JPS6127202Y2 - - Google Patents

Info

Publication number
JPS6127202Y2
JPS6127202Y2 JP32778U JP32778U JPS6127202Y2 JP S6127202 Y2 JPS6127202 Y2 JP S6127202Y2 JP 32778 U JP32778 U JP 32778U JP 32778 U JP32778 U JP 32778U JP S6127202 Y2 JPS6127202 Y2 JP S6127202Y2
Authority
JP
Japan
Prior art keywords
resonator
dielectric
conductor
coaxial
outer conductor
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
JP32778U
Other languages
Japanese (ja)
Other versions
JPS53145433U (en
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 filed Critical
Priority to JP32778U priority Critical patent/JPS6127202Y2/ja
Priority to US05/876,245 priority patent/US4223287A/en
Priority to DE19782805964 priority patent/DE2805964A1/en
Priority to FR7804143A priority patent/FR2380646B1/en
Publication of JPS53145433U publication Critical patent/JPS53145433U/ja
Application granted granted Critical
Publication of JPS6127202Y2 publication Critical patent/JPS6127202Y2/ja
Expired legal-status Critical Current

Links

Landscapes

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

Description

【考案の詳細な説明】 この考案は同軸共振器に関し、特に例えば内導
体および外導体間に誘電体を介在させた1/4波長
同軸TEM共振器に関する。
[Detailed Description of the Invention] This invention relates to a coaxial resonator, and particularly to a 1/4 wavelength coaxial TEM resonator in which a dielectric material is interposed between an inner conductor and an outer conductor.

従来VHF帯もしくはUHF帯で用いられている
フイルタとして、LC共振器を用いたものや、同
軸共振器を用いたものがある。しかしながら、前
者は充分な選択度特性が得られなく、後者は形状
が大きいという欠点があつた。
Filters conventionally used in the VHF band or UHF band include those using LC resonators and those using coaxial resonators. However, the former had the disadvantage that sufficient selectivity characteristics could not be obtained, and the latter had the disadvantage of being large in size.

最近では、通信機器の分野においては、システ
ムの小形軽量化が求められているが、他の部品は
小形軽量化が計られている中で、その重要性から
数多く使われているにも拘わらずフイルタは、小
形軽量化が困難なためシステムの小形軽量化を遅
らせる原因となつていた。そのためこのようなフ
イルタの小形軽量化がこの分野の技術者にとつて
至上命題であつた。そこで本考案者らは、内導体
および外導体の間に誘電体を充填した1/4波長同
軸TEM共振器を開発した。このような誘電体同
軸TEM共振器は、その小形化が可能なため、フ
イルタかつ従つてシステム全体の小形軽量化にき
わめて多大な利点を有するものである。しかしな
がら、このような誘電体を充填した1/4波長同軸
TEM共振器は、そのQが高いことから、1/4波長
共振器において避け難い3倍あるいは5倍等の高
周波成分が励振され易く、特に第3高調波共振が
スプリアスとして発生する。一方、一般の送信機
等ではアクテイブな素子は必ず2倍ないし3倍等
の高調波が発生するものであり、上述のごとくの
誘電体を充填した1/4波長同軸TEM共振器を用い
れば、その特性から前記第3高調波がスプリアス
となつて発生されることになる。
Recently, in the field of communication equipment, there has been a demand for smaller and lighter systems, and while other parts are being made smaller and lighter, despite their importance, they are still used in large numbers. Since filters are difficult to make smaller and lighter, they have been a cause of delays in reducing the size and weight of systems. Therefore, reducing the size and weight of such filters has been a top priority for engineers in this field. Therefore, the present inventors developed a quarter-wavelength coaxial TEM resonator in which a dielectric material is filled between the inner and outer conductors. Since such a dielectric coaxial TEM resonator can be made compact, it has an extremely large advantage in reducing the size and weight of the filter and therefore the entire system. However, such dielectric-filled 1/4 wavelength coaxial
Since the TEM resonator has a high Q, high frequency components such as 3 times or 5 times as high, which are difficult to avoid in a 1/4 wavelength resonator, are easily excited, and in particular, third harmonic resonance occurs as spurious. On the other hand, in general transmitters, etc., the active elements always generate harmonics such as double or triple harmonics, so if a 1/4 wavelength coaxial TEM resonator filled with a dielectric material as described above is used, Due to its characteristics, the third harmonic is generated as spurious.

それゆえに、この考案の主たる目的は、上述の
ごとくの問題点を除き、高調波のスプリアス特性
を改善し得る同軸共振器を提供することである。
Therefore, the main purpose of this invention is to provide a coaxial resonator which can improve spurious characteristics of harmonics while eliminating the above-mentioned problems.

