JPS62190711A - High frequency magnetic field generator/detector - Google Patents
High frequency magnetic field generator/detectorInfo
- Publication number
- JPS62190711A JPS62190711A JP61031969A JP3196986A JPS62190711A JP S62190711 A JPS62190711 A JP S62190711A JP 61031969 A JP61031969 A JP 61031969A JP 3196986 A JP3196986 A JP 3196986A JP S62190711 A JPS62190711 A JP S62190711A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- frequency magnetic
- variable capacitor
- field generator
- 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.)
- Pending
Links
- 230000005291 magnetic effect Effects 0.000 title claims abstract description 25
- 239000003990 capacitor Substances 0.000 claims abstract description 41
- 239000004020 conductor Substances 0.000 claims abstract description 30
- 230000008878 coupling Effects 0.000 claims description 3
- 238000010168 coupling process Methods 0.000 claims description 3
- 238000005859 coupling reaction Methods 0.000 claims description 3
- 238000001514 detection method Methods 0.000 claims 1
- 238000005476 soldering Methods 0.000 claims 1
- 230000005611 electricity Effects 0.000 abstract 1
- 230000004048 modification Effects 0.000 description 4
- 238000012986 modification Methods 0.000 description 4
- 230000005684 electric field Effects 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 238000005481 NMR spectroscopy Methods 0.000 description 1
- 241001080526 Vertica Species 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002966 varnish Substances 0.000 description 1
- 230000002747 voluntary effect Effects 0.000 description 1
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- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、高周波磁場発生・検出器、特に核磁気共鳴
装置に用いられる高周波磁場発生・検出器に関するもの
でるる。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high frequency magnetic field generator/detector, particularly to a high frequency magnetic field generator/detector used in a nuclear magnetic resonance apparatus.
第夕図は例えば[ジャーナル・オプ・マグネティック・
レゾナンス(Journal of Magnetic
Resonance)J 、第36巻、第1IIIり頁
〜第1II/頁(tqqq年)に示されている従来の高
周波磁場発生・検出器を示す斜視図でおり、図において
(1)はH字型をしたl対の導体板例えば銅板を円筒状
に構成すると\もに所定の軸(図示しない)K対して対
称的に配置されたコイルでめり、バーチカル・バンド(
vertica:L band)と呼ばれる非突出部(
la)およびウィング(wing)と呼ばれる突出部(
tb)を有している。(2)は隣接するウィング(lb
)間に挿入された固定コンデンサでおる。(3)はウィ
ング(lb)の内側に絶縁層(図示しない)を介してか
つ上述した軸を共通の中心として配置された電界シール
ド用のl対の導体環でおり、一方の導体環(3a)がト
ップ・ガード・リングと呼ばれかつ他方の導体環(3b
)がボトム・ガード・リングと呼ばれる。(4(a)
、 (#b)はそれぞれ導体板O)、導体環(3)と一
体に形成された電極である。(りa)。The evening map is, for example, [Journal of Magnetics]
Resonance (Journal of Magnetic
This is a perspective view showing a conventional high-frequency magnetic field generator/detector shown in Resonance) J, Vol. When a pair of conductor plates, such as a copper plate, are arranged in a cylindrical shape, they are bent by coils arranged symmetrically with respect to a predetermined axis (not shown) K, resulting in a vertical band (
vertica: non-protruding part (L band)
la) and protrusions called wings (
tb). (2) is the adjacent wing (lb
) with a fixed capacitor inserted between them. (3) is a pair of conductor rings for electric field shielding arranged inside the wing (lb) via an insulating layer (not shown) and with the above-mentioned axis as a common center; one conductor ring (3a ) is called the top guard ring and the other conductor ring (3b
) is called the bottom guard ring. (4(a)
, (#b) are electrodes formed integrally with the conductor plate O) and the conductor ring (3), respectively. (Ria).
(りb)はこれら電極r+a)、nb)間に直列接続さ
れた整合用可変コンデンサでらる。(6)は送受信器(
図示しない)と接続される端子であり、可変コンデンサ
(りa)を介して電極(lIa)へ接続されかつ電極(
ib )へ直結される。(b) is a matching variable capacitor connected in series between these electrodes r+a) and nb). (6) is the transmitter/receiver (
This terminal is connected to the electrode (lIa) via the variable capacitor (ria) and is connected to the electrode (lIa) via the variable capacitor (lia).
ib).
