JPS6335240A - High frequency magnetic field generating and detecting apparatus - Google Patents

High frequency magnetic field generating and detecting apparatus

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Publication number
JPS6335240A
JPS6335240A JP61179526A JP17952686A JPS6335240A JP S6335240 A JPS6335240 A JP S6335240A JP 61179526 A JP61179526 A JP 61179526A JP 17952686 A JP17952686 A JP 17952686A JP S6335240 A JPS6335240 A JP S6335240A
Authority
JP
Japan
Prior art keywords
conductor
magnetic field
frequency magnetic
detection device
field generation
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
Application number
JP61179526A
Other languages
Japanese (ja)
Inventor
西原 進
潔 依田
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 JP61179526A priority Critical patent/JPS6335240A/en
Priority to US07/013,901 priority patent/US4755756A/en
Publication of JPS6335240A publication Critical patent/JPS6335240A/en
Pending legal-status Critical Current

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Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Abstract] This bulletin contains application data before electronic filing, so abstract data is not recorded.

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・検出装置、特に核磁気共鳴
装置に用いる高周波磁場発生・検出装置に関するもので
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.

〔従来の技術〕[Conventional technology]

第6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 Magneti
cResonance ) 3 6巻、447頁〜45
1頁(19’79)に示されている従来の高周波磁場発
生・検出装置全示す図であり、図において(1)は銅板
で構成されるコイル部でバーチカル バンド(vart
ical band)(1a)、ウィング(wing)
 (lb)、窓部(’la )よシ構成される。(2)
は隣接するウィング間に挿入されたコンデンサ、(3)
はウィングの内側に絶縁層を介して設置された電界シー
ルド用の保護環でガードリング(Guarol Rin
g)と呼ばれ、トップガードリング(Top Guar
d Ring) (3a)、とボトムガードリンク(B
ottom Guard Ring) (3b)より構
成される。
Figure 6 shows, for example, the journal op magnetic
Resonance ( Journal of Magneti
cResonance) Volume 3 6, Pages 447-45
This is a diagram showing the entire conventional high-frequency magnetic field generation/detection device shown on page 1 (19'79).
ical band) (1a), wing
(lb) and the window ('la). (2)
is a capacitor inserted between adjacent wings, (3)
Guard ring is a protective ring for electric field shield installed inside the wing via an insulating layer.
g) and is called a top guard ring (Top Guar ring).
d Ring) (3a), and the bottom guard link (B
ottom Guard Ring) (3b).

(4)は給電点、(5)はインピーダンス整合用コンデ
ンサ、(6)は送受信機と接続される端子である。
(4) is a feeding point, (5) is an impedance matching capacitor, and (6) is a terminal connected to a transmitter/receiver.

次に動作について説明する。Next, the operation will be explained.

コイル部(1)、コンデンサ(2)、ガードリング(3
)は等節約にLC直列共振回路を構成する。インピーダ
ンス整合用コンデンサ(5)、端子(6) ′t−経て
所定のインピーダンスを有する送信器及び受信器(図示
せず)と接続され、送信器から電流がコイル部(1)に
供給され所定の高周波磁場を作る一方、コイル部(1)
内に設けられた測定対象からの信号を受信器に導びくよ
うに働らく。ガードリング(3)は、電界シールドの働
らきをし、この高周波磁場発生・検十装置内に測定対象
を設置した場合に、発生電界:こよる6111定対象内
の誘電損失を低減する。
Coil part (1), capacitor (2), guard ring (3)
) constitutes an LC series resonant circuit equally parsimoniously. The impedance matching capacitor (5) and the terminal (6) are connected to a transmitter and a receiver (not shown) having a predetermined impedance through the impedance matching capacitor (5) and a terminal (6). While creating a high frequency magnetic field, the coil part (1)
It functions to guide the signal from the object to be measured located inside to the receiver. The guard ring (3) functions as an electric field shield, and when a measurement object is installed in this high frequency magnetic field generation/detection device, it reduces the dielectric loss within the object due to the generated electric field.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

6を来の高周波磁場発生・検出装置は以−1一のように
構成されているので、回路インピーダンスの平衡不平衡
変換が考慮されておらず、端子(0)に接続する同軸ケ
ーブルに同相電流が流れて、不安定、低効率になるなど
の欠点があった。
Since the high-frequency magnetic field generation/detection device described in Section 6 is configured as shown below, the balance/unbalance conversion of the circuit impedance is not taken into consideration, and the common mode current flows through the coaxial cable connected to terminal (0). There were disadvantages such as the flow of electricity, resulting in instability and low efficiency.