この考案は、要約すれば、内部導体と外部導体
との間に誘電体を介在させた1/4波長同軸TEM共
振器において、その共振器の短絡側において前記
誘電体の一部を除去することによりこの部分の実
効誘電率を相対的に他の部分より小さくし、共振
特性をずらしてスプリアス特性を改善した同軸共
振器である。
In summary, this idea is to remove a part of the dielectric material on the short-circuit side of the resonator in a 1/4 wavelength coaxial TEM resonator in which a dielectric material is interposed between the inner conductor and the outer conductor. This is a coaxial resonator in which the effective dielectric constant of this portion is made relatively smaller than that of other portions, and the resonance characteristics are shifted to improve spurious characteristics.

この考案の上述の目的およびその他の目的と特
徴は図面を参照して行なう以下の詳細な説明から
一層明らかとなろう。
The above objects and other objects and features of the present invention will become more apparent from the following detailed description with reference to the drawings.

第1図はこの考案の一実施例を示す図解的断面
図である。構成において、1/4波長同軸TEM共振
器1は、それぞれ、内導体2、外導体3、前記内
導体2および外導体3の間に充填される誘電体4
を含んで成る。このような1/4波長同軸TEM共振
器1はたとえば一例として以下のような具体的構
造を有する。円筒状の誘電体4の外周壁には導体
からなる円筒状金属体を密嵌して外導体3とす
る。誘電体4の中空部分に補強のためのセラミツ
クからなる中心棒5を挿通してなる。中心棒5は
外導体3と同じ軸長で、その外周壁には例えば高
周波特性の良いかつ誘導体との接着性の良い、例
えば銀ペーストを焼き付けて内導体2としてい
る。なお、内導体2は、外導体3と同じく、導体
からなる円筒状金属体で置き換えてもよい。これ
ら金属体を用いる場合、誘電体4の外周壁や内周
壁にあらかじめ銀を焼付けた上で用いることも考
えられる。誘電体4はたとえば酸化チタン系セラ
ミツク材料が長いがこれは、損失を少あくするた
めに内導体2を銀製にする場合、銀の焼成温度が
600ないし900℃であるからこれに耐える材料であ
ることが条件となるからである。勿論、内導体2
を銀の焼き付けで形成しないときは、誘電体4は
別の材料でも良い。
FIG. 1 is a schematic sectional view showing an embodiment of this invention. In the configuration, the 1/4 wavelength coaxial TEM resonator 1 includes an inner conductor 2, an outer conductor 3, and a dielectric 4 filled between the inner conductor 2 and the outer conductor 3, respectively.
It consists of Such a 1/4 wavelength coaxial TEM resonator 1 has, for example, the following specific structure. A cylindrical metal body made of a conductor is tightly fitted into the outer peripheral wall of the cylindrical dielectric body 4 to form the outer conductor 3. A central rod 5 made of ceramic for reinforcement is inserted into a hollow portion of the dielectric 4. The center rod 5 has the same axial length as the outer conductor 3, and the inner conductor 2 is formed by baking, for example, silver paste, which has good high frequency characteristics and good adhesion to the dielectric, on its outer peripheral wall. Note that, like the outer conductor 3, the inner conductor 2 may be replaced with a cylindrical metal body made of a conductor. When using these metal bodies, it is also conceivable to use them after baking silver on the outer peripheral wall and inner peripheral wall of the dielectric body 4 in advance. The dielectric 4 is made of, for example, a titanium oxide ceramic material, but this is because when the inner conductor 2 is made of silver in order to reduce loss, the firing temperature of the silver is
This is because the temperature is 600 to 900°C, so the material must be able to withstand this temperature. Of course, inner conductor 2
When the dielectric 4 is not formed by baking silver, the dielectric 4 may be made of another material.

このような同軸共振器1によると、その一方端
側の内導体2、外導体3間6には誘電体4が存在
しないことになる。この一方端側を短絡面側とし
て用いる。誘電体4が存在していない部分6の軸
長は、共振器1の全長の1/3まで程度の長さまで
とり得るのが好ましい。
According to such a coaxial resonator 1, there is no dielectric material 4 between the inner conductor 2 and the outer conductor 3 on one end side. This one end side is used as the short circuit side. Preferably, the axial length of the portion 6 where the dielectric 4 is not present can be up to about 1/3 of the total length of the resonator 1.

上述のごとくの構成によれば、基本波の電界は
共振器の短絡面側で0また0に近いので、内導体
2、外導体3間に存在する物質(つまり通常は空
気、真空状態など)の誘電率が低くても、共振周
波数に対する影響が小さいが、第3高調波の電界
は共振器のこの短絡側においても大きくなるので
実効誘電率が著しく低下しその共振周波数に対す
る影響がきわめて大きくなる。すなわち、スプリ
アス特性を悪化させる原因である第3高調波の共
振がより高い周波数減で生じることになる。
According to the configuration described above, the electric field of the fundamental wave is 0 or close to 0 on the short-circuit surface side of the resonator, so the material existing between the inner conductor 2 and the outer conductor 3 (usually air, vacuum state, etc.) Even if the permittivity of the resonator is low, the effect on the resonant frequency is small, but the electric field of the third harmonic becomes large even on this short-circuited side of the resonator, so the effective permittivity decreases significantly and its effect on the resonant frequency becomes extremely large. . That is, resonance of the third harmonic, which is a cause of deteriorating spurious characteristics, occurs at a higher frequency.