従来の高周波磁場発生・検出器は上述したように構成さ
れ、導体板(1)、固定コンデンサ(2)、導体環(3
)が等価的にLC直列共振回路として働く立体回路を形
成する。さらに、電極(<za)、(lIb)間は容量
結合されているので、可変コンデンサ(ta)、(tb
)を追加するととにより共振周波数を調整することがで
きる。従って、可変コンデンサ(rag、(りb)によ
ジインピーダンスを整合すれば、所定のインピーダンス
を有する送受信器と端子(6)を接続できる。なお、導
体環(3)は上述したように電界シールドのため、即ち
高周波磁場発生・検出器内に測定対象を設置した場合に
発生電界による測定対象内の誘電損失を低減するために
用いられる。A conventional high-frequency magnetic field generator/detector is configured as described above, and includes a conductor plate (1), a fixed capacitor (2), and a conductor ring (3).
) forms a three-dimensional circuit that equivalently functions as an LC series resonant circuit. Furthermore, since the electrodes (<za) and (lIb) are capacitively coupled, the variable capacitors (ta) and (tb
) can be used to adjust the resonant frequency. Therefore, by matching the diimpedance with a variable capacitor (rag, (rib)), a transmitter/receiver having a predetermined impedance can be connected to the terminal (6).The conductor ring (3) is used as an electric field shield as described above. Therefore, it is used to reduce dielectric loss within the measurement object due to the generated electric field when the measurement object is installed in a high-frequency magnetic field generator/detector.
従来の高周波磁場発生・検出器では、回路インピーダン
スの平衡不平衡変換が考慮されていないので、端子に接
続する同軸ケーブルに同相電流が流れて動作が不安定に
なると\もに低効率になるなどの問題点があった。Conventional high-frequency magnetic field generators and detectors do not take into account the balance-unbalance conversion of circuit impedance, so if a common-mode current flows through the coaxial cable connected to the terminal and the operation becomes unstable, the efficiency will decrease. There was a problem.
この発明はこのような問題点を解決するためになされた
もので、回路インピーダンスの平衡不平衡性を考慮し、
安定で効率の良い高周波磁場発生・検出器を得ることを
目的とする。This invention was made to solve these problems, and takes into account the balance and unbalance of circuit impedance.
The aim is to obtain a stable and efficient high-frequency magnetic field generator/detector.
突出部を切断して2分し、この−分した非突出部間に接
続された第7可変コンデンサ並びにこの第1可変コンデ
ンサの各端にそれぞれ接続された第2可変コンデンサお
よび第3可変コンデンサからなる平衡型インピーダンス
整合回路と、この平衡型インピーダンス整合回路に接続
された平衡不平衡変換器とを設けたものである。The protruding part is cut into two parts, and a seventh variable capacitor is connected between the divided non-protruding parts, and a second variable capacitor and a third variable capacitor are respectively connected to each end of the first variable capacitor. This system includes a balanced impedance matching circuit and a balanced-unbalanced converter connected to the balanced impedance matching circuit.
この発F!Aにおいて、平衡型インピーダンス整合回路
および平衡不平衡変換器は、2分された非突出部に平衡
給電する。This departure F! In A, the balanced impedance matching circuit and the balanced unbalanced converter supply balanced power to the bisected non-protruding portion.
第1図はこの発明の一実施例を示す斜視図でめシ、従来
例と同様に/対の導電体(1)がおり、その突出部即ち
ウィング(tb)同士を近接させた後、これらウィング
(tb)を電気的に接続する、即ち本実施例では従来例
と同様に固定コンデンサ(2)で容量結合することによ
り、立体回路が構成される。たソし、従来例と違って、
この発明ではl対の導体板(1)のうち!方の導体板例
えば第1図において右側の導体板はその非突出部即ちバ
ーチカル・バンドr/a)が切断、部分され、2分され
たバーチカル・バンド(/a)が電極(7a)、r7b
)になる。(ga)はLC直列共振回路用かつインピー
ダンス整合用の第1可変コンデンサでろり、電極(?a
)、r7b)間に接続される。(tb)、(gc)は第
1可変コンデンサ(ta)の各端にそれぞれ接続され、
第1可変コンデンサ(ta)と\もに平衡型インピーダ
ンス整合回路(1)を構成する。(9)はこの平衡型イ
ンピーダンス整合回路(1)の第λ可変コンデンサ(t
b)および第3可変コンデンサ(gc)に接続された平
衡不平衡変換器例えば部分のl波長の電気長を有する同
軸ケーブルである。なお、バーチカル・バンド(ta)
のなす角度θはざ0°〈θ〈900である。FIG. 1 is a perspective view showing an embodiment of the present invention. As in the conventional example, there is a pair of conductors (1), whose protrusions or wings (tb) are brought close to each other, and then these A three-dimensional circuit is constructed by electrically connecting the wings (tb), that is, in this embodiment, by capacitively coupling them with a fixed capacitor (2) as in the conventional example. However, unlike the conventional example,
In this invention, among l pairs of conductor plates (1)! For example, in the conductor plate on the right side in FIG.
