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JPS6156882B2 - - Google Patents
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JPS6156882B2 - - Google Patents

Info

Publication number
JPS6156882B2
JPS6156882B2 JP3217880A JP3217880A JPS6156882B2 JP S6156882 B2 JPS6156882 B2 JP S6156882B2 JP 3217880 A JP3217880 A JP 3217880A JP 3217880 A JP3217880 A JP 3217880A JP S6156882 B2 JPS6156882 B2 JP S6156882B2
Authority
JP
Japan
Prior art keywords
yoke
cheese
coaxial line
mode
mode wave
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
JP3217880A
Other languages
Japanese (ja)
Other versions
JPS56129402A (en
Inventor
Shojiro Kanitani
Fumio Takeda
Osami Ishida
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 JP3217880A priority Critical patent/JPS56129402A/en
Publication of JPS56129402A publication Critical patent/JPS56129402A/en
Publication of JPS6156882B2 publication Critical patent/JPS6156882B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/16Auxiliary devices for mode selection, e.g. mode suppression or mode promotion; for mode conversion
    • H01P1/162Auxiliary devices for mode selection, e.g. mode suppression or mode promotion; for mode conversion absorbing spurious or unwanted modes of propagation

Landscapes

  • Waveguide Connection Structure (AREA)
  • Waveguide Switches, Polarizers, And Phase Shifters (AREA)
  • Waveguides (AREA)

Description

【発明の詳細な説明】 この発明は、マイクロ波で用いられる導波管チ
ヨークの改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a waveguide choke used in microwaves.

マイクロ波の同軸線路あるいは導波管におい
て、二つの同軸線路あるいは二つの導波管を機械
的に非接触とし、かつ電気的に接続する場合には
非接触部に4分の1波長チヨークを設ける必要が
ある。
In microwave coaxial lines or waveguides, when two coaxial lines or two waveguides are mechanically non-contact and electrically connected, a quarter-wavelength choke is provided in the non-contact part. There is a need.

第1図は、2周波数帯共用導波管チヨークの一
例を示す斜視図であり、図中、1は内導体、2は
外導体、3は内導体1と外導体2とから形成され
る同軸線路、4は円形導波管、5は円形導波管4
中の伝搬する高周波数帯HのTE11モード波に対
して動作するチヨークH、6は同軸線路3中を伝
搬する低周波数帯LのTEMモード波に対して動
作するチヨークLである。
FIG. 1 is a perspective view showing an example of a two-frequency band common waveguide yoke. In the figure, 1 is an inner conductor, 2 is an outer conductor, and 3 is a coaxial line, 4 is a circular waveguide, 5 is a circular waveguide 4
The yoke H and 6 operate on the TE 11 mode wave in the high frequency band H propagating in the coaxial line 3, and the yoke L operates on the TEM mode wave in the low frequency band L propagating in the coaxial line 3.

第2図はチヨークH5、チヨークL6の一部を
拡大した断面図であり、図中、チヨークH5の深
さ方向底部分をA、チヨークH5の円形導波管4
側部分をC,AとCとの中間の位置にある非接触
部をB、チヨークL6の深さ方向底部分をD、チ
ヨークL6の同軸線路3側部分をEとする。B部
分はCとD部分の中間の位置でもある。AとB部
分およびBとC部分の距離をlH,BとD部分お
よびBとE部分の距離をlLとする。
FIG. 2 is an enlarged cross-sectional view of a part of the yoke H5 and the yoke L6.
The side portion is C, the non-contact portion located between A and C is B, the bottom portion in the depth direction of the yoke L6 is D, and the coaxial line 3 side portion of the yoke L6 is E. Part B is also at a position intermediate between parts C and D. Let the distance between A and B portions and B and C portions be l H , and the distance between B and D portions and B and E portions be l L .

まず、チヨークH5の動作原理を説明する。 First, the principle of operation of the yoke H5 will be explained.

円形導波管4にTE11モード波が伝搬すると、
チヨークH5中には、同軸線路のTE11モード波
が励振される。これを第3図および第4図に示
す。図中、円形導波管4中に示す矢印は円形導波
管のTE11モード波の電気力線を示し、チヨーク
H5中に示す矢印はチヨークH5を同軸線路とし
たときの同軸線路のTE11モード波の電気力線を
示す。
When the TE 11 mode wave propagates in the circular waveguide 4,
A TE 11 mode wave of the coaxial line is excited in the chain H5. This is shown in FIGS. 3 and 4. In the figure, the arrow shown in the circular waveguide 4 indicates the electric line of force of the TE 11 mode wave of the circular waveguide, and the arrow shown in the yoke H5 indicates the TE 11 of the coaxial line when the yoke H5 is used as a coaxial line. Shows the electric field lines of mode waves.

