JPS62190710A - High frequency magnetic field generator/detector - Google Patents
High frequency magnetic field generator/detectorInfo
- Publication number
- JPS62190710A JPS62190710A JP61031968A JP3196886A JPS62190710A JP S62190710 A JPS62190710 A JP S62190710A JP 61031968 A JP61031968 A JP 61031968A JP 3196886 A JP3196886 A JP 3196886A JP S62190710 A JPS62190710 A JP S62190710A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- variable capacitor
- frequency magnetic
- balanced
- field generator
- 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 20
- 239000003990 capacitor Substances 0.000 claims abstract description 38
- 239000004020 conductor Substances 0.000 claims description 17
- 238000001514 detection method Methods 0.000 claims description 3
- 230000005684 electric field Effects 0.000 description 3
- 238000005259 measurement Methods 0.000 description 2
- 238000005481 NMR spectroscopy Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
Landscapes
- 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
のである。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a high frequency magnetic field generation/detection device, particularly to a high frequency magnetic field generation/detection device used in a nuclear magnetic resonance apparatus.
第2図は例えば[ジャーナル・オブ・マグネティック・
レゾナンス(Journal of Magnetic
Resonance)J、第36巻、第447頁〜第4
51頁(1979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あり、図において(1)は
■字型をした1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)に対して対称的に配
置されたコイルであり、バーチカル・バンド(Vθrt
ical band)と呼ばれる非突出部(1a)およ
びウィング(wing)と呼ばれる突出部(1b)を有
している。(2)は隣接するウィング(1b)間に挿入
された固定コンデンサである。(Is)はウィング(1
b)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設置された電界シールド用の1
対の導体環であり、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(6b)がボト
ム・ガード・リングと呼ばれるO (41L)、(4t
l)はそれぞれ導体板(1)、導体環(3)と一体に形
成された電極である。(5a)、(5b)はこれら電極
(4a)、(ab)間に直列接続された整合用可変コン
デンサである。(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(5a)を介して電
極(4a)へ接続されかつ電極(4b)へ直結される。Figure 2 shows, for example, [Journal of Magnetics]
Resonance (Journal of Magnetic
Resonance) J, Vol. 36, pp. 447-4
This is a perspective view showing a conventional high-frequency magnetic field generator/detector shown on page 51 (1979). It is a coil arranged symmetrically with respect to a predetermined axis (not shown), and has a vertical band (Vθrt
It has a non-protruding part (1a) called an ical band and a protruding part (1b) called a wing. (2) is a fixed capacitor inserted between adjacent wings (1b). (Is) is a wing (1
b) 1 for electric field shielding installed on the inside of the cell via an insulating layer (not shown) and with the above-mentioned axis as a common center;
They are a pair of conductor rings, one conductor ring (3a) is called the top guard ring and the other conductor ring (6b) is called the bottom guard ring.
1) are electrodes formed integrally with a conductor plate (1) and a conductor ring (3), respectively. (5a) and (5b) are matching variable capacitors connected in series between these electrodes (4a) and (ab). (6) is a terminal connected to a transmitter/receiver (not shown), connected to the electrode (4a) via a variable capacitor (5a), and directly connected to the electrode (4b).
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)、コンデンサ(2)、導体環(6)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(4a)、(4b)間は容量結合され
ているので、可変コンデンサ(5a)、(5b)を追加
するこ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(5a)、(5b)によりインピ
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(′
6)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 constructed as described above, and the conductor plate (1), the capacitor (2), and the conductor ring (6) form a three-dimensional circuit that equivalently functions as an LC series resonant circuit. Furthermore, since the electrodes (4a) and (4b) are capacitively coupled, the resonance frequency can be adjusted by adding variable capacitors (5a) and (5b). Therefore, by matching the impedance using variable capacitors (5a) and (5b), it is possible to connect a transmitter/receiver having a predetermined impedance to the terminal (6). Note that the conductor ring (′
6) is used for electric field shielding as described above, that is, for reducing 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.
この発明に係る高周波磁場発生・検出器は隣接する1対
のウィングを容量結合する第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、この平衡型インビーダ
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 high frequency magnetic field generator/detector according to the present invention includes a first variable capacitor capacitively coupling a pair of adjacent wings, and a second variable capacitor connected to each end of the first variable capacitor.
A balanced impedance matching circuit including a variable capacitor and a third variable capacitor, and a balanced-unbalanced converter connected to the balanced impedance matching circuit are provided.
この発明において平衡型インピーダンス整合回路および
平衡不平衡変換器が隣接した1対のウィングに平衡給電
する。In this invention, a balanced impedance matching circuit and a balanced-unbalanced converter feed balanced power to a pair of adjacent wings.
第1図はこの発明の一実施例を示す斜視図であり、(1
)〜(3)および(6)は従来例と同じものである。FIG. 1 is a perspective view showing an embodiment of the present invention.
) to (3) and (6) are the same as in the conventional example.
