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    • 1. 发明申请
    • System Incorporating Current Path Between Conductive Members
    • 导电构件之间的电流路径的系统
    • US20130229086A1
    • 2013-09-05
    • US13877766
    • 2011-10-06
    • Rainer Meinke
    • Rainer Meinke
    • H01R3/00H02K13/00
    • H01R3/00H02J3/00H02K5/22H02K13/00H02K55/00Y02E40/62
    • An electrical system having a current path formed in a region between first and second electrodes. When a low pressure is sustained in the region, and a plasma is generated in a portion of a gap between the electrodes, current flows across the gap from the first electrode to the second electrode. In one embodiment the system is operable as a motor or a generator, having a first electrode and a member including a second electrode which is rotatable with respect to the first electrode. In another embodiment a first conductor is positioned to carry current toward or away from a first terminal at a high temperature, and a second conductor is spaced apart from the first terminal to carry current toward or away from a second terminal when the second conductor is at a low temperature relative to the temperature of the first region.
    • 一种具有形成在第一和第二电极之间的区域中的电流通路的电气系统。 当在该区域中维持低压并且在电极之间的间隙的一部分中产生等离子体时,电流从第一电极流过间隙,从而流过第二电极。 在一个实施例中,该系统可操作为电动机或发电机,其具有第一电极和包括可相对于第一电极旋转的第二电极的构件。 在另一个实施例中,第一导体被定位成在高温下朝向或远离第一端子携带电流,并且当第二导体处于第二导体时,第二导体与第一端子间隔开以朝向或远离第二端子传送电流 相对于第一区域的温度的低温度。
    • 4. 发明申请
    • Magnetic Coil Capable of Simultaneously Providing Multiple Multipole Orders With an Improved Transfer Function
    • 磁线圈能够同时提供具有改进的传递函数的多个多项式
    • US20100031496A1
    • 2010-02-11
    • US12473549
    • 2009-05-28
    • Rainer MeinkeCarl Goodzeit
    • Rainer MeinkeCarl Goodzeit
    • H01F41/04
    • G21K1/093H01F7/20Y10T29/49071
    • A method for constructing a conductor assembly of the type formed of one or more coil rows which, when conducting current, generate a magnetic field or in which, in the presence of a changing magnetic field, a voltage is induced. In one embodiment comprises forming a conductor pattern in a first coil row according to the relationship X(θ)=[h/(2*π)]θ+ΣAn sin(nθ+φn) Y(θ)=R cos(θ) Z(θ)=R sin(θ), the first coil row pattern suitable for simultaneously generating at least two multipole orthogonal field components of different orders, wherein: X is measurable along an X axis, Y is measurable along a Y axis and Z is measurable along a Z axis, the coil row extends along the X axis, the coil row is formed with a conductor configured in a series of turns about the X axis creating spaced-apart segments of the conductor such that, along first portions of the segments, individual segments are relatively straight and along second portions of the segments the segments follow a contour having a definable radius of curvature, the series of turns providing a geometrical configuration for generating a first multipole component of order n=i with An=Ai and φn=φi and a second multipole component of order n=j with An=Aj and φn=φj with φi not equal to φj.
    • 一种用于构造由一个或多个线圈列形成的类型的导体组件的方法,其在导电电流时产生磁场,或者在存在变化的磁场的情况下引起电压。 在一个实施例中包括根据关系X(θ)= [h /(2 * pi)]θ+ΣAnsin(nta + phin)Y(θ)= R cos(θ)在第一线圈列中形成导体图案 Z(θ)= R sin(θ),适合于同时产生不同阶数的至少两个多极正交场分量的第一线圈行图案,其中:X可沿X轴测量,Y可沿Y轴和Z 沿着Z轴可测量,线圈列沿着X轴延伸,线圈列形成有绕X轴构成一系列匝的导体,从而产生导体的间隔开的部分,使得沿第一部分 片段,单个片段相对直,并且沿着片段的第二部分,片段遵循具有可定义曲率半径的轮廓,所述一系列匝提供用于产生具有An = Ai的阶n = i的第一多极分量的几何配置,以及 phin = phii和第二个多极分量 n = j,An = Aj,phin = phij,phii不等于phij。
    • 5. 发明申请
    • Structure For A Wiring Assembly And Method Suitable For Forming Multiple Coil Rows With Splice Free Conductor
    • 适用于使用无接头导体形成多个线圈的接线组件和方法的结构
    • US20090251271A1
    • 2009-10-08
    • US12061870
    • 2008-04-03
    • Gerald StelzerRainer MeinkePaul Bruton
    • Gerald StelzerRainer MeinkePaul Bruton
    • H01F27/30H01F7/06
    • H01F7/202H01F5/02H01F6/06H01F41/086H01F41/098Y10T29/4902
    • A conductor assembly and method for constructing an assembly of the type which, when conducting current, generates a magnetic field or which, in the presence of a changing magnetic field, induces a voltage. In one embodiment the method includes forming a structure comprising layers of material extending along a first aperture path. The structure includes multiple concentric layer surfaces. A channel is formed in each of the layers of the material and along each of the multiple surfaces. Conductive material is positioned in each channel to provide a spiral configuration. The surfaces of multiple ones of the layers are of tubular shape. The layers of material are sequentially positioned one over another and about an axis along which first and second opposing coil end regions are formed. The layers are formed with a region of a first thickness and a shoulder region. The shoulder region is alternately formed in the sequence at one coil end region or at the other coil end region. Each shoulder region has a greater thickness than the first thickness.
