JPS6142882B2 - - Google Patents
Info
- Publication number
- JPS6142882B2 JPS6142882B2 JP52072418A JP7241877A JPS6142882B2 JP S6142882 B2 JPS6142882 B2 JP S6142882B2 JP 52072418 A JP52072418 A JP 52072418A JP 7241877 A JP7241877 A JP 7241877A JP S6142882 B2 JPS6142882 B2 JP S6142882B2
- Authority
- JP
- Japan
- Prior art keywords
- resonator
- substrate
- casing
- dielectric
- resonant circuit
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P7/00—Resonators of the waveguide type
- H01P7/08—Strip line resonators
- H01P7/082—Microstripline resonators
Landscapes
- Non-Reversible Transmitting Devices (AREA)
- Stabilization Of Oscillater, Synchronisation, Frequency Synthesizers (AREA)
- Control Of Motors That Do Not Use Commutators (AREA)
Description
【発明の詳細な説明】
本発明は、高周波帯で使用する共振器に関する
ものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a resonator used in a high frequency band.
誘電体基板上に共振回路を構成する平面化共振
器としては、マイクロストリツプ線路、サスペン
デツト線路,スロツト線路,共平面線路などがあ
る。 Planar resonators forming a resonant circuit on a dielectric substrate include microstrip lines, suspended lines, slot lines, and coplanar lines.
第1図は、サスペンデツト線路構造での共振回
路の構成例である。第1図は直線形の両端開放共
振器を示すもので、1は結合部、2は共振回路で
この長さは共振波長の半分又は4分の1等に設計
される。3は誘電体基板である。 FIG. 1 shows an example of the configuration of a resonant circuit in a suspended line structure. FIG. 1 shows a linear resonator with both ends open. 1 is a coupling portion, 2 is a resonant circuit, and the length thereof is designed to be half or a quarter of the resonant wavelength. 3 is a dielectric substrate.
第2図はこの誘電体基板を筐体の中に保持した
状態を示す図である。誘電体基板21の上に共振
回路パターン24が形成されている。これを金属
筐体22の中に支持台23の上に保持して固定す
る。即ちサスペンデツト線路の構造をとる。 FIG. 2 is a diagram showing a state in which this dielectric substrate is held in a casing. A resonant circuit pattern 24 is formed on the dielectric substrate 21 . This is held and fixed in a metal casing 22 on a support stand 23. That is, it has a suspended line structure.
さて、高周波帯における共振器の温度に対する
安定化を行うためには、たとえば同軸形又は導波
管の共振器において線膨張係数の異なる金属を用
いる方法が多くとられているが、高周波平面回路
化共振器例えばサスペンデツト線路の共振器等に
ついては、この方法は適用困難であつた。 Now, in order to stabilize the temperature of a resonator in a high frequency band, many methods are used, for example, to use metals with different coefficients of linear expansion in coaxial or waveguide resonators. This method is difficult to apply to resonators such as resonators of suspended lines.
本発明は、上記従来技術の欠点に鑑み、サスペ
ンデツト線路構造を有する1/2波長両端開放型の
共振器に対し、基板の厚さ、前記基板と接地筐体
との間隔、及び筐体の高さの間に特定の関係をも
たらせた上で、前記基板として誘電率の温度係数
が負であるポリフツ化エチレン系部材を用いるこ
とにより、特に線膨張係数の異なる金属や、誘電
率の温度係数の異なる誘電体等を組み合わせるこ
となく、温度特性の良い共振器を提供しようとす
るものである。 In view of the above-mentioned drawbacks of the prior art, the present invention provides a 1/2 wavelength open-ended resonator having a suspended line structure, with the thickness of the substrate, the distance between the substrate and the grounded casing, and the height of the casing. By creating a specific relationship between the dielectric constant and the temperature coefficient of the dielectric constant, by using a polyethylene fluoride member with a negative temperature coefficient of dielectric constant as the substrate, it is possible to The objective is to provide a resonator with good temperature characteristics without combining dielectric materials with different coefficients.
以下、図面を用いてその一実施例を説明する。 An embodiment will be described below with reference to the drawings.
まず本発明の基本的概念から説明すると、第2
図において、基板の支持高さΔh=0(これはシ
ールドしたマイクロストリツプ線路に該当する)
から、次第に高くしてゆくと、共振器としては、
はじめ誘電体の誘電率の寄与が大きく、次第にそ
の寄与が小さくなる。即ち、Δhを大きくすれば
等価誘電率は小さくなる。 First, the basic concept of the present invention will be explained.
