JPS6226201B2 - - Google Patents

Info

Publication number
JPS6226201B2
JPS6226201B2 JP23814184A JP23814184A JPS6226201B2 JP S6226201 B2 JPS6226201 B2 JP S6226201B2 JP 23814184 A JP23814184 A JP 23814184A JP 23814184 A JP23814184 A JP 23814184A JP S6226201 B2 JPS6226201 B2 JP S6226201B2
Authority
JP
Japan
Prior art keywords
conductor
dielectric resonator
gap
dielectric
frequency
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.)
Expired
Application number
JP23814184A
Other languages
Japanese (ja)
Other versions
JPS60143004A (en
Inventor
Hiroyuki Abe
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP23814184A priority Critical patent/JPS60143004A/en
Publication of JPS60143004A publication Critical patent/JPS60143004A/en
Publication of JPS6226201B2 publication Critical patent/JPS6226201B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P7/00Resonators of the waveguide type
    • H01P7/10Dielectric resonators

Description

【発明の詳細な説明】 この発明は、マイクロ波帯の共振回路であると
ころの誘電体共振回路に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a dielectric resonant circuit which is a microwave band resonant circuit.

この共振回路は、TiO2系のセラミツクのよう
な、低損失でかつ温度特性のよい材料で作られた
誘電体共振器と、絶縁体基板及びその上面に形成
されたストリツプ線路よりなるマイクロ波集積回
路(以下MICと略す)を結合せしめてなるもので
ある。誘電体共振器としては、円筒形又は直方体
のものが加工の容易なこと、Q値が高いことか
ら、一般的に用いられている。通常一定の形状に
成型された誘電体共振器とMICとを結合させた場
合の共振周波数は、加工の精度、ストリツプ線路
と誘電体共振器の位置関係の異同、筐体壁と誘電
体共振器の位置関係の異同等があつて、設計値通
りの値を得ることは非常に難かしかつた。従つて
既に成型済みの誘電体共振器の形状を変える事な
く、共振周波数を連続的に可変ならしめる何らか
の機構が必要とされる。
This resonant circuit consists of a dielectric resonator made of a material with low loss and good temperature characteristics, such as TiO 2 ceramic, and a microwave integrated circuit consisting of an insulating substrate and a strip line formed on its top surface. It is made by combining circuits (hereinafter abbreviated as MIC). As dielectric resonators, cylindrical or rectangular parallelepiped ones are generally used because they are easy to process and have a high Q value. The resonant frequency when a dielectric resonator, which is usually molded into a certain shape, is coupled with a MIC depends on the processing accuracy, the difference in the positional relationship between the strip line and the dielectric resonator, and the difference between the housing wall and the dielectric resonator. It was very difficult to obtain the designed value due to the difference in the positional relationship between the two. Therefore, some kind of mechanism is required that allows the resonant frequency to be varied continuously without changing the shape of the already molded dielectric resonator.

従来機械的に共振周波数を変化せしめる機構と
しては、第1図に示すように、ストリツプ線路1
に近接して設けられた誘電体共振器13の上方に
金属板15を設けこの金属板を上下せしめる事に
より、共振周波数の変化を得る機構が用いられて
いた。このような機構が筐体16内に設けられて
いるため、筐体の形状は必然的に大きなものとな
り、不要モードの発生する危険を増し、又、筐体
の幾何学的形状のより大きな温度変化が、より大
きな共振周波数変動を生ずる等の欠点があつた。
Conventionally, as a mechanism for mechanically changing the resonant frequency, a strip line 1 is used as shown in Figure 1.
A mechanism has been used in which a metal plate 15 is provided above a dielectric resonator 13 provided close to the dielectric resonator 13, and the resonant frequency is changed by moving the metal plate up and down. Since such a mechanism is provided within the housing 16, the shape of the housing is necessarily large, which increases the risk of unwanted modes and also increases the temperature of the housing geometry. There were drawbacks such as the change in resonance frequency causing larger fluctuations in the resonant frequency.

この発明の目的は、上記の欠点を除去せしめ導
電体の体積、位置を変化させて共振周波数の調整
が可能でかつ、導電体の空隙内における体積、位
置が温度変化に伴う熱膨張により微少変化する事
を利用して、誘電体共振器の周波数温度変化を補
償する事が可能で、さらに形状の小型な筐体内に
収容しうる誘電体共振回路を提供することにあ
る。
The purpose of this invention is to eliminate the above-mentioned drawbacks, and to make it possible to adjust the resonant frequency by changing the volume and position of the conductor, and to make it possible to adjust the resonance frequency by changing the volume and position of the conductor, and to make it possible for the volume and position of the conductor within the gap to change slightly due to thermal expansion caused by temperature changes. It is an object of the present invention to provide a dielectric resonant circuit that can compensate for temperature changes in the frequency of a dielectric resonator by taking advantage of this fact, and can be housed in a small-sized housing.