ンス整合用の第1可変コンデンサであり、電極(7!L
)、(7b)間従って固定コンデンサ(2)で容量結合
されていない一対のウィング(1b)の電極(7a)、
(7b)間に接続される。(8b)、(fla)は第1
可変コンデンサ(8a)の各端にそれぞれ接続され、第
1可変コンデンサ(8a)と\もに平衡型インピーダン
ス整合回路(8)を構成する。(9)はこの平衡型イン
ピーダンス整合回路(8)の第2可変コンデンサ(at
))および第3可変コンデンサ(8C)に接続された平
衡不平衡変換器例えば2分の1波長の電気長を有する同
軸ケーブルである。(10)はボトム・ガード・リング
(5b)、第1可変コンデンサ(8a)および端子(6
)に接続されたアース線である。なお、バーチカル・バ
ンド(11L)のなす角度0は
80°(t(90゜
である。It is the first variable capacitor for performance matching, and the electrode (7!L
), (7b) between the electrodes (7a) of the pair of wings (1b) which are therefore not capacitively coupled by the fixed capacitor (2),
(7b) connected between. (8b), (fla) are the first
They are connected to each end of the variable capacitor (8a), and together with the first variable capacitor (8a) constitute a balanced impedance matching circuit (8). (9) is the second variable capacitor (at) of this balanced impedance matching circuit (8).
)) and a balanced-unbalanced converter connected to the third variable capacitor (8C), for example a coaxial cable with an electrical length of half a wavelength. (10) is the bottom guard ring (5b), the first variable capacitor (8a) and the terminal (6
) is the ground wire connected to the Note that the angle 0 formed by the vertical band (11L) is 80° (t (90°).
この発明においては、第1可変コンデンサ(8a)によ
り、等価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2可変コンデンサ(8″b)および第3
可変コンデンサ(8C)を平衡減に配置しかつ平衡不平
衡変換器(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(
7b)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。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以上のよ
う暑こ、この発明は1対の突出部を容量結合する第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ある。In this invention, the first variable capacitor (8a) adjusts the resonance frequency and impedance matching frequency of the three-dimensional circuit that functions as an equivalent series resonant circuit. In addition to this, a second variable capacitor (8″b) and a third
By arranging the variable capacitor (8C) in a balanced manner and using the balanced/unbalanced converter (9), when a coaxial cable and transmitter/receiver with unbalanced impedance are connected to the terminal (6), the maximum power can be delivered to the load. can be supplied, and the detected power is also maximized. In this case, the electrode (7a) and (
Since voltages of equal magnitude and opposite polarity are applied to 7b), the LC series resonant circuit is completely balancedly fed. This can increase the stability and efficiency of the high-frequency magnetic field generator/detector.By installing a conductor cylinder, that is, a metal cylinder, for electromagnetic shielding, the loss of the LC resonant circuit can be reduced. A balanced impedance matching circuit consisting of a first variable capacitor that capacitively couples the protrusion, a second variable capacitor and a third variable capacitor connected to each end of the first variable capacitor, and a balanced impedance matching circuit connected to the balanced impedance matching circuit. Since a balanced unbalanced converter is 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、そして第2
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、(1′b)はウィング、(2)は固定
コンデンサ、(8a)は第1可変コンデンサ、(8b)
は第2可変コンデンサs (a’)は第3可変コンデン
サ、(8)は平衡型インピーダンス整合回路、(9)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。
帛1図
スn
帛2図
手続補正書「自発」
■8塊1.現、−υ、 ■FIG. 1 is a perspective view showing one embodiment of the present invention, and FIG.
The figure is a perspective view showing a conventional high-frequency magnetic field generator/detector. (1) is a conductor plate, (1'b) is a wing, (2) is a fixed capacitor, (8a) is the first variable capacitor, (8b)
is a second variable capacitor s (a') is a third variable capacitor, (8) is a balanced impedance matching circuit, and (9) is a balanced-unbalanced converter. In addition, in the figures, the same reference numerals indicate the same or equivalent parts. Figure 1 Sn Figure 2 Procedural Amendment “Spontaneous” ■8 blocks 1. Current, −υ, ■
Claims (4)
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、これら突出部のうち少なくとも3対を
固定コンデンサで容量結合するとゝもに残る1対の突出
部を第1可変コンデンサで容量結合し、もって等価的に
LC共振回路を構成する立体回路と、前記第1可変コン
デンサ並びにそ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 at least three pairs of these protrusions are fixed capacitors. When capacitively coupled, a pair of remaining protrusions are capacitively coupled by a first variable capacitor, thereby forming a three-dimensional circuit that equivalently constitutes an LC resonant circuit, and a three-dimensional circuit connected to the first variable capacitor and each end thereof, respectively. A high frequency magnetic field generator/detector comprising: a balanced impedance matching circuit including a second variable capacitor and a third variable capacitor; and a balanced/unbalanced converter connected to the balanced impedance matching 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
導体環を含み、少なくとも1方の導体環をアース電位に
した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) A three-dimensional circuit includes a pair of conductor rings installed inside a protrusion of a conductor plate with an insulating layer in between and a predetermined axis as a common center, and at least one conductor ring is connected to a ground potential. A high-frequency magnetic field generator/detector according to claim 1, characterized in that:
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.
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61031968A JPS62190710A (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 |
---|---|---|---|
JP61031968A JPS62190710A (en) | 1986-02-18 | 1986-02-18 | High frequency magnetic field generator/detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62190710A true JPS62190710A (en) | 1987-08-20 |
Family
ID=12345751
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61031968A Pending JPS62190710A (en) | 1986-02-18 | 1986-02-18 | High frequency magnetic field generator/detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62190710A (en) |
-
1986
- 1986-02-18 JP JP61031968A patent/JPS62190710A/en active Pending
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