以上のようにこの考案によれば、誘電体を内導
体および外導体の間に介在させた1/4波長同軸
TEM共振器の短絡側の固体として存在する誘電
体が欠除されているので、このように1/4波長同
軸TEM共振器に特有の第3高調波共振(励振)
の周波数が実用上問題のない高域までずれてその
スプリアス特性が著しく改善され得る。
As described above, according to this invention, a 1/4 wavelength coaxial
Since the dielectric that exists as a solid on the short-circuited side of the TEM resonator is removed, this third harmonic resonance (excitation), which is unique to the 1/4 wavelength coaxial TEM resonator, is generated.
By shifting the frequency to a high range that poses no problem in practice, the spurious characteristics can be significantly improved.

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

第1図はこの考案の一実施例を示す図解的断面
図、第2図は第1図のA−A線断面図である。 1は1/4波長同軸TEM共振器、2は内導体、3
は外導体、4は誘電体、6は誘電体4が存在して
いない部分。
FIG. 1 is a schematic sectional view showing an embodiment of this invention, and FIG. 2 is a sectional view taken along the line A--A in FIG. 1 is a 1/4 wavelength coaxial TEM resonator, 2 is an inner conductor, 3 is
4 is the outer conductor, 4 is the dielectric material, and 6 is the part where the dielectric material 4 is not present.

Claims (1)

【実用新案登録請求の範囲】 (1) 内部導体と外部導体と該内部導体および外部
導体の間に介在された誘電体とを含む1/4波長
同軸TEM共振器であつて、短絡側の前記誘電
体の一部が欠除されていることを特徴とする同
軸共振器。 (2) 外部導体が円筒状金属体からなる実用新案登
録請求の範囲第(1)項記載の同軸共振器。
[Claims for Utility Model Registration] (1) A 1/4 wavelength coaxial TEM resonator including an inner conductor, an outer conductor, and a dielectric interposed between the inner conductor and the outer conductor, wherein the A coaxial resonator characterized by having a portion of the dielectric removed. (2) The coaxial resonator according to claim (1), wherein the outer conductor is a cylindrical metal body.
JP32778U 1977-02-14 1978-01-05 Expired JPS6127202Y2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP32778U JPS6127202Y2 (en) 1978-01-05 1978-01-05
US05/876,245 US4223287A (en) 1977-02-14 1978-02-09 Electrical filter employing transverse electromagnetic mode coaxial resonators
DE19782805964 DE2805964A1 (en) 1977-02-14 1978-02-13 ELECTRIC FILTER
FR7804143A FR2380646B1 (en) 1977-02-14 1978-02-14 MICROWAVE FILTER

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32778U JPS6127202Y2 (en) 1978-01-05 1978-01-05

Publications (2)

Publication Number Publication Date
JPS53145433U JPS53145433U (en) 1978-11-16
JPS6127202Y2 true JPS6127202Y2 (en) 1986-08-14

Family

ID=28801493

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32778U Expired JPS6127202Y2 (en) 1977-02-14 1978-01-05

Country Status (1)

Country Link
JP (1) JPS6127202Y2 (en)

Also Published As

Publication number Publication date
JPS53145433U (en) 1978-11-16

Similar Documents

Publication Publication Date Title
US4506241A (en) Coaxial dielectric resonator having different impedance portions and method of manufacturing the same
JPS6353723B2 (en)
US5066933A (en) Band-pass filter
US2523841A (en) Wave guide coupler
SE7909547L (en) Radiofrequency
EP0865094A3 (en) Wave filter having two or more coaxial dielectric resonators in juxtaposition
US4271399A (en) Dielectric resonator for VHF to microwave region
JPS6127202Y2 (en)
US4313097A (en) Image frequency reflection mode filter for use in a high-frequency receiver
JPS6029204Y2 (en) coaxial resonator
JPS54154958A (en) High frequency filter
JPS5829881B2 (en) Filter using coaxial resonator
JPH0374841B2 (en)
JP2682646B2 (en) Coaxial dielectric resonator
JPS6115603Y2 (en)
JPH0856104A (en) Resonator
JPS58194406A (en) Coaxial dielectric resonator
JPS5938761B2 (en) coaxial resonator
SU843039A1 (en) Band-pass filter on overthreshold waveguide
Li et al. A dual-mode dielectric resonator filter with metal patches
JPH062323Y2 (en) Terminal pin of dielectric resonator
JPS58207701A (en) Broad band filter
JPS6114164Y2 (en)
JPS5942729Y2 (en) Distributed constant filter
JPS6029206Y2 (en) semi-coaxial cavity