この発明によれば絶縁体基板及びその上面に形
成されたストリツプ線路よりなるマイクロ波集積
回路と、これに結合される誘電体共振器と、上記
絶縁体基板の一部を取り除いて形成された空隙
と、この空隙に挿入される熱膨張係数の異なる複
数種の材質の層状構造をもつ導電体を有し、この
導電体の位置、体積を変化させる事により、共振
周波数を可変ならしめた事を特徴とする誘電体共
振回路が得られる。
According to the present invention, there is provided a microwave integrated circuit comprising an insulating substrate and a strip line formed on the upper surface thereof, a dielectric resonator coupled thereto, and an air gap formed by removing a part of the insulating substrate. A conductor with a layered structure made of multiple materials with different coefficients of thermal expansion is inserted into this gap, and by changing the position and volume of this conductor, the resonant frequency can be made variable. A dielectric resonant circuit with characteristics can be obtained.

この発明による共振器においては導電体の空隙
内における体積、位置が、温度変化に伴う熱膨張
により微少変化する事を利用して誘電体共振器の
周波数温度変化を補償する事が可能となり、しか
も型状が小型でかつ温度安定度のよい誘電体共振
回路の実現が可能になる。
In the resonator according to the present invention, it is possible to compensate for temperature changes in the frequency of the dielectric resonator by utilizing the fact that the volume and position of the conductor within the gap change slightly due to thermal expansion accompanying temperature changes. It becomes possible to realize a dielectric resonant circuit that is small in size and has good temperature stability.

以下、この発明を実施例によつて詳細に説明す
る。
Hereinafter, the present invention will be explained in detail by way of examples.

第2図はこの発明の一実施例であるところの誘
電体共振回路を説明するための図である。同図に
おいて31は、一部がとり除かれて空隙34が、
形成された絶縁体基板であり、誘電体共振器33
は、絶縁体基板上で、ストリツプ線路32に近接
した位置に、上記の空隙部を覆うようにおかれて
いる。一部にねじ部が形成された導電体35は筐
体36の底部に設けられたねじ穴を通じて固定さ
れる。導電体の一部は上記の絶縁体基板に穿たれ
た空隙内に挿入されている。導電体を回転させる
事によつて筐体と金属体の相対的な位置は変化
し、導電体の空隙内に挿入されている部分の、位
置、体積が変化し、これにより共振周波数が変化
する。
FIG. 2 is a diagram for explaining a dielectric resonant circuit which is an embodiment of the present invention. In the same figure, 31 is partially removed to create a gap 34.
A dielectric resonator 33 is formed on the insulator substrate.
is placed on the insulating substrate at a position close to the strip line 32 so as to cover the above-mentioned gap. The conductor 35 partially formed with a threaded portion is fixed through a screw hole provided at the bottom of the casing 36 . A portion of the conductor is inserted into the gap bored in the insulator substrate. By rotating the conductor, the relative position of the casing and the metal body changes, and the position and volume of the part inserted into the gap of the conductor changes, which changes the resonant frequency. .

第2図より明らかなように、筐体の内部空間の
高さhは誘電体共振器の高さと絶縁体基板の厚さ
の和より大なるものであればよい。
As is clear from FIG. 2, the height h of the internal space of the casing only needs to be greater than the sum of the height of the dielectric resonator and the thickness of the insulating substrate.

ところで、上述のような周波数調整機構を備え
た共振回路の共振周波数の温度変化は誘電体共振
器の温度特性による周波数微少変化及び熱膨張現
象により、空隙内に挿入されている導電体の体
積、位置が変化する事による周波数微少変化が加
算されたものとして現出する。従つて後者の原因
による周波数微少変化によつて前者の微少変化を
補償するようにすれば周波数安定度のよい誘電体
共振回路を得ることができる。
By the way, temperature changes in the resonant frequency of a resonant circuit equipped with the above-mentioned frequency adjustment mechanism are due to minute changes in frequency due to the temperature characteristics of the dielectric resonator and thermal expansion phenomena, resulting in changes in the volume of the conductor inserted into the gap, It appears as an addition of minute changes in frequency due to changes in position. Therefore, if the former minute change is compensated for by the frequency minute change due to the latter cause, a dielectric resonant circuit with good frequency stability can be obtained.

