JPS6161502A - Dielectric resonator - Google Patents

Dielectric resonator

Info

Publication number
JPS6161502A
JPS6161502A JP18306684A JP18306684A JPS6161502A JP S6161502 A JPS6161502 A JP S6161502A JP 18306684 A JP18306684 A JP 18306684A JP 18306684 A JP18306684 A JP 18306684A JP S6161502 A JPS6161502 A JP S6161502A
Authority
JP
Japan
Prior art keywords
deltal
thermal expansion
temperature
frequency
oscillator
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.)
Pending
Application number
JP18306684A
Other languages
Japanese (ja)
Inventor
Koji Nishida
西田 幸治
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP18306684A priority Critical patent/JPS6161502A/en
Publication of JPS6161502A publication Critical patent/JPS6161502A/en
Pending 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

Landscapes

  • Control Of Motors That Do Not Use Commutators (AREA)

Abstract

PURPOSE:To suppress the frequency fluctuation of an oscillator due to temperature change by combining two kinds of metallic members having different thermal expansion coefficient and utilizing the difference in length due to expansion. CONSTITUTION:The thermal expansion coefficient for a screw 3 and a metallic piece 7 is different from each other, the thermal expansion coefficients are taken as (b), (a), the distance is taken as (l) and the length of the screw 3 is taken as l1, and the temperature range is DELTAl of the distance 5 due to tempera ture change DELTAT is expressed as DELTAll=DELTAT.[al-l1(b-a)]. The size has a relation with an oscillator frequency and when the range in DELTAl changes, the temperature fluctuation width of the oscillated frequency is changed. When b>a in the relation with DELTAl, the value DELTAl changes when the (l) is changed and the polarity of the DELTAl is changed at a certain (l). Since the (l) must be larger than 0, when a more negative is required, the two metals having a large thermal expansion coefficient difference is used.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は、衛星放送直接受信装置等のコンバータ;:
、使用される誘電体共振器に関するものでへ 、特(:その湿度変化に対する周波数の安定化(=関す
るものである。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a converter for a satellite broadcast direct receiving device, etc.;
This relates to the dielectric resonator used, and especially to the stabilization of its frequency against changes in humidity.

〔従来の技術〕[Conventional technology]

一般に、この種の共振器(発振器)に要求される性能と
しては、発振周波数は10.678 GHzであり、温
度範囲(−30°C〜+50°0)における発振周波数
変動は、±1.5 MHz以下というように非常(:狭
い変動幅を要求されている。第1図は従来のこの種の装
置の断面側面図を示すもので、(1)は所要の発振周波
数(共振周波数)に応じて所定形状(:形成された誘電
体、(21は発振周波数の微調整用金属板、(3)は金
属板(21を上下させるためのねじ部、(4)はケース
、(51は誘電体(1)と金属板(2)の対向間隔、(
61はねじ部(3)のケース内の長さである。
Generally, the performance required for this type of resonator (oscillator) is that the oscillation frequency is 10.678 GHz, and the oscillation frequency fluctuation in the temperature range (-30°C to +50°0) is ±1.5. A very narrow fluctuation range, such as MHz or less, is required. Figure 1 shows a cross-sectional side view of a conventional device of this type. (21 is a metal plate for fine adjustment of the oscillation frequency, (3) is a metal plate (screw part for raising and lowering 21, (4) is a case, (51 is a dielectric body) The opposing distance between (1) and metal plate (2), (
61 is the length of the threaded portion (3) inside the case.

次に従来技術の動作について説明する。Next, the operation of the prior art will be explained.

