JPS6353906A - Radio frequency magnetic field generating detector - Google Patents
Radio frequency magnetic field generating detectorInfo
- Publication number
- JPS6353906A JPS6353906A JP61197582A JP19758286A JPS6353906A JP S6353906 A JPS6353906 A JP S6353906A JP 61197582 A JP61197582 A JP 61197582A JP 19758286 A JP19758286 A JP 19758286A JP S6353906 A JPS6353906 A JP S6353906A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- variable capacitor
- frequency magnetic
- field generator
- balanced
- 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
- 239000003990 capacitor Substances 0.000 claims abstract description 38
- 239000004020 conductor Substances 0.000 claims description 18
- 238000010168 coupling process Methods 0.000 abstract description 2
- 238000005859 coupling reaction Methods 0.000 abstract description 2
- 230000008878 coupling Effects 0.000 abstract 1
- 238000000034 method Methods 0.000 abstract 1
- 230000005684 electric field Effects 0.000 description 3
- 230000005540 biological transmission Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
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、特に該磁気共鳴
装置に用いられる高周波磁場発生・検出器に関するもの
であろう
〔従来の技術〕
第4図は例えば[ジャーナル・オブ・マグネテ(ツクー
L’シー1− ンス(Journal of Magn
eticResonance)J、第36巻、第447
頁〜第451頁(1979年)に示されヱいる従来の高
周波磁場発生・検出器を示す斜視図であり1図において
(1)は8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)に対し又対
称的に配置されたコイルであり、バーチカル・ハンド(
vertical band)と呼ばれる非突出部(L
a)およびウィング(wing )と呼ばれる突出部Q
b)を有しt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めるう(3)はウィン
グ(1b)の内側に絶縁N(図示しない)を介し王かつ
t述した軸を共通の中心とじt設置された電界シールド
用の1対の導体環であり、−万の導体環(3a)がトッ
プ・ガード・リングと呼ばれかつ他方の導K[(3b)
がボトム・ガード・リングと呼ばれる。[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a high frequency magnetic field generator/detector, particularly a high frequency magnetic field generator/detector used in the magnetic resonance apparatus [Prior Art] Figure 4 is, for example, the Journal of Magnet (Journal of Magnet).
eticResonance) J, Volume 36, No. 447
This is a perspective view showing a conventional high-frequency magnetic field generator/detector shown in pages 1 to 451 (1979). When configured as above, the coils are arranged symmetrically with respect to a predetermined axis (not shown), and the vertical hand (
The non-protruding part (L
a) and a protrusion Q called a wing
b) has t. (2) is the adjacent wing (1b)
A fixed capacitor inserted between the capacitors (3) and 1 for electric field shielding is installed on the inside of the wing (1b) via an insulator N (not shown) and with the axes mentioned above at the common center. The conductor ring (3a) is called the top guard ring, and the other conductor ring (3b) is a pair of conductor rings.
is called the bottom guard ring.
(4a)、(4b)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) 、(5
b)はこれら電極(4a) 、(4b)間に直列接続さ
れた整合用可変コンデンサでめるっ(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)を介し又電極(4a)へ接続されかつQ[(4
b)へ直結されろう従来の高周波磁場発生・検出器はと
述したように構成され、導体板(1)、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
く立木回路を形成する、さらに、電極(4a)、(4b
)間は各量結合されτ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。従つt、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
ろうなお、導体環(3)はと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。(4a) and (4b) are the conductor plate (1) and the conductor ring (
3) is an electrode formed integrally with the electrode. (5a), (5
b) is a matching variable capacitor connected in series between these electrodes (4a) and (4b), and (6) is a transmitter/receiver (
Q [(4
The conventional high-frequency magnetic field generator/detector that will be directly connected to
), the conductor ring (3) forms a standing tree circuit that functions equivalently as an LC series resonant circuit, and furthermore, the electrodes (4a), (4b
) are coupled by each amount τ, so the variable capacitor (5a
), (5b) can be added to adjust the resonance frequency. t, variable capacitor (5a),
If the impedance is matched using (5b), it will be possible to connect the transmitter/receiver with a predetermined impedance to the terminal (6).As mentioned above, the conductor ring (3) is used for electric field shielding, i.e., for generating and detecting high frequency magnetic fields. It is used to reduce dielectric loss within the measurement object due to the generated electric field when the measurement object is installed inside the instrument.
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t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っ
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属し、
安定で効率の良い高周波磁場発生・検出器を得ることを
目的とするう
また6全身用の高周波コイルが円筒型の場合、送信磁場
発生の効率が低く、また受信信号のい(Signal
to No1se Rat io )が比較的小さいな
どの問題があった。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. This invention, which had some problems, was made in order to solve these problems.
Aiming to obtain a stable and efficient high-frequency magnetic field generator/detector 6 If the high-frequency coil for the whole body is cylindrical, the efficiency of transmitting magnetic field generation is low, and the reception signal is
There were problems such as a relatively small ratio (to No.1se Ratio).
