人電気通信大学 | Transmission line resonator, band-pass filter employing transfer line resonator, splitter, synthesizer, band elimination filter, high-pass filter, balance filter, and low-pass filter |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3762976B2 (en) * | 2003-05-22 | 2006-04-05 | 財団法人理工学振興会 | Ring filter and broadband bandpass filter using the same |
JP4250718B2 (en) * | 2004-04-30 | 2009-04-08 | 富士通コンポーネント株式会社 | Filter device and circuit module |
-
2021
- 2021-12-14 CN CN202111527391.9A patent/CN114256576B/en active Active
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN1119351A (en) * | 1993-12-27 | 1996-03-27 | 松下电器产业株式会社 | Resonator and high-frequency circuit element using the same |
WO2013147152A1 (en) * | 2012-03-29 | 2013-10-03 | 国立大学法人電気通信大学 | Transmission line resonator, band-pass filter employing transfer line resonator, splitter, synthesizer, band elimination filter, high-pass filter, balance filter, and low-pass filter |
Also Published As
Publication number | Publication date |
---|---|
CN114256576A (en) | 2022-03-29 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN203760599U (en) | Compact type ultra wide band double-band-notch balance band-pass filter | |
CN103094646B (en) | Substrate integration waveguide load dielectric resonator filter | |
CN103915665B (en) | The balancing band bandpass filter that a kind of compact ultra broadband biobelt falls into | |
CN108172958A (en) | A Periodic Slow Wave Transmission Line Unit Based on Coplanar Waveguide | |
CN114256576B (en) | D-band Tesla node coupling structure | |
CN104993205A (en) | Microstrip fold line directional coupler | |
CN105990630A (en) | High-selectivity Balun band pass filter based on substrate integrated waveguide | |
CN102290627A (en) | Broadband low-loss passive balun on chip having laminated winding structure | |
CN104659451B (en) | The four modular belt bandpass filters based on 1/3 equilateral triangle substrate integrated resonator | |
CN103367843A (en) | Four-model resonator-based compact dual-passband high-temperature superconductive filter | |
CN104241743A (en) | Millimeter wave filter adopting frequency selectivity coupling for suppressing fundamental waves | |
CN203596401U (en) | Ultra wide band band-pass filter of stub loaded rectangular-ring resonator | |
CN204130666U (en) | A Substrate Integrated Waveguide Bandpass Filter for WLAN System | |
CN104409813A (en) | Vertical interdigital filter based on source-load coupling | |
CN107887676A (en) | One kind miniaturization balance double-passband filter | |
CN104882650B (en) | A kind of balance filter that resonator is loaded using coupling minor matters | |
CN204651448U (en) | A Balanced Filter Using Improved Coupled Feeder | |
CN107369869B (en) | A Low Insertion Loss Filter Based on Packaged Microstrip | |
CN206076464U (en) | A kind of miniaturization Terahertz low pass filter | |
CN103050754B (en) | Microstrip line-coplanar stripline broadband transitional structure | |
CN106229591B (en) | A kind of miniaturization Terahertz low-pass filter | |
CN209948010U (en) | An ultra-wideband filter with a miniaturized broadside coupling structure | |
CN203826525U (en) | Low-pass filter | |
CN108682607A (en) | A kind of U-shaped micro-strip slow-wave structure of corrugated casing | |
CN103326090B (en) | A three-pass high-temperature superconducting filter |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |