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    • 3. 发明申请
    • Systems and Methods for Obstructing Magnetic Flux
    • 阻塞磁通的系统和方法
    • US20110133738A1
    • 2011-06-09
    • US12632208
    • 2009-12-07
    • Henry C. AbbinkEdward Kanegsberg
    • Henry C. AbbinkEdward Kanegsberg
    • G01R33/44
    • H05K9/00G01C19/60H05K13/00
    • An aspect of the present invention relates to system and method for substantially obstructing magnetic flux. One aspect of the present invention provides an apparatus for substantially obstructing at least one magnetic flux path between an ambient space and a protected volume. The apparatus includes an inner shield, substantially enclosing the protected volume. The inner shield has at least one inner shield aperture extending therethrough to allow external access to the protected volume. An outer shield substantially encloses the inner shield. The outer shield has at least one outer shield aperture extending therethrough to allow internal access from the ambient space. The apparatus is configured to impede magnetic flux between at least one inner shield aperture and at least one outer shield aperture.
    • 本发明的一个方面涉及用于基本上阻碍磁通量的系统和方法。 本发明的一个方面提供一种用于基本上阻挡环境空间和受保护体积之间的至少一个磁通路径的装置。 该装置包括基本上包围受保护体积的内屏蔽件。 内屏蔽件具有延伸穿过其中的至少一个内屏蔽孔,以允许外部访问受保护的体积。 外屏蔽件基本上包围内屏蔽。 外屏蔽件具有延伸穿过其中的至少一个外屏蔽孔,以允许从环境空间内部通路。 该装置被配置为阻止至少一个内屏蔽孔和至少一个外屏蔽孔之间的磁通量。
    • 4. 发明申请
    • Self-calibrating nuclear magnetic resonance gyro
    • 自校准核磁共振陀螺仪
    • US20090033329A1
    • 2009-02-05
    • US11888280
    • 2007-07-31
    • Robert E. StewartEdward Kanegsberg
    • Robert E. StewartEdward Kanegsberg
    • G01C19/60
    • G01C19/60G01C25/00
    • The method and apparatus in one embodiment may have: a gyro housing containing a bias field; a bias field that generates a stable axial magnetic field; Xenon or other gas contained within at least a portion of the axial magnetic field, Xenon or other gas nuclear spins precessing at a constant angular rate with respect to the gyro housing in response to the axial magnetic field; wherein reversing a polarity of the bias field reverses a polarity of the magnetic field and a polarity of the precession of the Xenon or other gas nuclear spin, and wherein a reversing of the polarity of the gyro scalefactor thereby results without reversing a polarity of the gyro bias.
    • 一个实施例中的方法和装置可以具有:包含偏置场的陀螺仪壳体; 产生稳定轴向磁场的偏置场; 包含在轴向磁场的至少一部分中的氙或其它气体,氙或其它气体核以相对于陀螺仪壳体以恒定角速率响应于轴向磁场而进动; 其中反转偏置场的极性反转了磁场的极性和氙气或其他气体核自旋的进动的极性,并且其中陀螺仪比例因子的极性反转从而导致陀螺仪的极性反转 偏压。
    • 5. 发明授权
    • Nuclear magnetic resonance gyroscope
    • 核磁共振陀螺仪
    • US07282910B1
    • 2007-10-16
    • US11406586
    • 2006-04-19
    • Edward Kanegsberg
    • Edward Kanegsberg
    • G01V3/00
    • G01R33/26G01C19/62G01C25/00
    • A method comprises the steps of providing a nuclear magnetic resonance cell with first, second, and third nuclear moment gases and at least one optically pumpable substance; obtaining first, second, and third measured precession frequencies that correspond to the first, second, and third nuclear moment gases, wherein the first, second, and third measured precession frequencies are altered from corresponding first, second, and third Larmor precession frequencies by a rotational rate and corresponding first, second, and third local magnetic fields; and determining the rotational rate with compensation for the first, second, and third local magnetic fields through employment of the first, second, and third measured precession frequencies.
    • 一种方法包括以下步骤:提供具有第一,第二和第三核力矩气体的核磁共振电池和至少一种可光学泵浦的物质; 获得对应于第一,第二和第三核时间气体的第一,第二和第三测量进动频率,其中第一,第二和第三测量的进动频率从对应的第一,第二和第三拉莫尔进动频率改变为 旋转速率和对应的第一,第二和第三局部磁场; 以及通过使用第一,第二和第三测量的进动频率来补偿第一,第二和第三局部磁场的旋转速率。
    • 6. 发明申请
    • SYSTEMS AND METHODS FOR OBSTRUCTING MAGNETIC FLUX
    • 阻塞磁通的系统和方法
    • US20130279144A1
    • 2013-10-24
    • US13926195
    • 2013-06-25
    • HENRY C. ABBINKEdward Kanegsberg
    • HENRY C. ABBINKEdward Kanegsberg
    • H05K9/00H05K13/00
    • H05K9/00G01C19/60H05K13/00Y10T29/49002
    • An aspect of the present invention relates to system and method for substantially obstructing magnetic flux. One aspect of the present invention provides an apparatus for substantially obstructing at least one magnetic flux path between an ambient space and a protected volume. The apparatus includes an inner shield, substantially enclosing the protected volume. The inner shield has at least one inner shield aperture extending therethrough to allow external access to the protected volume. An outer shield substantially encloses the inner shield. The outer shield has at least one outer shield aperture extending therethrough to allow internal access from the ambient space. The apparatus is configured to impede magnetic flux between at least one inner shield aperture and at least one outer shield aperture.