In the figure, the support height of the board Δh = 0 (this corresponds to a shielded microstrip line)
If the height is gradually increased from , as a resonator,
At first, the contribution of the dielectric constant of the dielectric is large, and the contribution gradually becomes smaller. That is, as Δh increases, the equivalent dielectric constant decreases.
これを共振器の温度変化という点でみれば、Δ
hが小さい場合には、誘電率の温度変化の依存度
が大きく、Δhを大きくすれば金属導体の線膨張
係数が大きく効いてくる。即ち、共振器の共振周
波数は、実効誘電率εr,共振回路長をlとす
れば、
で与えられる。この温度変化を零とするためには
Kを定数として、
df/dT=K(df/dεr・dεr/dT+df
/dl・dl/dT)=0……(2)
にする必要がある。 If we look at this in terms of temperature change in the resonator, Δ
When h is small, the dependence of the dielectric constant on temperature changes is large, and when Δh is large, the coefficient of linear expansion of the metal conductor becomes more effective. That is, the resonant frequency of the resonator is given by the effective permittivity ε r and the resonant circuit length l. is given by In order to make this temperature change zero, with K as a constant, df/dT=K(df/dε r・dε r /dT+df
/dl・dl/dT)=0...(2) It is necessary to do so.
今、金属導体の線膨張係数をα,実効誘電率の
温度係数をβとすれば(2)式より近似的に
β≒2α ……(3)
で、温度補償が可能である。 Now, if the coefficient of linear expansion of the metal conductor is α and the temperature coefficient of the effective dielectric constant is β, temperature compensation is possible by approximating β≒2α from equation (2) (3).
即ち、誘電率の負の温度係数を有する誘電体材
料においては、第2図に示す基板支持方式におい
て、特に何らの他の材料を附属せしめることな
く、共振器の温度補償が可能である。 That is, in the case of a dielectric material having a negative temperature coefficient of permittivity, temperature compensation of the resonator is possible without adding any other material in the substrate support method shown in FIG.
さらに本発明の場合、誘電体基板としてはポリ
フツ化エチレン系部材が使用される。このポリフ
ツ化エチレン系フアイバグラスを使用した時、第
2図に示す様に、誘電体基板の厚さ:h0,基板と
筐体低面(接地面)との間隔:Δh,筐体の高さ
(接地導体の間隔):Hとの間を
h0:Δh:H=0.5〜1.2:1.7:10の範囲に選ぶ
と共振器の温度補償が十分有効に行われる。この
場合共振回路の導体幅Wは、ほとんど影響がなく
無視しうる。 Furthermore, in the case of the present invention, a polyfluorinated ethylene member is used as the dielectric substrate. When this polyfluorinated ethylene fiberglass is used, as shown in Figure 2, the thickness of the dielectric substrate: h 0 , the distance between the substrate and the lower surface of the casing (ground plane): Δh, and the height of the casing. If the distance between h 0 :Δh:H=0.5 and 1.2:1.7:10 is selected, temperature compensation of the resonator can be performed sufficiently effectively. In this case, the conductor width W of the resonant circuit has almost no effect and can be ignored.
以下にその実施例を示す。第3図は、誘電体基
板として厚さ0.8mmのポリフツ化エチレン系ガラ
ス樹脂基板を用い、共振回路長170mm,幅4mmの
回路を構成し、筐体内の高さ10mmの中に支持した
時の共振周波数の温度係数を基板の高さΔhを変
数として示したものである。 Examples are shown below. Figure 3 shows a circuit with a resonant circuit length of 170 mm and a width of 4 mm using a polyethylene fluoride glass resin substrate with a thickness of 0.8 mm as a dielectric substrate and supported within a 10 mm height inside the housing. The temperature coefficient of the resonance frequency is shown using the substrate height Δh as a variable.
本実施例では、Δh=1.7mmとすれば安定度の
良い発振器が得られることがわかる。 In this example, it can be seen that if Δh=1.7 mm, a highly stable oscillator can be obtained.
これよりΔhの小さいところでは、第(1)式か
ら、共振周波数の変化はεrの効果が大きく、正
の係数を有する。 When Δh is smaller than this, from equation (1), the change in resonance frequency has a large effect of ε r and has a positive coefficient.