第4図は、第3図中にイ,ロで示す部分の断面
図である。
FIG. 4 is a sectional view of the portions indicated by A and B in FIG. 3.

いま、Hの波に対するチヨークH5中の同軸
線路TE11モード波の管内波長をλgTE11 とし、 lH=λgTE11 /4 ……(1) とすると、チヨークH5のA部分は電気的に短絡
されているためB,C部分ではそれぞれ電気的に
開放および短絡状態となる。このため、円形導波
管4はC部分において機械的に非接触ではある
が、電気的に短絡状態となるため、電気的に連続
な円形導波管4として動作する。
Now, let the tube wavelength of the coaxial line TE 11 mode wave in the chain yoke H5 for the H wave be λg TE11 H , and l H = λg TE11 H /4 ...(1), then the A part of the yoke H5 is electrically Since they are short-circuited, portions B and C are electrically open and short-circuited, respectively. Therefore, although the circular waveguide 4 is mechanically non-contact at the portion C, it is electrically short-circuited, and thus operates as an electrically continuous circular waveguide 4.

つぎにチヨークL6の動作原理を説明する。 Next, the principle of operation of the yoke L6 will be explained.

チヨークL6の動作原理は、前述したチヨーク
H5の動作原理と同様である。すなわち、同軸線
路3をTEMモード波が伝搬するので、チヨーク
L6には、TEMモード波が励振される。このた
め、チヨークL6中のTEMモード波の波長をλ
TEM とし、チヨークL6の深さlLを lL=λTEM /4 ……(2) とするとE部分が電気的には短絡される。
The operating principle of the yoke L6 is similar to the operating principle of the yoke H5 described above. That is, since the TEM mode wave propagates through the coaxial line 3, the TEM mode wave is excited in the chain yoke L6. For this reason, the wavelength of the TEM mode wave in the chiyoke L6 is set to λ
TEM L and the depth l L of the yoke L6 as l LTEM L /4 (2), the E portion is electrically short-circuited.

チヨークH5、チヨークL6の各チヨーク単体
のもつ電気的特性は、それぞれ比較的広帯域に良
好な特性を呈する。しかし、使用帯域内におい
て、設計周波数以外の周波数ではその性能が若干
劣化する。
The electric characteristics of each of the yoke H5 and the yoke L6 are relatively good over a wide band. However, within the used band, the performance deteriorates slightly at frequencies other than the design frequency.

C部分が電気的に不完全な短絡状態のチヨーク
H5を用いると、チヨークH5中の同軸線路の
TE11モード波がB部分の非接触部を介してチヨ
ークL6中に漏洩し、チヨークL6内に同軸線路
のTE11モード波が励振される。チヨーク6内に
励振された同軸線路のTE11モード波の管内波長
をλTE11 とするとλTE11 の2分の1の整数
倍がlL
と等しくなる周波数においてチヨークL6のB部
分は電気的に短絡状態となる。
When using a short-circuited cheese yoke H5 where the C portion is electrically incomplete, the coaxial line in the yoke H5
The TE 11 mode wave leaks into the cheese yoke L6 through the non-contact portion of the B portion, and the TE 11 mode wave of the coaxial line is excited in the cheese yoke L6. If the tube wavelength of the TE 11 mode wave of the coaxial line excited in the cheese yoke 6 is λ TE11 L , then the integer multiple of 1/2 of λ TE11 L is l L
At a frequency equal to , the B portion of the chain yoke L6 becomes electrically short-circuited.

このため、チヨークH5のC部分は電気的に開
放状態に近くなり、チヨークH5を用いた円形導
波管4は電気的に不連線な特性を示す。
Therefore, the portion C of the yoke H5 becomes electrically close to an open state, and the circular waveguide 4 using the yoke H5 exhibits electrically discontinuous characteristics.

したがつて、従来の2周波数帯共用チヨークに
おいては、HLの波に対して最適に設計した
チヨークH5、チヨークL6を用いても、H
Lの周波数比によつては、高い使用周波数帯域
にVSWRの劣化および伝送損失の増大する現象の
生じる場合があつた。このため、従来このような
現象を避けるため、2周波数帯共用チヨークはチ
ヨークL6の形状が制限され、Lの波に対して
最適設計がおこなえない欠点があつた。
Therefore, in the conventional two-frequency band common cheese yoke, even if the yoke H5 and the yoke L6, which are optimally designed for H and L waves, are used, the H ,
Depending on the frequency ratio of L , deterioration of VSWR and increase in transmission loss may occur in high frequency bands used. For this reason, conventionally, in order to avoid such a phenomenon, the shape of the joint yoke L6 of the two-frequency band common yoke was limited, which had the disadvantage that an optimal design for the L wave could not be performed.

