2z2BH+A(z)z=00 ]]> applies for the axial magnetic field profile BH+A(z) generated by the main field coil and the shielding coil during operation along the z-axis in the center at z=0 and; <math overflow="scroll"><mrow><mrow><mfrac><msup><mo>ⅆ</mo><mn>2</mn></msup><mrow><mo>ⅆ</mo><msup><mi>z</mi><mn>2</mn></msup></mrow></mfrac><mo>⁢</mo><mrow><msub><mi>B</mi><mi>F</mi></msub><mo>⁡</mo><mrow><mo>(</mo><mi>z</mi><mo>)</mo></mrow></mrow></mrow><mo>⁢</mo><msub><mo>❘</mo><mrow><mi>z</mi><mo>=</mo><mn>0</mn></mrow></msub><mo>⁢</mo><mrow><mo>≥</mo><mn>0</mn></mrow></mrow></math> applies for the axial magnetic field profile BF(z) generated by the ferromagnetic field-shaping device (3; 18) during operation along the z-axis in the center at z=0, wherein the z-axis is oriented in a positive direction of the B0-field. An actively shielded superconducting magnet configuration of considerably simplified structure is thereby provided with a homogeneous and particularly high magnetic field B0 in the volume under investigation."/> Compact superconducting magnet configuration with active shielding, wherein the shielding coil damps the field maximum of the main coil as well as associated magnetic resonance tomograph, NMR spectrometer and ion cyclotron resonance mass spectrometer
首页> 外国专利> Compact superconducting magnet configuration with active shielding, wherein the shielding coil damps the field maximum of the main coil as well as associated magnetic resonance tomograph, NMR spectrometer and ion cyclotron resonance mass spectrometer

Compact superconducting magnet configuration with active shielding, wherein the shielding coil damps the field maximum of the main coil as well as associated magnetic resonance tomograph, NMR spectrometer and ion cyclotron resonance mass spectrometer

机译:具有有源屏蔽的紧凑型超导磁体配置,其中屏蔽线圈会衰减主线圈以及相关的磁共振断层扫描仪,NMR光谱仪和离子回旋共振质谱仪的最大磁场

摘要

An actively shielded superconducting magnet configuration (M1; M2; M3; 14) for generating a homogeneous magnetic field B0 in a volume under investigation (4b) has a radially inner superconducting main field coil (1) which is disposed rotationally symmetrically about an axis (z axis) and a coaxial radially outer superconducting shielding coil (2) which is operated in an opposite direction. The magnet configuration consists of the main field coil, the shielding coil and a ferromagnetic field-shaping device (3; 18), wherein the ferromagnetic field-shaping device is disposed radially inside the main field coil. The main field coil consists of an unstructured solenoid coil or of several radially nested unstructured solenoid coils (15, 16) which are operated in the same direction. An extension Labs of the shielding coil in the axial direction is smaller than the extension Lhaupt of the main field coil in the axial direction.; <math overflow="scroll"><mrow><mrow><mfrac><msup><mo>ⅆ</mo><mn>2</mn></msup><mrow><mo>ⅆ</mo><msup><mi>z</mi><mn>2</mn></msup></mrow></mfrac><mo>⁢</mo><mrow><msub><mi>B</mi><mrow><mi>H</mi><mo>+</mo><mi>A</mi></mrow></msub><mo>⁡</mo><mrow><mo>(</mo><mi>z</mi><mo>)</mo></mrow></mrow></mrow><mo>⁢</mo><msub><mo>❘</mo><mrow><mi>z</mi><mo>=</mo><mn>0</mn></mrow></msub><mo>⁢</mo><mrow><mo>≤</mo><mn>0</mn></mrow></mrow></math> applies for the axial magnetic field profile BH+A(z) generated by the main field coil and the shielding coil during operation along the z-axis in the center at z=0 and; <math overflow="scroll"><mrow><mrow><mfrac><msup><mo>ⅆ</mo><mn>2</mn></msup><mrow><mo>ⅆ</mo><msup><mi>z</mi><mn>2</mn></msup></mrow></mfrac><mo>⁢</mo><mrow><msub><mi>B</mi><mi>F</mi></msub><mo>⁡</mo><mrow><mo>(</mo><mi>z</mi><mo>)</mo></mrow></mrow></mrow><mo>⁢</mo><msub><mo>❘</mo><mrow><mi>z</mi><mo>=</mo><mn>0</mn></mrow></msub><mo>⁢</mo><mrow><mo>≥</mo><mn>0</mn></mrow></mrow></math> applies for the axial magnetic field profile BF(z) generated by the ferromagnetic field-shaping device (3; 18) during operation along the z-axis in the center at z=0, wherein the z-axis is oriented in a positive direction of the B0-field. An actively shielded superconducting magnet configuration of considerably simplified structure is thereby provided with a homogeneous and particularly high magnetic field B0 in the volume under investigation.
机译:用于产生均匀磁场B 0的有源屏蔽超导磁体配置(M 1 ; M 2 ; M 3; 14 在研究的体积( 4 b )中有一个径向内部的超导主磁场线圈( 1 ),该线圈旋转对称地布置绕着一个轴(z轴)和一个沿相反方向工作的同轴径向外部超导屏蔽线圈( 2 )。磁体结构由主磁场线圈,屏蔽线圈和铁磁场整形设备( 3; 18 )组成,其中铁磁场整形设备在径向上位于主磁场线圈内部。主磁场线圈由非结构化螺线管线圈或沿相同方向操作的多个径向嵌套的非结构化螺线管线圈( 15、16 )组成。屏蔽线圈在轴向上的延伸长度L abs 小于主磁场线圈在轴向上的延伸长度L haupt <![CDATA [<数学溢出=“ scroll”> 2 z 2 B H + A z z = 0 0 ]]> 适用于主磁场​​线圈和屏蔽线圈在z = 0时在中心沿z轴运行时产生的轴向磁场分布B H + A (z); <![CDATA [<数学溢出=“ scroll”> 2 z 2 B F z z = 0 0 ]]> 适用于铁磁场整形装置( 3; 18 )在中心处沿z轴运行时产生的轴向磁场分布B F (z) z = 0,其中z轴指向B 0 场的正方向。因此,在被研究的体积中,具有相当简化的结构的有源屏蔽超导磁体构造具有均匀且特别高的磁场B 0

著录项

  • 公开/公告号US8154368B2

    专利类型

  • 公开/公告日2012-04-10

    原文格式PDF

  • 申请/专利权人 MICHAEL WESTPHAL;GERALD NEUBERTH;

    申请/专利号US20100896924

  • 发明设计人 GERALD NEUBERTH;MICHAEL WESTPHAL;

    申请日2010-10-04

  • 分类号H01F1/00;H01F7/00;H01F6/00;

  • 国家 US

  • 入库时间 2022-08-21 17:26:11

相似文献

  • 专利
  • 外文文献
  • 中文文献
获取专利

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号