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Gt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&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
のでめるつ
また。全身用の高周波コイルの形を楕円型にするう
〔作 用〕
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結電
する。The high frequency magnetic field generator/detector according to the present invention includes a first variable capacitor Gt-coupling a pair of adjacent wings, and a second variable capacitor connected to each end of the first variable capacitor.
A mermetal bridge is provided with a balanced impedance matching circuit consisting of a variable capacitor and a third variable capacitor, and a balanced unbalanced converter connected to this balanced impedance matching circuit. To make the shape of the whole body high-frequency coil elliptical [Operation] In the present invention, a balanced impedance matching circuit and a balanced unbalanced converter are balancedly connected to a pair of adjacent wings.
また、全身用の高周波コイルを楕円型にすることにより
、送信磁場発生の効率や受信信号のS/Nが面立する。Furthermore, by making the high-frequency coil for the whole body into an elliptical shape, the efficiency of generating the transmitting magnetic field and the S/N of the received signal are improved.
第1図はこの発明の第1の実施例を示す斜視図であり、
高周波コイルが円筒型の場合であり、(1)〜(3)お
よび(6)は従来りと同じものであるo (7a)。FIG. 1 is a perspective view showing a first embodiment of the invention,
This is the case where the high frequency coil is cylindrical, and (1) to (3) and (6) are the same as conventional ones. (7a).
(7b)は各4本数(1)の隣接するウィング(lb)
と一体に形成された電極であるう(8a)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
サであり、電極(7a)、(7b)間従りt固定コンデ
ンサ(21で6量結合されτいない一対のウィング(1
b)の電極(7a)、(7b)間に接続される。(8b
) 、(sc ) ハ第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(8b)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。GOはボト
ム・ガード・リング(3b)、第1可変コンデンサ(8
a)および端子(6)に接続されたアース線でろる口な
お、バーチカル・バンド(la)のなす角度θハフ0°
〈θく1000で好ましくは75°くθく900 でめ
る。(7b) each has four (1) adjacent wings (lb)
The electrode (8a) formed integrally with the electrode (8a) is the first variable capacitor for the LC series resonant circuit and impedance matching. A pair of wings (1
b) is connected between the electrodes (7a) and (7b). (8b
), (sc) are respectively connected to each end of the first variable capacitor (8a), and together with the first variable capacitor (8a) constitute a balanced impedance matching circuit (8). (9) is a balanced unbalanced converter connected to the second variable capacitor (8b) and the third variable capacitor (8C) of this balanced impedance matching circuit (8),
It is a coaxial cable with an electrical length of wavelength. GO is the bottom guard ring (3b), the first variable capacitor (8
a) and the ground wire connected to terminal (6). Note that the angle θ huff 0° formed by the vertical band (la) is
(preferably 75° x 900).
第2.3図はこの発明の第2.第3実施例を示す斜視図
であり、高周波コイルが楕円の筒型の場合であり、(1
)〜(11mは第1の実施例と同じものである。第2図
におい又はバーチカル・バンドは楕円の短径方向に配置
されtいる例であり、第3図は長径方向に配置され又い
る例である。Figure 2.3 is the second example of this invention. FIG. 7 is a perspective view showing a third embodiment, in which the high-frequency coil has an elliptical cylindrical shape;
) to (11m are the same as in the first embodiment. In Fig. 2, the vertical band is arranged in the short axis direction of the ellipse, and in Fig. 3, the vertical band is arranged in the long axis direction. This is an example.
この発明におい又は、第1可変コンデンサ(8a)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1.第2可変コンデンサ(8b)および第3可
変コンデンサ(8C)を平衡型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(7
b)には大きさが等しくt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ろうこ
れが高周波磁場発生・検出器の安定度、効率を高くでき
る理由となろうなお、図示しないが、この発明の高周波
磁場発生・検出器は導体板の外側に、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鵬円筒を設置す
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とするうなお、導体板は2
対以を使用しても良い口
また、全身用の円筒型の高周波磁場発生・検出器は大型
になり、送信磁場発生の効率または受信信号のS/Nが
小さくなる5人間の木の断面はほぼ楕円形であるので、
高周波磁場発生・検出器を円筒の直径が長径となるより
な楕円筒にすることができる。これにより、円筒の場合
に比べ2高い磁場発生の効率となり受信信号のS/Nも
向tする。列えば64MHzに対し又は2円筒の場合に
比較しヱだ円形では同一の送信電力の場合60〜70%
送信磁場が増加することが実験により判明したう
また、楕円の長径方向が水平になるようにRFコイルを
設置した時に矢印で示すように高周波磁場を水平又は鉛
直方向に発生させるかにより、それぞれバーチカルパン
トを短径方向、長径方向に配置する。Alternatively, in this invention, the first variable capacitor (8a) adjusts the resonant frequency and impedance matching frequency of the three-dimensional circuit that functions as an isometric series resonant circuit. In addition to this, 1. By arranging the second variable capacitor (8b) and the third variable capacitor (8C) in a balanced manner and using a balanced-unbalanced converter (9), a coaxial cable and a transmitter/receiver with unbalanced impedance can be connected to the terminal (6). When coupled to , the maximum power can be delivered to the load and the maximum power sensed. In this case, electrodes (7a) and (7
Since voltages of equal magnitude and opposite polarity are applied to b), the LC series resonant circuit will be fed with completely balanced power.This may be the reason why the stability and efficiency of the high frequency magnetic field generator/detector can be increased. Although not shown, the high-frequency magnetic field generator/detector of the present invention reduces the loss of the LC resonant circuit by installing a conductor tube for electromagnetic shielding, that is, a Kinpo cylinder, having a common central axis on the outside of the conductor plate. However, since the spatial uniformity of the generated high frequency magnetic field is in the same direction, the conductor plate is
In addition, the cylindrical high-frequency magnetic field generator/detector for the whole body becomes larger, and the efficiency of transmitting magnetic field generation or the S/N of the received signal becomes smaller. It is almost oval in shape, so
The high-frequency magnetic field generator/detector can be made into an elliptical cylinder whose major axis is the diameter of the cylinder. As a result, the efficiency of magnetic field generation is 2 higher than in the case of a cylinder, and the S/N of the received signal is also decreased. For example, compared to 64MHz or the case of two cylinders, the elliptical case has a transmission power of 60 to 70% for the same transmission power.