この発明は上記のような問題点を解消するためになされ
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・検出装置を得る
ことを目的とする。
The present invention has been made to solve the above-mentioned problems, and aims to provide a stable and efficient high-frequency magnetic field generation/detection device by taking into consideration the unbalanced circuit impedance.

また、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S/N(’Sign
al to Noise Ratio)が比較的小さい
などの問題があった。
In addition, when the high-frequency coil for the whole body is cylindrical, the efficiency of generating the transmitting magnetic field is low, and the S/N (S/N) of the received signal is low.
There were problems such as a relatively small al to noise ratio.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る高周波磁場発生・検出装置は、コイル部
のバーチカルバンド(タテ導体部)の中央部で部分し、
部分されたタテ導体部の端部を誘電体物質を介して重ね
合せて誘電体結合した構成として可変コンデンサとする
と共に、この部分されたタテ導体部の各端部部分を給電
点とし、別に不平衡・平衡変換回路を設けてこの給電点
に平衡給電するようにしたものである。また、全身用の
高周波コイルの形を楕円形にする。
The high frequency magnetic field generation/detection device according to the present invention has a part at the center of the vertical band (vertical conductor part) of the coil part,
A variable capacitor is constructed by dielectrically bonding the ends of the vertical conductor portions by overlapping them through a dielectric material, and each end portion of the vertical conductor portion is used as a power feeding point, and a separate power source is used. A balanced/balanced conversion circuit is provided to feed balanced power to this feeding point. In addition, the shape of the high-frequency coil for the whole body is made oval.

〔作用〕[Effect]

この発明における高周波磁場発生●検出装置は上記の構
成にすることによクコイル部(1)に、コイル部を含む
真の負荷にのみ有効に働らく平衡電流(アースに対逆相
の電流〕のみが流れ、同相電流は抑制されるので、給電
効率が著しく向上する。
The high-frequency magnetic field generation/detection device of this invention has the above configuration, so that only a balanced current (a current with a negative phase to the ground) that effectively acts only on the true load including the coil section is applied to the coil section (1). flows, and the common-mode current is suppressed, significantly improving power supply efficiency.

また、全身用の高周波コイルを楕円型にすることによシ
、送信磁場発生の効率や受信信号の8/Nが向上する。
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 8/N ratio of the received signal are improved.

〔実施例〕〔Example〕

以下、この発明の実施例を図について説明する。 Embodiments of the present invention will be described below with reference to the drawings.

第1図は第1の実施例の斜視図、第2図はその説明のた
めの一部断面構成図、第3図はその等価回路である。
FIG. 1 is a perspective view of the first embodiment, FIG. 2 is a partially sectional configuration diagram for explaining the same, and FIG. 3 is an equivalent circuit thereof.

第1図及び第2図において同一符号のものは同−又は相
当部分を示す。(1)はコイル部であってタテ導体部(
la) (従来例のバーチカルパントに相当)とヨコ導
体部(従来例のウィングに相当)より構成される。(2
)はコンデンサであって隣接するヨコ導体部の端部を容
量結合するものである。(3)はガードリングでトップ
ガードリング(3a)とボトムガードリング(3b)よ
り構成される。(6)は端子で給電電流の供給と検出電
流の取出を行う。(’i’a)、(’7b)は給電点、
(8)は整合回路で誘電体o0を介して上下のタテ導体
部の重さなり部分で構成されるコンデンサ部(8a)及
び可変コンデンサ(8b)、(8Q)により構成される
。なお、コンデンサ部(8a)の静電容量は重さな9部
分の大きさを変えることにより可変される構造となって
いる。(9)はi波長ケーブルで、端子(6)から供給
される不平衡電流全180°遅相して逆相変換し整合回
路(8)ヲ経て2つの給電点(”7a)。
In FIG. 1 and FIG. 2, the same reference numerals indicate the same or corresponding parts. (1) is the coil part and the vertical conductor part (
la) (corresponding to the vertical pant of the conventional example) and a horizontal conductor part (corresponding to the wing of the conventional example). (2
) is a capacitor that capacitively couples the ends of adjacent horizontal conductor parts. (3) is a guard ring, which is composed of a top guard ring (3a) and a bottom guard ring (3b). (6) is a terminal that supplies the power supply current and takes out the detection current. ('i'a), ('7b) are feeding points,
Reference numeral (8) denotes a matching circuit, which is composed of a capacitor section (8a) and variable capacitors (8b) and (8Q) which are formed by overlapping portions of upper and lower vertical conductor sections via a dielectric material o0. Note that the capacitance of the capacitor section (8a) can be varied by changing the size of the 9 heavy parts. (9) is an i-wavelength cable, and the unbalanced current supplied from the terminal (6) is delayed by 180 degrees and converted into an inverted phase, and then passes through the matching circuit (8) to two feeding points (7a).

(7b)に同振幅逆相電流を給電できるようにする不平
衡・平衡変換の働らきをするものである。
(7b) functions as an unbalanced/balanced conversion so that the same amplitude and negative sequence current can be supplied.

なお、タテ導体部のなす角度θの一例としては8o0〈
θ〈900である。また、(lc)はタテ導体部(la
)とヨコ導体部(1b)で包まれる空間部分であってコ
イル部の窓部という。
An example of the angle θ formed by the vertical conductor is 8o0〈
θ<900. In addition, (lc) is the vertical conductor part (la
) and the horizontal conductor section (1b), and is called the window section of the coil section.

高周波コイルの形は楕円の筒型であQ、第1図において
はバーチカルパントは楕円の短径方向に配置されている
例であり、第4図は長径方向に配置されている例である
The shape of the high-frequency coil is an elliptical cylinder Q, and FIG. 1 shows an example in which the vertical punts are arranged in the short axis direction of the ellipse, and FIG. 4 shows an example in which they are arranged in the long axis direction.

次に動作について説明する。Next, the operation will be explained.

第3図の等価回路に示すように、タテ導体部(1a)(
インダクタンスで示されている)とヨコ導体部コイル部
(1)、コンデンサ(2)、ガードリング(3)及びコ
ンデンサ(8a)で構成される等測的な直並列共振回路
に対し、給電点(’7a)j7b)から整合回路(3)
を経て平衡給電が行われる。
As shown in the equivalent circuit of Fig. 3, the vertical conductor portion (1a) (
For an isometric series-parallel resonant circuit consisting of a horizontal conductor coil portion (1), a capacitor (2), a guard ring (3), and a capacitor (8a), the feed point ( '7a) j7b) to matching circuit (3)
Balanced power supply is performed through this process.

共振回路及び整合回路の調整を行って所賛の信号が効率
よく負荷に供給されるようにする。
The resonant circuit and matching circuit are adjusted so that the desired signal is efficiently supplied to the load.

この構成では、負荷はアースに対して逆相等振幅でバラ
ンスしており、かつ給電電流はコイル部を含む真の負荷
が必要とする平衡電流に完全に変換されて供給される。
In this configuration, the load is balanced with equal amplitude and negative phase with respect to the ground, and the feeding current is completely converted into a balanced current required by the true load including the coil section and supplied.

また、共振と共に整合もきちんととれるようになってい
るので、給電効率は極めてよいものとなる。また、か\
る構成になっているのでコイル部の中に置かれた測定対
象からの信号も効率よく抽出することができる。
In addition, since resonance and matching are properly achieved, power feeding efficiency is extremely high. again\
Since the structure is such that signals from a measurement target placed inside the coil section can be efficiently extracted.