この発明はこれらの欠点を除去するため低周波
数帯用チヨークの同軸線路側管壁の管軸方向に抵
抗体を挿入したスリツトを設けたもので、以下図
面について詳細に説明する。
In order to eliminate these drawbacks, the present invention provides a slit in which a resistor is inserted in the tube axis direction of the tube wall on the coaxial line side of the choke for low frequency bands, and will be described in detail below with reference to the drawings.

第5図は、この発明の一実施例であつて、図中
1〜4は第1図中に示すものと同一である。7は
第1図中チヨークL6の同軸線路3側管壁に設け
た管軸方向に長いスリツトに抵抗体を挿入した抵
抗体入りスリツトであり、8は同軸線路3中を伝
搬するTEMモード波に対して動作するスリツト
付チヨークLである。なお、図中には示していな
いが、スリツト付チヨークL8と円形導波管4と
の間に第1図のチヨークH5が第1図と同様に設
けてある。抵抗体入りスリツト7の部分を拡大し
て示したものが第6図である。抵抗体入りスリツ
ト7は周方向に対称に4個設けている。
FIG. 5 shows an embodiment of the present invention, in which numerals 1 to 4 are the same as those shown in FIG. 7 is a resistor-containing slit in which a resistor is inserted into a long slit in the tube axis direction provided in the tube wall on the side of the coaxial line 3 of the yoke L6 in FIG. This is a slit-equipped cheese yoke L that operates against the slit. Although not shown in the figure, the yoke H5 shown in FIG. 1 is provided between the slitted yoke L8 and the circular waveguide 4 in the same manner as in FIG. FIG. 6 shows an enlarged view of the resistor-containing slit 7. Four resistor-containing slits 7 are provided symmetrically in the circumferential direction.

抵抗体入りスリツト7はスリツト付チヨークL
8に励振されるTEMモード波に対しては、スリ
ツトのある外壁に流れるTEMモード波の壁面電
流が管軸方向成分のみであることからほとんど影
響を与えない。しかし、抵抗体入りスリツト7は
スリツト付チヨークL8に励振されるTE11モー
ド波に対して外壁に流れるTE11モード波の壁面
電流の周方向成分に大きな減衰を与える作用を呈
する。
The slit 7 with a resistor is a chiyoke L with a slit.
8, the wall current of the TEM mode wave flowing through the outer wall with the slit has only a component in the direction of the tube axis, so it has almost no effect. However, the resistor-containing slit 7 has the effect of greatly attenuating the circumferential component of the wall current of the TE 11 mode wave flowing in the outer wall with respect to the TE 11 mode wave excited in the slit-equipped cheese yoke L8.

このため、スリツト付チヨークL8は、同軸線
路3の低周波数帯LのTEMモード波に対して
は、従来のチヨークL6と同様に良好な電気的特
性を呈し、円形導波管4の高周波数帯HのTE11
モード波に対しては、スリツト付チヨークL8内
に励振される同軸線路TE11モード波による伝送
特性の劣化をほとんど生じさせない。
Therefore, the slitted cheese yoke L8 exhibits good electrical characteristics similar to the conventional cheese yoke L6 for TEM mode waves in the low frequency band L of the coaxial line 3, and exhibits good electrical characteristics in the high frequency band L of the circular waveguide 4. HTE 11
Regarding mode waves, the coaxial line TE11 mode waves excited in the slitted cheese yoke L8 cause almost no deterioration in transmission characteristics.

したがつて、この2周波数帯共用導波管チヨー
クでは、LHの波の周波数比に関係なく、
LHの波に対するチヨーク形状をそれぞれ最適
となるように設計することができ、LHのい
ずれの波に対しても良好な電気的特性を得ること
ができる。
Therefore, in this two-frequency band shared waveguide choke, regardless of the frequency ratio of the L and H waves,
It is possible to design the chiyoke shape to be optimal for each of the L and H waves, and it is possible to obtain good electrical characteristics for both the L and H waves.

なお、以上はスリツトの数は4個の場合につい
て説明したが4個に限るものではなく、スリツト
の軸長は低周波数帯用チヨークの軸長より短くて
もよい。
In addition, although the case in which the number of slits is four has been described above, it is not limited to four, and the axial length of the slits may be shorter than the axial length of the choke for low frequency bands.