ねじ部(3)を動かすことにより、間隔(5)を変え、
発振器の発振周波数を設定する。室温で望む発振周波数
(:設定した後、ねじ(3)をケース+41に、固定し
て動かないようC二する。ここで、この従来のものでは
、ねじ部(3)とケース(4)とは、同材質または膨張
係数のあまり変わらないものを使用しているので、温度
が変化すると、ケース(4)の熱膨張により間隔(5)
が変動する。又、発振器固有の周波域変動が起きる。従
来はその発振周波数変動を補正するような温度係数を持
つ誘電体(11を使用し、発振周波数の温度変動を押え
ていた。
By moving the screw part (3), the interval (5) can be changed,
Set the oscillation frequency of the oscillator. After setting the desired oscillation frequency at room temperature, fix the screw (3) to the case +41 and apply C2 so that it does not move.In this conventional type, the screw part (3) and the case (4) are made of the same material or have a coefficient of expansion that does not change much, so when the temperature changes, the interval (5) will change due to the thermal expansion of the case (4).
changes. Furthermore, fluctuations in the frequency range specific to the oscillator occur. Conventionally, a dielectric material (11) having a temperature coefficient that corrects the oscillation frequency fluctuation has been used to suppress the temperature fluctuation of the oscillation frequency.

従来の装置では、以上のよう(;構成されているので、
温度が変化すると、発振周波数が変化し、また能動素子
のバラツキや、発振器固有のバラツキによる周波数変動
が発生したりすることにより、発振周波数の温度変動が
大きくなり、要求性能を満足しなくなる。その場合には
、温度係数の違う誘電体共振器に変更しなければならな
いが、変えた誘電体共振器の寸法、温度係数のバラツキ
により、再調整をせざるを得ない。再現性が悪く、調整
に相当の時間を要するなどの欠点があった。
Conventional devices are configured as shown above (;
When the temperature changes, the oscillation frequency changes, and frequency fluctuations occur due to variations in active elements and variations inherent in the oscillator, so the temperature fluctuations in the oscillation frequency become large and the required performance is no longer satisfied. In that case, it is necessary to change to a dielectric resonator with a different temperature coefficient, but due to variations in the dimensions and temperature coefficient of the changed dielectric resonator, readjustment is necessary. There were drawbacks such as poor reproducibility and a considerable amount of time required for adjustment.

〔発明の概要〕[Summary of the invention]

この発明は、上記のような従来ものの欠点を除去するた
め(=なされたもので、熱膨張係数の異なる2種類の金
属部材を組み合わせて、その膨張長さの差を利用するこ
とにより、温度変化に対する発振器の周波数変動を抑制
することができる誘電体共振器を提供するものである。
This invention was made in order to eliminate the drawbacks of the conventional products as described above, and by combining two types of metal members with different coefficients of thermal expansion and utilizing the difference in their expansion lengths, temperature changes can be reduced. The present invention provides a dielectric resonator capable of suppressing frequency fluctuations of an oscillator relative to the oscillator.

〔発明の実施例〕[Embodiments of the invention]

以下この発明の一実施例を図について説明する。 An embodiment of the present invention will be described below with reference to the drawings.

第2図において、(1)は誘電体共振器、(2)は発振
周波数の微調整用の金属板、(3)は金属板(2)を上
下させるためのねじ部、(4)はケース、(5)は誘電
体共振器(1)と金属板(2)の間隔、(6)はネジ、
部(3)のケース内の長さ、(7)はねじ部(3)と膨
張係数の違う金属片で、この金属片(7)はその取付ね
じ+81 +−より上下移動可能にケース(4)に取付
けられている。+91は間隔(5)とネジ部(61の長
さの和である。
In Figure 2, (1) is a dielectric resonator, (2) is a metal plate for fine adjustment of the oscillation frequency, (3) is a screw part for raising and lowering the metal plate (2), and (4) is a case. , (5) is the distance between the dielectric resonator (1) and the metal plate (2), (6) is the screw,
The length of part (3) inside the case, (7) is a metal piece with a different coefficient of expansion from the threaded part (3), and this metal piece (7) is attached to the case (4) so that it can be moved up and down from its mounting screw +81 +-. ). +91 is the sum of the distance (5) and the length of the threaded portion (61).