上記実施例ではヨコ導体部(1b)の隣合う部分の接合
はコンデンサ(2)ヲ介して容量結合されていたが、第
5図に示す他の実施例のように共振周波数の関係ではこ
のコンデンサを外し直接接合してもよく、ガードリング
も外してもよく、かかる場合についても同様にタテ導体
部の中央部で上下に分離しその間を誘電体を介して重ね
合せると共にその部分を給電点として平衡給電方式を適
用する構成にすることにより効率よい励磁電流の給電と
信号検出を行うことが出来る。
In the above embodiment, the junctions of adjacent parts of the horizontal conductor portion (1b) were capacitively coupled via the capacitor (2), but as in the other embodiment shown in FIG. The conductor may be removed and connected directly, or the guard ring may also be removed. In such cases, the vertical conductor may be separated into upper and lower parts at the center, overlapped with a dielectric between them, and that part may be used as a power feeding point. By adopting a configuration that applies a balanced power supply system, efficient excitation current supply and signal detection can be performed.

なお、第5図において第1図と同一符号のものは同−又
は相当部分を示す。
In FIG. 5, the same reference numerals as in FIG. 1 indicate the same or equivalent parts.

なお、上記実施例において不平衡・平衡変換手段として
一波長ケーブルを使う場合について説明したが、2次巻
線のバランスのよいトランスを用いてもよい。
In the above embodiments, a single wavelength cable is used as the unbalanced/balanced conversion means, but a transformer with a well-balanced secondary winding may also be used.

また、タテ導体部の間に設けられた誘電体を介して構成
される可変コンデンサ部分に並列に固定コンデンサ又は
可変コンデンサを接続してもよく、この可変コンデンサ
により、整合をとっても良い。
Further, a fixed capacitor or a variable capacitor may be connected in parallel to the variable capacitor portion configured via a dielectric provided between the vertical conductor portions, and matching may be achieved using this variable capacitor.

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B/II
が小さくなる。人間の体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
う々楕円筒にすることができる。これにより、円筒の場
合に比べて高い磁場発生の効率となり受信信号の87N
も向上する。
In addition, the cylindrical high-frequency magnetic field generator/detector for the whole body has become larger, and the efficiency of transmitting magnetic field generation or B/II of the received signal has increased.
becomes smaller. Since the cross section of the human body is approximately elliptical, the high-frequency magnetic field generator/detector can be made into an elliptical cylinder so that the diameter of the cylinder is the major axis. As a result, the efficiency of magnetic field generation is higher than in the case of a cylinder, and the received signal is 87N
It also improves.

例えば、64MHzに対しては、円筒の場合に比較して
楕円形では同一の送信電力の場合60〜70チ送信磁場
が増加することが実験により判明した。
For example, for 64 MHz, it has been experimentally found that the transmitted magnetic field increases by 60 to 70 cm for the same transmit power in the case of an elliptical shape compared to the case of a cylinder.

′!1.fc1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バンドを短径
方向、長径方向に配置する。
′! 1. RF so that the major axis direction of the fc1 ellipse is horizontal.
Depending on whether the high-frequency magnetic field is generated horizontally or vertically when the coil is installed, the vertical bands are arranged in the minor axis direction and the major axis direction, respectively.

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明に係る高周波磁場発生・検出装
置は、コイル部のタテ導体部の中央部で二つに分け、部
分されたタテ導体部の端部を誘電体物質を介して重ね合
せて誘電体結合した構成として可変コンデンサとすると
共に、この部分されたタテ導体部の端部部分を給電点と
して、別に不平衡・平衡変換回路を設けてこの給電点に
平衡給電するようにしたので、コイル部にはコイル部を
含む真の負荷にのみ有効に働らく平衡電流のみが給電さ
れ、不平衡電流が流れないので、給電効率及び信号検出
効率が著しく向上する効果を有する。
As described above, in the high-frequency magnetic field generation/detection device according to the present invention, the vertical conductor portion of the coil portion is divided into two at the center, and the ends of the vertical conductor portions are overlapped with each other via a dielectric material. In addition to making a variable capacitor with a dielectric-coupled configuration, the end portion of the vertical conductor section is used as a power feeding point, and a separate unbalanced/balanced conversion circuit is provided to feed balanced power to this feeding point. Since only a balanced current that effectively acts only on the true load including the coil portion is fed to the coil portion, and no unbalanced current flows, the power feeding efficiency and signal detection efficiency are significantly improved.

また、全身用の高周波磁場発生・検出器の形を楕円形に
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も向上する。
Furthermore, by making the whole-body high-frequency magnetic field generator/detector elliptical in shape, the efficiency of magnetic field generation is high, and the S/N of the received signal is also improved.

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

第1図はこの発明の実施例、第2図はこの実施例の説明
用の図面、第3図は同じく等価回路、第4図はこの発明
の他の実施例、第5図はこの発明の他の実施例で第1図
の場合のコンデンサ(2)がない場合の一例金示す。第
6図は従来例を示す図である。 (1)・・・コイル部、(1a〕・・・タテ導体部、(
1b)・・・ヨコ導体部、(lc)・・・窓部、(2)
・・・コンデンサ、(3)・・・ガードリング、(3a
)・・・トップガードリング、(3b)・・・ボトムガ
ードリング、(6)・・・端子、(7a)、(’7b)
・・・給電点、(8)・・・整合回路、(8a)・・コ
ンデンサ部、(Bb)、(Ba)・・・可変コンデンサ
、(9)・・・石波長ケーブル、C1O・・・誘電体。 なお、図中同一符号は同−又は相当部分を示す。
FIG. 1 is an embodiment of this invention, FIG. 2 is an explanatory drawing of this embodiment, FIG. 3 is an equivalent circuit, FIG. 4 is another embodiment of this invention, and FIG. 5 is a drawing for explaining this embodiment. In another embodiment, an example in which the capacitor (2) of FIG. 1 is not provided is shown. FIG. 6 is a diagram showing a conventional example. (1)...Coil part, (1a)...Vertical conductor part, (
1b)...Horizontal conductor part, (lc)...Window part, (2)
... Capacitor, (3) ... Guard ring, (3a
)...Top guard ring, (3b)...Bottom guard ring, (6)...Terminal, (7a), ('7b)
...Feeding point, (8)...Matching circuit, (8a)...Capacitor section, (Bb), (Ba)...Variable capacitor, (9)...Stone wavelength cable, C1O... dielectric. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (8)