)become. (ga) is the first variable capacitor for the LC series resonant circuit and impedance matching, and the electrode (?a
), r7b). (tb) and (gc) are respectively connected to each end of the first variable capacitor (ta),
Together with the first variable capacitor (ta), a balanced impedance matching circuit (1) is constructed. (9) is the λ-th variable capacitor (t) of this balanced impedance matching circuit (1).
b) and a balanced-unbalanced converter connected to a third variable capacitor (gc), for example a coaxial cable with an electrical length of 1 wavelength of the section. In addition, vertical band (ta)
The angle θ formed by this is 0°〈θ〈900.
この発明においては、第1可変コンデンサ(ta)によ
り、等測的な直列共振回路として働く立体回路の共振周
波数およびインピーダンス整合用周波数を調節する。こ
れに加えて、第λ可変コンデンサ(tb)および第3可
変コンデンサ(tc )を平衡型に配置しかつ平衡不平
衡型変換器(9)を用いることにより、不平衡インピー
ダンスをもつ同軸ケーブルおよび送受信器を端子(6)
に結合したとき、負荷に最大の電力を供給でき、また検
出される電力も最大となる。この場合、電極(7a)と
(りb)には大きさが等しくて極性が逆の電圧が印加さ
れるので、LC直列共振回路は完全に平衡給電される。In this invention, the first variable capacitor (ta) adjusts the resonant frequency and impedance matching frequency of the three-dimensional circuit that functions as an isometric series resonant circuit. In addition, by arranging the λ-th variable capacitor (tb) and the third variable capacitor (tc) in a balanced manner and using a balanced-unbalanced converter (9), the coaxial cable with unbalanced impedance and the transmitting/receiving Connect the device to the terminal (6)
When coupled to , the maximum power can be delivered to the load and the maximum power sensed. In this case, voltages of equal magnitude and opposite polarity are applied to the electrodes (7a) and (rib), so that the LC series resonant circuit is completely balanced.
これが高周波磁場発生・検出器の安定度、効率を高くで
きる理由となる。なお、図示しないが、この発明の高周
波磁場発生・検出器の外側に、共通の中心軸を有する電
磁シールド用の導体筒すなわち金属円筒を設置すること
により、LC共振回路の損失が減少し、発生する高周波
磁場の空間均一度が向上する。This is the reason why the stability and efficiency of the high-frequency magnetic field generator/detector can be increased. Although not shown, by installing an electromagnetic shielding conductor tube, that is, a metal cylinder having a common central axis, outside the high-frequency magnetic field generator/detector of the present invention, the loss of the LC resonant circuit is reduced, and the generated The spatial uniformity of the high-frequency magnetic field is improved.
第2図は第1図に示した実施例の変形例を示す斜視図で
あり、一対の導体板(1)および平衡不平衡変換器(9
)を使用した例である。FIG. 2 is a perspective view showing a modification of the embodiment shown in FIG.
) is used.
第3図はこの発明の他の実施例を示す斜視図であり、第
1図に示した実施例とは突出部即ちウィング(lb)の
電気的接続の仕方が違い、固定コンデンサ(2)で容量
結合する代シに、圧接または半田付けでウィング(tb
)を電気的に接続している。FIG. 3 is a perspective view showing another embodiment of the present invention, which differs from the embodiment shown in FIG. 1 in the way the protrusion or wing (lb) is electrically connected, and is a fixed capacitor (2). A wing (tb
) are electrically connected.
なお1図示しないが、固定コンデンサ(,2)で容量結
合する代りに、導線や導体を用いてウィング(tb)を
電気的に接続しても良い。Although not shown in FIG. 1, the wings (tb) may be electrically connected using conductive wires or conductors instead of capacitively coupling with the fixed capacitors (, 2).
第を図は第3図に示した実施例の変形例を示す斜視図で
あり、第2図と同様のものでるる。The second figure is a perspective view showing a modification of the embodiment shown in FIG. 3, and is similar to that in FIG. 2.