Experiments have shown that the transmitted magnetic field increases.Also, when the RF coil is installed so that the major axis of the ellipse is horizontal, the vertical Arrange the punts in the short axis direction and the long axis direction.
以とのように、この発明は1対の突出部を各量結合する
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
衡不平衡変換器により、安定で効率の良い高周波磁場発
生・検出器を得れる効果がある。また、全身用の高周波
磁場発生・検出器の形を楕円にすることにより高い磁場
発生の効率となり受信信号のS/N も向とする。As described above, the present invention includes a first variable capacitor that couples a pair of protrusions in different amounts, a second variable capacitor and a third variable capacitor connected to each end of the first variable capacitor, respectively.
A balanced impedance matching circuit consisting of a variable capacitor and a balanced unbalanced converter connected to this balanced impedance matching circuit have the effect of providing a stable and efficient high frequency magnetic field generator/detector. Furthermore, by making the shape of the high-frequency magnetic field generator/detector for the whole body into an ellipse, the efficiency of magnetic field generation is high, and the S/N ratio of the received signal is also improved.
第1図はこの発明の一実施例による高周波磁場発生・検
出器を示す斜視図、第2,3図はこの発明の池の実施例
を示す斜視図、第4図は従来の高周波磁場発生・検出器
である、
図におい”(、fi+は導体板、 (1a)はバーチカ
ルパント、 (lb)はウィング&(2)は固定コンデ
ンサ。
(8す、(8b)、(80は可変コンデンサ、(9)は
平衡不平衡変換器である。各図中の同一符号は同一また
は相当部分を示す。
代 理 人 大 岩 増 雄第1図
ja
h・第1可変コ〉1°゛シブ
θb $z可変コンテ゛;′ワ′
8c:第J可茨コ〉デ゛〉ア
第2図
第3図
第4図FIG. 1 is a perspective view showing a high-frequency magnetic field generator/detector according to an embodiment of the present invention, FIGS. 2 and 3 are perspective views showing an embodiment of the pond according to the present invention, and FIG. 4 is a conventional high-frequency magnetic field generator/detector. The detector is shown in the figure, fi+ is a conductor plate, (1a) is a vertical capacitor, (lb) is a wing & (2) is a fixed capacitor. 9) is a balanced unbalanced converter. The same reference numerals in each figure indicate the same or equivalent parts. Agent: Masuo Oiwa Variable Container; 'W' 8c: No. J Variable Container Diagram 2 Figure 3 Figure 4
Claims (6)
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、もつて等価的に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, the pair of protrusions that remain together are called the first
A balanced impedance consisting of a three-dimensional circuit that is capacitively coupled with a variable capacitor to equivalently constitute an LC resonant circuit, and the first variable capacitor, and a second variable capacitor and a third variable capacitor connected to each end of the first variable capacitor. A high-frequency magnetic field generator/detector comprising a matching circuit 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:
請求の範囲第1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, wherein the three-dimensional circuit is cylindrical.
特許請求の範囲第1項記載の高周波磁場発生・検出器。(4) The high-frequency magnetic field generator/detector according to claim 1, wherein the three-dimensional circuit has an elliptical cylinder shape.
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。(5) 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項または第2項の高周波磁場発生・検出器。(6) The high frequency magnetic field generator/detector according to claim 1 or 2, wherein the balanced/unbalanced converter is a coaxial cable having an electrical length of 1/2 wavelength.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61197582A JPS6353906A (en) | 1986-08-22 | 1986-08-22 | Radio frequency magnetic field generating detector |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61197582A JPS6353906A (en) | 1986-08-22 | 1986-08-22 | Radio frequency magnetic field generating detector |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6353906A true JPS6353906A (en) | 1988-03-08 |
Family
ID=16376884
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61197582A Pending JPS6353906A (en) | 1986-08-22 | 1986-08-22 | Radio frequency magnetic field generating detector |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6353906A (en) |
-
1986
- 1986-08-22 JP JP61197582A patent/JPS6353906A/en active Pending
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