第2図(−おいて、ねじ部(3)と金属片(7)の熱膨
張係数が明らかに違うものを使用し、それぞれの膨張係
数なり、aとする、間隔(5)を!、ネジ部(3)の長
さを11とし、また温度範囲をnとした場合、ΔTの温
度変化による間隔(5)の変化ΔノはΔj=ΔT ・(
aj −is (k>−a ) ) ・−・−・−・一
式(1)となる。このΔノと発振器周波数とが関係あり
、ajの範囲が変わると、発振周波数の温度変動幅も変
わること(:なる。それらの−例を第3図に示す。
Figure 2 (-) Use threaded part (3) and metal piece (7) with clearly different coefficients of thermal expansion, each coefficient of expansion is a, the interval (5) is!, screw When the length of part (3) is 11 and the temperature range is n, the change Δ in interval (5) due to temperature change in ΔT is Δj=ΔT ・(
aj −is (k>−a) ) ・−・−・−・Set (1) is obtained. There is a relationship between Δ and the oscillator frequency, and as the range of aj changes, the temperature fluctuation range of the oscillation frequency also changes.An example of this is shown in FIG.

ところで、ajと)との関係は、b)aの場合、図4に
示すよう(:、イが変わるとΔlの値がかわり、ある!
になるとΔ)の正負が変わる。ただし、ノは0より大き
くなくてはならないので、Δノが大きい負の値が必要な
時(=は、2つの金属の膨張係数の差の大きいものを使
用すれば良い。
By the way, in the case of b) a, the relationship between aj and ) is as shown in FIG.
When it becomes, the sign of Δ) changes. However, since ∆ must be greater than 0, when ∆ requires a large negative value (= should be used with a large difference in the expansion coefficients of the two metals).

次(:、周波数を調整する時の一例を説明する。Next (:, An example of adjusting the frequency will be explained.

発振器の発振周波数が能動素子や発振器固有による温度
変動幅が一Δf存在する時、それを打ち消す+Δfに相
当するΔ]を第3図から求め、さら;二ΔJC相当する
lを第4図から求める、!に相当する11は式fi+よ
り 11が求まれば、jlの長さになるよう取付ねじ(8)
をゆるめ、金属片(7)の長さを11にし、間隔(51
がl l”l。
When the oscillation frequency of the oscillator has a temperature fluctuation range of 1Δf due to the active elements and the oscillator, Δ] corresponding to +Δf to cancel it is determined from Figure 3, and l corresponding to 2ΔJC is determined from Figure 4. ,! 11, which corresponds to
Loosen the metal piece (7) and set the length of the metal piece (7) to 11.
ga l l”l.

なるようネジ部(3)を調整した後、取付ねじ18)を
締付け、固定する。このように11を変え毬ことにより
、所望する温度変動幅に簡単に設定出来る。さらに、温
度変動幅をOに近くすることが出来、能動素子のバラツ
キ、発振器固有のバラツキが存在しても要求性能を十分
に満足出来る。
After adjusting the threaded part (3) so that By changing 11 in this way, it is possible to easily set the desired temperature fluctuation range. Furthermore, the temperature fluctuation range can be made close to O, and the required performance can be fully satisfied even if there are variations in active elements and variations inherent in the oscillator.

なお、上記の実施例では金属片(7)の長さを調整した
が、図5(:示すように固定器αqを設けることでもよ
く、その位置を上下方向に動かすことにより、ねじ部(
3)の長さ(6ンを変えれば、同様の効果を奏する。な
おこの場合のケース(4)は上記実施例の金属片(7)
と同様::ねじ部(3)の熱膨張係数とは異なるものを
使用するものとする。
Although the length of the metal piece (7) was adjusted in the above embodiment, it is also possible to provide a fixator αq as shown in FIG.
The same effect can be obtained by changing the length (6) of 3). In this case, case (4) is the metal piece (7) of the above example.
Same as:: A coefficient of thermal expansion that is different from that of the threaded portion (3) shall be used.