第2図においては、導電体35の一部が導電体
本体とは熱膨張率の異なる材質の調整板39で構
成されている。いま導電体、筐体の側部が熱膨張
率γなる材質でつくられ、調整板39が熱膨張
率γなる材質でつくられているとすればγ>γ
においては温度上昇とともに、空隙内に挿入され
てある導電体部分の体積は増加する。γ<γ
場合は、これと逆の傾向が生ずる。誘電体共振器
の温度係数の、正負の別、絶対値の大小に従つ
て、適当な熱膨張率の材質を調整板の材料として
選択し、調整板の厚さを選択することにより、誘
電体共振器の温度変化を補償するような組合せを
得ることができる。
In FIG. 2, a part of the conductor 35 is composed of an adjustment plate 39 made of a material having a different coefficient of thermal expansion from that of the conductor body. Now, if the conductor and the side part of the casing are made of a material with a coefficient of thermal expansion γ 0 , and the adjustment plate 39 is made of a material with a coefficient of thermal expansion γ, then γ>γ 0.
As the temperature rises, the volume of the conductive portion inserted into the gap increases. When γ<γ 0 , the opposite trend occurs. Depending on whether the temperature coefficient of the dielectric resonator is positive or negative and the magnitude of the absolute value, a material with an appropriate coefficient of thermal expansion is selected as the material for the adjustment plate, and the thickness of the adjustment plate is selected. Combinations can be obtained that compensate for temperature variations in the resonator.

以上説明したように、この発明によれば、形状
の小型な誘電体共振器を得る事ができ、また導電
体、導電体支持体、または筐体の材質として、適
当な熱膨張率のものを選択する事により、温度変
化に対する周波数安定度のよい誘電体共振器を得
ることができ、その効果は大きい。
As explained above, according to the present invention, it is possible to obtain a dielectric resonator with a small shape, and the material of the conductor, conductor support, or casing has an appropriate coefficient of thermal expansion. By making this selection, it is possible to obtain a dielectric resonator with good frequency stability against temperature changes, which is highly effective.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の共振周波数調整機構を示す図
で、11は絶縁体基板である。第2図はこの発明
の第1の発明の一実施例を示す図である。
FIG. 1 is a diagram showing a conventional resonant frequency adjustment mechanism, and 11 is an insulating substrate. FIG. 2 is a diagram showing an embodiment of the first aspect of the present invention.

Claims (1)

【特許請求の範囲】[Claims] 1 絶縁体基板及びその上面に形成されたストリ
ツプ線路よりなるマイクロ波集積回路と、これに
結合される誘電体共振器と、上記絶縁体基板の一
部を取り除いて形成された空隙と、この空隙内に
挿入される熱膨張係数の異なる複数種の材質の層
状構造をもつ導電体を有し、この導電体の位置、
体積を変化せしめる事により、共振周波数を可変
ならしめる事を特徴とする誘電体共振回路。
1. A microwave integrated circuit consisting of an insulating substrate and a strip line formed on its upper surface, a dielectric resonator coupled thereto, a gap formed by removing a part of the insulating substrate, and this gap. It has a conductor with a layered structure of multiple types of materials with different coefficients of thermal expansion inserted into the interior, and the position of this conductor,
A dielectric resonant circuit that is characterized by making the resonant frequency variable by changing its volume.
JP23814184A 1984-11-12 1984-11-12 Dielectric resonance circuit Granted JPS60143004A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23814184A JPS60143004A (en) 1984-11-12 1984-11-12 Dielectric resonance circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23814184A JPS60143004A (en) 1984-11-12 1984-11-12 Dielectric resonance circuit

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP11403976A Division JPS6031121B2 (en) 1976-09-22 1976-09-22 dielectric resonant circuit

Publications (2)

Publication Number Publication Date
JPS60143004A JPS60143004A (en) 1985-07-29
JPS6226201B2 true JPS6226201B2 (en) 1987-06-08

Family

ID=17025798

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23814184A Granted JPS60143004A (en) 1984-11-12 1984-11-12 Dielectric resonance circuit

Country Status (1)

Country Link
JP (1) JPS60143004A (en)

Also Published As

Publication number Publication date
JPS60143004A (en) 1985-07-29

Similar Documents

Publication Publication Date Title
US4142164A (en) Dielectric resonator of improved type
JPH02502059A (en) transmission line resonator
JPS6211801B2 (en)
EP0211455B1 (en) Microwave metallic cavity
JPH01251801A (en) Three-conductor structure filter
JPS6031121B2 (en) dielectric resonant circuit
JP3174797B2 (en) Dielectric resonator
JPS6350102A (en) Dielectric resonator
JPH0628801Y2 (en) Dielectric filter
JPS6226201B2 (en)
JPH05206730A (en) Voltage controlled oscillator and adjustment method of its oscillating frequency
JP3203728B2 (en) Dielectric resonator and method for adjusting characteristics thereof
JPS6110324Y2 (en)
JPS62123801A (en) Coaxial filter
JPS61245606A (en) Microwave oscillator
JPH0342722Y2 (en)
JPH0379111A (en) Surface mount type composite piezoelectric element
JPS6320162Y2 (en)
JPS5836002A (en) Resonant circuit device
JPS6150525B2 (en)
JPH0633683Y2 (en) Three-conductor filter package
JPS627721B2 (en)
JPH0633684Y2 (en) Dielectric filter
JPS6311761Y2 (en)
JP2000252715A (en) Microwave circuit