実際にはΔh=1.7mmで+10ppm/℃以下の安
定度を得ることができた。誘電体基板としては他
に、ポリフツ化エチレン系板が使用できる。また
共振回路の導体幅Wの変化は長さの変化に比して
非常に小さく、問題は少ない。 In reality, we were able to obtain stability of less than +10 ppm/°C at Δh=1.7 mm. Alternatively, a polyethylene fluoride board can be used as the dielectric substrate. Further, the change in the conductor width W of the resonant circuit is very small compared to the change in length, so there are few problems.
この様に本発明は、平面回路化の共振器におい
て、特に新たな温度補償用のコンデンサ、誘電体
等の材料部品を附加することなく、回路が構成さ
れている誘電体基板の筐体における保持の方法及
びその誘電体基板の材質のみによつて、極めて簡
単な構造の周波数安定度の良い共振器を得ること
ができる。 In this manner, the present invention provides a method for holding a dielectric substrate on which a circuit is configured in a case in a planar circuit resonator without adding any new temperature-compensating capacitors, dielectrics, or other material components. By using only the method described above and the material of the dielectric substrate, a resonator with an extremely simple structure and good frequency stability can be obtained.
このような共振器の構造を用い、同体発振素子
(ガンダイオードやインパツトダイオード)やト
ランジスタを接続して発振器を構成すれば、共振
回路系の安定度は極めて向上する。 If such a resonator structure is used and an oscillator is constructed by connecting an in-body oscillation element (a Gunn diode or an impact diode) and a transistor, the stability of the resonant circuit system will be greatly improved.
第1図はサスペンデツト線路構造での共振回路
の構成例を示す平面図、第2図は本発明の一実施
例における共振器の断面図、第3図は基板保持の
高さ(Δh)による温度係数の変化を示す図であ
る。
21……誘電体基板、22……金属筐体、23
……支持台。
Fig. 1 is a plan view showing an example of the configuration of a resonant circuit in a suspended line structure, Fig. 2 is a cross-sectional view of a resonator in an embodiment of the present invention, and Fig. 3 is a temperature change depending on the substrate holding height (Δh). FIG. 3 is a diagram showing changes in coefficients. 21...Dielectric substrate, 22...Metal casing, 23
...Support stand.
Claims (1)
端開放型の共振器において、前記基板厚さh0,前
記基板と接地筐体との間隔Δh,筐体の高さHの
間にh0:Δh:H=0.5〜1.2:1.7:10の関係が成
り立つように構成するとともに、前記基板として
誘電率の温度係数が負であるポリフツ化エチレン
系部材を用いたことを特徴とする共振器。1. In a 1/2 wavelength open-ended resonator with a suspended line structure, the distance between the substrate thickness h 0 , the distance Δh between the substrate and the grounded casing, and the height H of the casing h 0 : Δh: 1. A resonator characterized in that the resonator is constructed so that the relationship of H=0.5 to 1.2:1.7:10 holds, and that a polyfluorinated ethylene member having a negative temperature coefficient of dielectric constant is used as the substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7241877A JPS546745A (en) | 1977-06-17 | 1977-06-17 | Resonator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7241877A JPS546745A (en) | 1977-06-17 | 1977-06-17 | Resonator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS546745A JPS546745A (en) | 1979-01-19 |
| JPS6142882B2 true JPS6142882B2 (en) | 1986-09-24 |
Family
ID=13488704
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7241877A Granted JPS546745A (en) | 1977-06-17 | 1977-06-17 | Resonator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS546745A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP3869776A1 (en) | 2020-02-20 | 2021-08-25 | Ricoh Company, Ltd. | Image reading device and image forming apparatus incorporating same |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5795705A (en) * | 1980-12-05 | 1982-06-14 | Matsushita Electric Ind Co Ltd | High frequency oscillating circuit |
| JP2683432B2 (en) * | 1989-11-13 | 1997-11-26 | 三菱電機株式会社 | MIC type frequency converter |
| JP4990488B2 (en) * | 2004-10-01 | 2012-08-01 | 矢崎総業株式会社 | Indicator lighting structure for instruments |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5256761Y2 (en) * | 1972-08-08 | 1977-12-22 |
-
1977
- 1977-06-17 JP JP7241877A patent/JPS546745A/en active Granted
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP3869776A1 (en) | 2020-02-20 | 2021-08-25 | Ricoh Company, Ltd. | Image reading device and image forming apparatus incorporating same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS546745A (en) | 1979-01-19 |
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