【特許請求の範囲】[Claims] (1)たて方向にのびる所定幅のタテ導体部と、この上
端部にこれと直交して設けられ、左右にのびる所定幅の
ヨコ導体部を有するT字型導体板を、タテ導体部を軸方
向として所定の弧を描くように湾曲させたもの複数個を
楕円状に隣接して配列した第1の導体と、 この第1の導体と略相似の形状を有し第1の導体とそれ
ぞれの有するタテ導体部の一部で誘電体を介して対向方
向にかん合配置される第2の導体を前記軸方向に動かし
て静電容量を変える可変コンデンサを備えた立体回路と
、 前記第1の導体のタテ導体部に設けられた第1の給電点
と前記第2の導体の前記第1の導体のタテ導体部に対向
する位置のタテ導体部に設けられた第2の給電点とを介
して前記各導体に高周波の平衡電流を給電する給電回路
とを備えたことを特徴とする高周波磁場発生・検出装置
(1) A T-shaped conductor plate having a vertical conductor part with a predetermined width extending in the vertical direction and a horizontal conductor part with a predetermined width provided at the upper end and perpendicular to this and extending left and right. a first conductor in which a plurality of conductors curved to draw a predetermined arc in the axial direction are arranged adjacently in an elliptical shape; a first conductor having a shape substantially similar to the first conductor; a three-dimensional circuit comprising a variable capacitor that changes capacitance by moving a second conductor in the axial direction that is arranged to be engaged with a part of the vertical conductor part in the opposite direction via a dielectric; a first power feeding point provided on the vertical conductor portion of the conductor; and a second power feeding point provided on the vertical conductor portion of the second conductor at a position opposite to the vertical conductor portion of the first conductor. A high-frequency magnetic field generation/detection device comprising: a power supply circuit that supplies a high-frequency balanced current to each of the conductors through the conductor.
(2)立体回路は、導体板の外側に、所定の軸を中心軸
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項記載の高周波磁場発生・検出装置。
(2) The high-frequency magnetic field generation/detection device according to claim 1, wherein the three-dimensional circuit has a conductor tube having a predetermined axis as its central axis on the outside of the conductor plate.
(3)前記第1の給電点と第2の給電点の間に固定コン
デンサもしくは可変コンデンサを備えたことを特徴とす
る特許請求の範囲第1項に記載の高周波磁場発生・検出
装置。
(3) The high frequency magnetic field generation/detection device according to claim 1, further comprising a fixed capacitor or a variable capacitor between the first feeding point and the second feeding point.
(4)平衡給電は、入力電流を1/2波長回路を経て逆
相としこの信号を各給電点へ給電することによつて達成
するようにしたことを特徴とする前記特許請求の範囲第
1項ないし第3項のいずれかに記載の高周波磁場発生・
検出装置。
(4) Balanced power feeding is achieved by passing the input current through a 1/2 wavelength circuit, reverse phase, and feeding this signal to each feeding point. High frequency magnetic field generation according to any one of paragraphs to 3.
Detection device.
(5)平衡給電は入力電流を1/2波長回路とインピー
ダンスマッチング回路を経て各給電点へ給電することに
よつて達成するようにしたことを特徴とする前記特許請
求の範囲第1項ないし第4項のいずれかに記載の高周波
磁場発生・検出装置。
(5) Balanced power supply is achieved by supplying input current to each power supply point via a 1/2 wavelength circuit and an impedance matching circuit. The high frequency magnetic field generation/detection device according to any one of Item 4.
(6)給電を前記給電点の1組又は複数組に対して行い
、給電しない給電点は所定のインピーダンスを接続する
ことを特徴とする前記特許請求の範囲第1項ないし第5
項のいずれかに記載の高周波磁場発生・検出装置。
(6) Claims 1 to 5 above, characterized in that power is supplied to one or more sets of the power supply points, and the power supply points to which power is not supplied are connected to a predetermined impedance.
The high frequency magnetic field generation/detection device according to any one of paragraphs.
(7)隣接するT字型導体板のヨコ導体部同士が直流的
に接続されていることを特徴とする前記特許請求の範囲
第1項ないし第6項のいずれかに記載の高周波磁場発生
・検出装置。
(7) The high-frequency magnetic field generation system according to any one of claims 1 to 6, characterized in that the horizontal conductor portions of adjacent T-shaped conductor plates are connected in a DC manner. Detection device.
(8)隣接するT字型導体板のヨコ導体部は所定の静電
容量を介して接続されていることを特徴とする前記特許
請求の範囲第1項ないし第7項のいずれかに記載の高周
波磁場発生・検出装置。
(8) The horizontal conductor portions of adjacent T-shaped conductor plates are connected via a predetermined capacitance. High frequency magnetic field generation/detection device.
JP61179526A 1986-02-18 1986-07-29 High frequency magnetic field generating and detecting apparatus Pending JPS6335240A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP61179526A JPS6335240A (en) 1986-07-29 1986-07-29 High frequency magnetic field generating and detecting apparatus
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
JP61179526A JPS6335240A (en) 1986-07-29 1986-07-29 High frequency magnetic field generating and detecting apparatus

Publications (1)

Publication Number Publication Date
JPS6335240A true JPS6335240A (en) 1988-02-15

Family

ID=16067302

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61179526A Pending JPS6335240A (en) 1986-02-18 1986-07-29 High frequency magnetic field generating and detecting apparatus

Country Status (1)

Country Link
JP (1) JPS6335240A (en)

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