    • 一种用于构造这种类型的组件的导体组件和方法,其在传导电流时产生磁场,或者在存在变化的磁场的情况下产生电压。 在一个实施例中,该方法包括形成包括沿着第一孔径路径延伸的材料层的结构。 该结构包括多个同心层表面。 在材料的每个层中并且沿着多个表面中的每一个形成通道。 导电材料位于每个通道中以提供螺旋形结构。 多个层的表面是管状的。 材料层顺序地定位在另一个上并围绕形成第一和第二相对的线圈端部区域的轴线。 这些层形成有第一厚度的区域和肩部区域。 肩部区域以一个线圈端部区域或另一个线圈端部区域顺序交替地形成。 每个肩部区域具有比第一厚度更大的厚度。
    • 6. 发明申请
    • Helical Coil Design and Process For Direct Fabrication From A Conductive Layer
    • 螺旋线圈设计和从导电层直接制造的工艺
    • US20090206974A1
    • 2009-08-20
    • US12388306
    • 2009-02-18
    • Rainer Meinke
    • Rainer Meinke
    • H01F27/28H01F41/04
    • H01F7/202H01F5/00Y10T29/4902
    • A conductor assembly of the type which, when conducting current, generates a magnetic field or in which, in the presence of a changing magnetic field, a voltage is induced. According to an exemplary embodiment a conductor is positioned along a path of variable direction relative to a reference axis. The conductor has a width measurable along an outer surface thereof and along a series of different planes transverse to the path direction. The measured conductor width varies among the different planes. In one example, the conductor path is helical, positioned about the axis between turns of helical spaces, and the conductor width varies as a function of the azimuth angle.
    • 一种导体组件,其在传导电流时产生磁场,或者在存在变化的磁场的情况下产生电压。 根据示例性实施例,导体相对于参考轴沿着可变方向的路径定位。 导体具有可沿其外表面测量的宽度,并沿横向于路径方向的一系列不同平面测量。 测量的导体宽度在不同的平面之间变化。 在一个示例中,导体路径是螺旋形的,围绕螺旋空间的匝之间的轴定位,并且导体宽度随方位角的函数而变化。
    • 10. 发明授权
    • Magnetic coil capable of simultaneously providing multiple multipole orders with an improved transfer function
    • 能够同时提供具有改进的传递函数的多个多极次序的磁线圈
    • US07872562B2
    • 2011-01-18
    • US12473549
    • 2009-05-28
    • Rainer MeinkeCarl Goodzeit
    • Rainer MeinkeCarl Goodzeit
    • H01F27/28G06G7/16
    • G21K1/093H01F7/20Y10T29/49071
    • A method for constructing a conductor assembly of the type formed of one or more coil rows which, when conducting current, generate a magnetic field or in which, in the presence of a changing magnetic field, a voltage is induced. In one embodiment comprises forming a conductor pattern in a first coil row according to the relationship X(θ)=[h/(2*π)]θ+ΣAn sin(nθ+φn) Y(θ)=R cos(θ) Z(θ)=R sin(θ), the first coil row pattern suitable for simultaneously generating at least two multipole orthogonal field components of different orders, wherein: X is measurable along an X axis, Y is measurable along a Y axis and Z is measurable along a Z axis, the coil row extends along the X axis, the coil row is formed with a conductor configured in a series of turns about the X axis creating spaced-apart segments of the conductor such that, along first portions of the segments, individual segments are relatively straight and along second portions of the segments the segments follow a contour having a definable radius of curvature, the series of turns providing a geometrical configuration for generating a first multipole component of order n=i with An=Ai and φn=φi and a second multipole component of order n=j with An=Aj and φn=φj with φi not equal to φj.
    • 一种用于构造由一个或多个线圈列形成的类型的导体组件的方法,其在导电电流时产生磁场,或者在存在变化的磁场的情况下引起电压。 在一个实施例中包括根据关系X(&Thetas;)= [h /(2 *&pgr;)]&het; +&Sgr; An sin(n&thetas; +&phgr; n)Y 其中:X是可以沿着一个或多个第一线圈行模式测量的,其中:X(X) X轴,Y可沿着Y轴测量,Z可沿着Z轴测量,线圈列沿着X轴延伸,线圈排形成有绕X轴构成的一系列匝,形成间隔开的 导体的部分,使得沿着所述段的第一部分,各个段相对直的并且沿着所述段的第二部分,所述段遵循具有可定义的曲率半径的轮廓,所述一系列匝提供用于产生第一 An = Ai和&phgr; n =&phgr; i 和第n = j的第二多极分量,其中An = Aj和&phgr; n =&phgr; j与&phgr; i不等于&phgr; j。