    • 本发明的一个方面涉及用于基本上阻碍磁通量的系统和方法。 本发明的一个方面提供一种用于基本上阻挡环境空间和受保护体积之间的至少一个磁通路径的装置。 该装置包括基本上包围受保护体积的内屏蔽件。 内屏蔽件具有延伸穿过其中的至少一个内屏蔽孔,以允许外部访问受保护的体积。 外屏蔽件基本上包围内屏蔽。 外屏蔽件具有延伸穿过其中的至少一个外屏蔽孔,以允许从环境空间内部通路。 该装置被配置为阻止至少一个内屏蔽孔和至少一个外屏蔽孔之间的磁通量。
    • 7. 发明授权
    • Systems and methods for obstructing magnetic flux while shielding a protected volume
    • 阻挡磁通量同时屏蔽受保护体积的系统和方法
    • US08552725B2
    • 2013-10-08
    • US12632208
    • 2009-12-07
    • Henry C. AbbinkEdward Kanegsberg
    • Henry C. AbbinkEdward Kanegsberg
    • G01C19/60G01R33/20
    • H05K9/00G01C19/60H05K13/00
    • An aspect of the present invention relates to system and method for substantially obstructing magnetic flux. One aspect of the present invention provides an apparatus for substantially obstructing at least one magnetic flux path between an ambient space and a protected volume. The apparatus includes an inner shield, substantially enclosing the protected volume. The inner shield has at least one inner shield aperture extending therethrough to allow external access to the protected volume. An outer shield substantially encloses the inner shield. The outer shield has at least one outer shield aperture extending therethrough to allow internal access from the ambient space. The apparatus is configured to impede magnetic flux between at least one inner shield aperture and at least one outer shield aperture.
    • 本发明的一个方面涉及用于基本上阻碍磁通量的系统和方法。 本发明的一个方面提供一种用于基本上阻挡环境空间和受保护体积之间的至少一个磁通路径的装置。 该装置包括基本上包围受保护体积的内屏蔽件。 内屏蔽件具有延伸穿过其中的至少一个内屏蔽孔,以允许外部访问受保护的体积。 外屏蔽件基本上包围内屏蔽。 外屏蔽件具有延伸穿过其中的至少一个外屏蔽孔,以允许从环境空间内部通路。 该装置被配置为阻止至少一个内屏蔽孔和至少一个外屏蔽孔之间的磁通量。
    • 9. 发明授权
    • Ring laser gyroscope scale factor error control apparatus and method
control apparatus and method
    • 环形激光陀螺仪比例因子误差控制装置及方法
    • US5442442A
    • 1995-08-15
    • US114481
    • 1987-10-28
    • Edward KanegsbergSteven C. GillespieJohn P. Rahn
    • Edward KanegsbergSteven C. GillespieJohn P. Rahn
    • G01C19/66G01B8/02H01S3/083
    • G01C19/66
    • The intensity and frequency variation due to retroscatter in a ring laser gyroscope are determined and used to correct the gyro scale factor. The orthogonal types of scatter due to dielectric variation and due to height variation, which lead to common mode phase delays of 0 and .pi./2 respectively are taken into account in calculating the correction to the scale factor. The scale factor errors are determined in terms of observable quantities. Scale factor error control is accomplished by extracting a portion of both of the two counterpropagating light beams and measuring their respective intensities, creating intensity modulation indices representative of the sum and difference intensities, using closed loop control of the real-time difference between the intensities of the beam in the ring laser gyro to reduce scale factor variation using push-pull mirror control of at least two mirrors. The residual error after push-pull mirror control minimization is output for use by a navigation system computer.
    • 确定环形激光陀螺仪中逆向散射的强度和频率变化,并用于校正陀螺仪比例因子。 在计算比例因子的校正时,考虑了由于电介质变化和由于高度变化导致的共模相位延迟0和pi / 2的正交分类的散射。 比例因子误差根据可观测量确定。 缩放因子误差控制是通过提取两个反向传播光束的一部分并测量它们各自的强度来实现的,使用闭环控制来产生表示和和强度的强度调制指数, 环形激光陀螺仪中的光束使用至少两个反射镜的推挽镜控制来减小比例因子变化。 输出推挽镜控制最小化后的残留误差,供导航系统计算机使用。
    • 10. 发明授权
    • Polarization analyzer orientation with nuclear magnetic resonance gyroscope
    • 使用核磁共振陀螺仪进行极化分析仪定向
    • US07936169B2
    • 2011-05-03
    • US12218298
    • 2008-07-14
    • Edward Kanegsberg
    • Edward Kanegsberg
    • G01V3/00
    • G01C19/62
    • An apparatus in one example comprises a polarization filter and a polarization analyzer. The polarization filter comprises a first polarization axis. The polarization analyzer comprises a second polarization axis. The polarization filter is configured to polarize detection light for a nuclear magnetic resonance (NMR) cell along the first polarization axis. The polarization analyzer is configured to receive the detection light from the NMR cell and pass a portion of the detection light to a processor for determination of angular rate information. The portion of the detection light passed to the processor is based on an orientation of the second polarization axis relative to the first polarization axis. The orientation is selected to maximize a signal-to-noise ratio of the detection light.
    • 一个示例中的装置包括偏振滤光器和偏振分析器。 偏振滤光器包括第一偏振轴。 偏振分析器包括第二偏振轴。 偏振滤光器被配置为沿着第一偏振轴极化用于核磁共振(NMR)单元的检测光。 偏振分析器被配置为从NMR单元接收检测光并将检测光的一部分传递到处理器以确定角速率信息。 传递到处理器的检测光的部分基于第二偏振轴相对于第一偏振轴的取向。 选择方向以最大化检测光的信噪比。