〔発明の効果〕〔Effect of the invention〕

以上のよう(−1この発明(=よれば、ねじ部と金属片
の熱膨張係数を相違させると共に金属片の長さを調整で
きるよう構成したので、誘電体と金属板の対向間隔の変
動のみならず、能動素子、その他の温度に対する周波数
変動要因が存在したとしても、それを含めた周波数の安
定化を図ることが出来る。
As described above (-1) According to this invention (=), since the threaded part and the metal piece are configured to have different coefficients of thermal expansion and the length of the metal piece can be adjusted, only the variation in the facing distance between the dielectric material and the metal plate is possible. Rather, even if there are active elements or other frequency fluctuation factors due to temperature, it is possible to stabilize the frequency including that.

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

第1図は従来の誘電体共振器(発振器)を示す断面側面
図、第2図はこの発明の一実施例(:よる誘電体共振器
(発振器)の断面側面図、第3図および第4図は第2図
の動作を説明するための特性図、第5図はこの発明の他
の実施例を示す断面側面図である。 (I+・・・誘電体共振器、(2)・・・金属板、(3
)・・・ねじ部、(4)・・・ケース、(7)・・・金
属片、(8)・・・取付ねじ。 なお、図中同一符号は同一、又は相当部分を示す。
FIG. 1 is a cross-sectional side view showing a conventional dielectric resonator (oscillator), FIG. 2 is a cross-sectional side view of a dielectric resonator (oscillator) according to an embodiment of the present invention, and FIGS. The figure is a characteristic diagram for explaining the operation of Fig. 2, and Fig. 5 is a cross-sectional side view showing another embodiment of the present invention. (I+... dielectric resonator, (2)... Metal plate, (3
)...Threaded part, (4)...Case, (7)...Metal piece, (8)...Mounting screw. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】[Claims] ケース内に設けられた誘電体、この誘電体に対向して配
設される金属板、この金属板がその一端側に設けられ、
上記誘電体と上記金属板との対向間隔を調整する調整部
材、この調整部材の他端側を移動調整可能に支持し、か
つ上記調整部材と並行する上記ケースの一部を形成する
と共にその長さが調整できるよう上記ケースに取付けら
れた金属片を備え、上記金属片と調整部材の熱膨張係数
が異なるようにしたことを特徴とする誘電体共振器。
A dielectric provided in the case, a metal plate disposed opposite to the dielectric, this metal plate provided on one end side,
An adjusting member for adjusting the facing distance between the dielectric and the metal plate, supporting the other end of the adjusting member so as to be movably adjustable, forming a part of the case parallel to the adjusting member, and extending the length of the adjusting member. A dielectric resonator comprising a metal piece attached to the case so that the height can be adjusted, and the metal piece and the adjustment member have different coefficients of thermal expansion.
JP18306684A 1984-08-31 1984-08-31 Dielectric resonator Pending JPS6161502A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18306684A JPS6161502A (en) 1984-08-31 1984-08-31 Dielectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18306684A JPS6161502A (en) 1984-08-31 1984-08-31 Dielectric resonator

Publications (1)

Publication Number Publication Date
JPS6161502A true JPS6161502A (en) 1986-03-29

Family

ID=16129149

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18306684A Pending JPS6161502A (en) 1984-08-31 1984-08-31 Dielectric resonator

Country Status (1)

Country Link
JP (1) JPS6161502A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114665246A (en) * 2022-04-15 2022-06-24 武汉凡谷电子技术股份有限公司 Dielectric resonator, filter, communication equipment and installation method

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114665246A (en) * 2022-04-15 2022-06-24 武汉凡谷电子技术股份有限公司 Dielectric resonator, filter, communication equipment and installation method
CN114665246B (en) * 2022-04-15 2024-04-05 武汉凡谷电子技术股份有限公司 Dielectric resonator, filter, communication equipment and installation method

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