以上のように、この発明に係る2周波数帯共用
チヨークでは、低周波数帯用チヨークの外壁の管
軸方向に設けた抵抗体入りスリツトにより低周波
数帯用チヨーク内に励振された高周波数帯の
TE11モード波が減衰されるため、低周波数帯用
チヨークの最適設計をすることができ、低周波数
帯および高周波数帯の両帯域とも広帯域に良好な
電気的特性を呈するチヨークを得ることができる
利点がある。
As described above, in the dual-frequency band joint choke according to the present invention, the high frequency band excited in the low frequency band choke by the resistor-containing slit provided in the tube axis direction on the outer wall of the low frequency band choke.
Since the TE 11 mode wave is attenuated, it is possible to optimally design a cheese yoke for low frequency bands, and it is possible to obtain a cheese yoke that exhibits good electrical characteristics over a wide range of both low and high frequency bands. There are advantages.

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

第1図は従来の2周波数帯共用導波管チヨーク
の斜視図、第2図は第1図のチヨーク部分の断面
図、第3図は高周波数帯用チヨーク部分に励振さ
れる同軸線路TE11モード波を説明するための
図、第4図は、第3図中イ,ロ部分の断面図、第
5図はこの発明の一実施例の斜視図、第6図は、
第5図の吸収体入りスリツト部の拡大図である。 図中、1は内導体、2は外導体、3は同軸線
路、4は円形導波管、5はチヨークH、6はチヨ
ークL、7は抵抗体入りスリツト、8はスリツト
付チヨークLである。なお、図中同一あるいは相
当部分には同一符号を付して示してある。
Figure 1 is a perspective view of a conventional two-frequency band common waveguide chain, Figure 2 is a cross-sectional view of the chain section in Figure 1, and Figure 3 is a coaxial line TE 11 excited in the high frequency band station section. 4 is a sectional view of parts A and B in FIG. 3, FIG. 5 is a perspective view of an embodiment of the present invention, and FIG. 6 is a diagram for explaining mode waves.
FIG. 6 is an enlarged view of the slit portion containing the absorbent body in FIG. 5; In the figure, 1 is an inner conductor, 2 is an outer conductor, 3 is a coaxial line, 4 is a circular waveguide, 5 is a chain H, 6 is a chain L, 7 is a slit with a resistor, and 8 is a chain L with a slit. . It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.

Claims (1)

【特許請求の範囲】[Claims] 1 TEMモード波が伝搬する同軸線路の内導体
内にTE11モード波が伝搬する円形導波管を設け
た構造の伝送路の前記内導体に設けられ、かつ同
心状に組み合わせた前記TE11モード波用チヨー
クと前記TEMモード波用チヨークからなる2周
波数帯共用導波管チヨークにおいて、前記TEM
モード波用チヨークの前記同軸線路側壁面に管軸
方向に細長いスリツトを周方向に対称に複数個設
け、前記スリツト内に抵抗体を挿入したことを特
徴とする2周波数帯共用導波管チヨーク。
1. The TE 11 mode is provided in the inner conductor of a transmission line having a structure in which a circular waveguide in which the TE 11 mode wave propagates is provided in the inner conductor of the coaxial line in which the TEM mode wave propagates, and the TE 11 mode is combined concentrically. In the two-frequency band shared waveguide cheese consisting of a cheese for waves and a cheese for TEM mode waves, the TEM mode wave
A waveguide chain for dual frequency bands, characterized in that a plurality of slits elongated in the tube axis direction are provided symmetrically in the circumferential direction on the side wall surface of the coaxial line of the mode wave chain, and a resistor is inserted into the slits.
JP3217880A 1980-03-14 1980-03-14 Waveguide choke in common use with two frequency band Granted JPS56129402A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3217880A JPS56129402A (en) 1980-03-14 1980-03-14 Waveguide choke in common use with two frequency band

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3217880A JPS56129402A (en) 1980-03-14 1980-03-14 Waveguide choke in common use with two frequency band

Publications (2)

Publication Number Publication Date
JPS56129402A JPS56129402A (en) 1981-10-09
JPS6156882B2 true JPS6156882B2 (en) 1986-12-04

Family

ID=12351673

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3217880A Granted JPS56129402A (en) 1980-03-14 1980-03-14 Waveguide choke in common use with two frequency band

Country Status (1)

Country Link
JP (1) JPS56129402A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4656162B2 (en) 2008-02-19 2011-03-23 株式会社デンソー Waveguide choke structure

Also Published As

Publication number Publication date
JPS56129402A (en) 1981-10-09

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