〔発明の効果〕
分し、この部分した非突出部間に接続された第1可変コ
ンデンサ並びKこの第1可変コンデンサの各端にそれぞ
れ接続された第コ可変コンデンサおよび第3可変コンデ
ンサからなる平衡型インピーダンス整合回路と、この平
衡型インピーダンス整合回路に接続された平衡不平衡変
換器とを設けたので、安定度および効率の良い高周波磁
場発生・検出器が得られる効果がろる。[Effects of the Invention] A balanced structure consisting of a first variable capacitor connected between the non-protruding parts, a first variable capacitor connected to each end of the first variable capacitor, and a third variable capacitor connected to each end of the first variable capacitor. Since the balanced type impedance matching circuit and the balanced/unbalanced converter connected to the balanced type impedance matching circuit are provided, it is possible to obtain a highly stable and efficient high frequency magnetic field generator/detector.
第1図はこの発明の一実施例を示す斜視図、第2図は第
1図に示した実施例の変形例を示す斜視図、第3図はこ
の発明の他の実施例を示す斜視図、第グ図は第3図に示
した実施例の変形例を示す斜視図、そして第1図は従来
の高周波磁場発生・検出器を示す斜視図である。
(1)は導体板、(/a)はバーチカル・バンド、(t
b)はウィング、(2)は固定コンデンサ、(ra)は
第1可変コンデンサ、(llb)は第コ可変コンデンサ
、(tc)は第3可変コンデンサ、(1)は平衡壓イン
ピーダンス整合回路、(テ)は平衡不平衡変換器である
。
なお、図中、同一符号は同一、又は相当部分を示す。
1 ;導体板
1Q 、 バーテウルバシド
1b ° ウィンr
2 ・ 国史コ5テ゛2“ワ。
3 、導体環
8 ゛ 平衡型仁C′−タ”ニス堅冶l可b8o ・
牙1 可豪フ〉テ゛′−サ
8b : 第2可茨コシデ゛ニサ
8C: 牙37T嘔t:lシテーンリ
9 、千f#!Tイ千イiFrg:梗答壓2図
手続補正書(自発)
1.事件の表示
昭和61年特許願第 51969 号2、発明の名称
高周波磁場発生・検出器
3、補正をする者
代表者志岐守哉
4、代理人
6、補正の内容
(1)明細書第6ページ第13行の「導電体(1)」の
記載を「導体板(1)」と補正する。
(2)明細書第7ページ第13行の「角度θは」の記載
の後に[70°〈θ<100’であり、好ましくは」を
挿入する。
(3)明細書第8ページ第15行の「および」の記載の
後に「2個の」を挿入する。
(4)明細書第4ページ第6行と第7行の間に下記の記
載を挿入する。
「第3図および第4図には導体環(3)がある場合を示
したが、導体環(3)はなくても良い。
また、第2図および第4図の構成において、給電を1箇
所から行う場合は、平衡型インピーダンス整合回路(8
)、平衡不平衡変換機(9)を1組とし、他を可変コン
デンサで終端して調整することにしてもよい。」FIG. 1 is a perspective view showing one embodiment of this invention, FIG. 2 is a perspective view showing a modification of the embodiment shown in FIG. 1, and FIG. 3 is a perspective view showing another embodiment of this invention. , Fig. 3 is a perspective view showing a modification of the embodiment shown in Fig. 3, and Fig. 1 is a perspective view showing a conventional high frequency magnetic field generator/detector. (1) is a conductor plate, (/a) is a vertical band, (t
b) is a wing, (2) is a fixed capacitor, (ra) is a first variable capacitor, (llb) is a third variable capacitor, (tc) is a third variable capacitor, (1) is a balanced impedance matching circuit, ( Te) is a balanced-unbalanced converter. In addition, in the figures, the same reference numerals indicate the same or equivalent parts. 1; Conductor plate 1Q, Verteurbacid 1b ° Win r 2. National history piece 5 tier 2"W. 3, Conductor ring 8" Balanced type Ni C'-ta" varnish hardening lable b8o.
Fang 1 Kagofu〉Te゛'-sa 8b: 2nd Kagoshidden Nisa 8C: Fang 37T t: l city 9, 1,000 f#! TI 1000 iFrg: 2nd figure procedural amendment (voluntary) 1. Display of the case Patent Application No. 51969 of 1985 2, Name of the invention High frequency magnetic field generator/detector 3, Person making the amendment Representative Moriya Shiki 4, Agent 6, Contents of the amendment (1) Page 6 of the specification The description of “conductor (1)” in line 13 is corrected to “conductor plate (1)”. (2) Insert "[70°<θ<100', preferably"] after the statement "Angle θ is" on page 7, line 13 of the specification. (3) Insert "two" after the statement "and" on page 8, line 15 of the specification. (4) Insert the following statement between lines 6 and 7 on page 4 of the specification. "Although Figures 3 and 4 show the case where there is a conductor ring (3), the conductor ring (3) may not be provided. Also, in the configurations of Figures 2 and 4, the power supply is When performing from a point, a balanced impedance matching circuit (8
), the balance/unbalance converter (9) may be used as one set, and the other may be terminated with a variable capacitor for adjustment. ”
Claims (7)
に対して対称的に配置し、前記導体板の突出部同士を近
接させた後、これら突出部を電気的に接続して構成され
た立体回路と、前記少なくとも1対の導体板のうち各対
の1方の導体板の非突出部を切断して2分し、この2分
した非突出部間に接続された第1可変コンデンサ並びに
この第1可変コンデンサの各端にそれぞれ接続された第
2可変コンデンサおよび第3可変コンデンサからなる平
衡型インピーダンス整合回路と、この平衡型インピーダ
ンス整合回路に接続された平衡不平衡変換器とを備え、
前記立体回路が前記第1可変コンデンサとゝもに等価的
にLC直列共振回路を構成したことを特徴とする高周波
磁場発生・検出器。(1) At least one pair of H-shaped conductor plates is arranged symmetrically with respect to a predetermined axis, the protrusions of the conductor plates are brought close to each other, and then these protrusions are electrically connected. The constructed three-dimensional circuit and the at least one pair of conductive plates are divided into two by cutting the non-protruding part of one of the conductive plates of each pair, and a first A balanced impedance matching circuit comprising a variable capacitor, a second variable capacitor and a third variable capacitor connected to each end of the first variable capacitor, and a balanced unbalanced converter connected to the balanced impedance matching circuit. Equipped with
A high frequency magnetic field generator/detector, characterized in that the three-dimensional circuit and the first variable capacitor equivalently constitute an LC series resonant circuit.
してかつ所定の軸を共通の中心として設置された1対の
導体環を含むことを特徴とする特許請求の範囲第1項記
載の高周波磁場発生・検出器。(2) The three-dimensional circuit includes a pair of conductor rings installed inside the protruding portion of the conductor plate with an insulating layer interposed therebetween and having a predetermined axis as a common center. High-frequency magnetic field generator/detector described in Section 1.
とする導体筒を有することを特徴とする特許請求の範囲
第1項または第2項記載の高周波磁場発生・検出器。(3) The high-frequency magnetic field generator/detector according to claim 1 or 2, wherein the three-dimensional circuit has a conductor tube having a predetermined axis as its central axis on the outside of the conductor plate.
する同軸ケーブルであることを特徴とする特許請求の範
囲第1項ないし第3項のいずれか記載の高周波磁場発生
・検出器。(4) High-frequency magnetic field generation and detection according to any one of claims 1 to 3, wherein the balanced-unbalanced converter is a coaxial cable having an electrical length of 1/2 wavelength. vessel.
量結合であることを特徴とする特許請求の範囲第1項な
いし第4項のいずれか記載の高周波磁場発生・検出器。(5) The high frequency magnetic field generator/detector according to any one of claims 1 to 4, wherein the electrical connection of the protrusion is capacitive coupling using a fixed capacitor.
ることを特徴とする特許請求の範囲第1項ないし第4項
のいずれか記載の高周波磁場発生・検出器。(6) The high frequency magnetic field generator/detector according to any one of claims 1 to 4, wherein the electrical connection of the protrusion is by pressure contact or soldering.
とを特徴とする特許請求の範囲第1項ないし第4項のい
ずれか記載の高周波磁場発生・検出器。(7) The high-frequency magnetic field generator/detector according to any one of claims 1 to 4, wherein the electrical connection of the protrusion is by a conducting wire or a conductor.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61031969A JPS62190711A (en) | 1986-02-18 | 1986-02-18 | High frequency magnetic field generator/detector |
US07/013,901 US4755756A (en) | 1986-02-18 | 1987-02-12 | Radio frequency coil for nuclear magnetic resonance imaging |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61031969A JPS62190711A (en) | 1986-02-18 | 1986-02-18 | High frequency magnetic field generator/detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62190711A true JPS62190711A (en) | 1987-08-20 |
Family
ID=12345780
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61031969A Pending JPS62190711A (en) | 1986-02-18 | 1986-02-18 | High frequency magnetic field generator/detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62190711A (en) |
-
1986
- 1986-02-18 JP JP61031969A patent/JPS62190711A/en active Pending
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