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    • 51. 发明申请
    • Method of non-destructively testing a work piece and non-destructive testing arrangement
    • 非破坏性测试工件和无损检测方法
    • US20080141778A1
    • 2008-06-19
    • US11998394
    • 2007-11-29
    • Thomas BosselmannHenrik Stiesdal
    • Thomas BosselmannHenrik Stiesdal
    • G01B15/00
    • G01B15/00G01N29/2493G01N29/4427G01N2291/044G01N2291/2693G01S13/878
    • A method of non-destructively testing a work piece is disclosed, wherein the work piece is placed within an active field of a positioning system; a frame of reference of the work piece is established based on the geometry of the work piece in the coordinates of the positioning system; the geometry of the work piece is detected by determining the position of specific transponders, which are fixed to the work piece, by the positioning system or the geometry of the work piece is detected by scanning at least parts of the contour of the work piece with a transponder of the positioning system; testing data is acquired for the work piece with a non-destructive testing probe, which comprises a transponder of the positioning system, while the position of the testing probe is recorded by the positioning system; the position of the testing probe is transformed into an intrinsic position defined with respect to the frame of reference of the work piece; and the intrinsic position of the testing probe is assigned to the testing data recorded at the respective position. Moreover, a non-destructive testing arrangement is provided.
    • 公开了一种对工件进行非破坏性测试的方法,其中工件被放置在定位系统的有效区域内; 基于在定位系统的坐标中的工件的几何形状建立工件的参考系; 通过定位系统确定固定在工件上的特定转发器的位置来检测工件的几何形状,或者通过用工件的几何形状扫描至少部分工件的轮廓来检测工件的几何形状, 定位系统的应答器; 使用非破坏性测试探针对工件获取测试数据,该测试探头包括定位系统的应答器,同时由定位系统记录测试探针的位置; 测试探针的位置被转换成相对于工件的参考框架限定的固有位置; 并且将测试探针的固有位置分配给记录在相应位置的测试数据。 此外,还提供了非破坏性的测试装置。
    • 53. 发明授权
    • Process and device for measuring an alternating electric current with
temperature compensation
    • 用温度补偿测量交流电流的过程和装置
    • US5847560A
    • 1998-12-08
    • US776830
    • 1997-03-07
    • Thomas BosselmannPeter Menke
    • Thomas BosselmannPeter Menke
    • G01R33/032G01R15/24G01R19/00G01R19/32G01R31/00
    • G01R15/246
    • Linearly polarized measuring light is broken down into two differently polarized component light signals in an analyzer after passing through a Faraday sensor device. The intensity of the corresponding electric intensity signals is normalized by dividing the respective alternating signal component by the respective direct signal component. From the two normalized intensity signals S1 and S2, a measuring signal is derived according to the formula: S=(2.multidot.S1.multidot.S2)/((S2-S1)+K.multidot.(S1+S2)) where cos(2.theta.+2.eta.)=-2/(3K) and sin(2.theta.-2.eta.)=1 are valid for a correction factor K, an injection angle .eta. between the plane of polarization of the injected measuring light to a natural axis of the linear birefringence in the sensor device and a exit angle .theta. between this natural axis and a natural axis of the analyzer.
    • PCT No.PCT / DE95 / 01138 Sec。 371日期1997年3月7日 102(e)1997年3月7日PCT PCT 1995年8月25日PCT公布。 出版物WO96 / 07922 日期:1996年3月14日在通过法拉第传感器装置后,将分离器中的线性偏振测量光分解成两个不同偏振分量光信号。 通过将相应的交变信号分量除以相应的直接信号分量来对相应的电强度信号的强度进行归一化。 根据两个归一化强度信号S1和S2,根据下式导出测量信号:S =(2xS1xS2)/((S2-S1)+ Kx(S1 + S2))其中cos(2θ+ 2 eta)= -2 /(3K)和sin(2θ-2 eta)= 1对于校正因子K有效,注入的测量光的偏振平面与传感器中的线性双折射的自然轴之间的注入角度eta 装置和该自然轴与分析器的自然轴之间的出射角θ。
    • 54. 发明授权
    • Method and device for measuring an electrical alternating quanity with
temperature compensation
    • 用温度补偿测量电气交流量的方法和装置
    • US5811964A
    • 1998-09-22
    • US624419
    • 1996-04-01
    • Thomas BosselmannPeter MenkeJoachim Niewisch
    • Thomas BosselmannPeter MenkeJoachim Niewisch
    • G01R33/032G01R15/24G01R19/00
    • G01R15/241G01R15/247G01R15/246
    • A polarized measuring light is provided to a sensing means under the influence of an alternating electrical quantity, the polarization of the measuring light changing as a function of the alternating electrical quantity. After passing through the sensing means, the measuring light is split into two differently polarized partial light signals, which are then converted into electrical intensity signals S1 and S2. An intensity-normalized signal P=(S1-S2)/(S1+S2) is then formed. A temperature-compensated measured signal can then be derived from the alternating signal component PAC and the direct signal component PDC of the intensity-normalized signal according to the equation S=(a*PAC+b*1)/(c*PDC+d*1). The temperature sensitivity can thus be reduced by a factor of ten.
    • PCT No.PCT / DE94 / 01104 Sec。 371日期:1996年4月1日 102(e)日期1996年4月1日PCT 1994年9月22日PCT公布。 WO95 / 10046 PCT公开号 日期1995年4月13日在交变电量的影响下,将偏振测量光提供给感测装置,测量光的极化作为交变电量的函数而变化。 在通过感测装置之后,将测量光分成两个不同偏振的部分光信号,然后转换成电强度信号S1和S2。 然后形成强度归一化信号P =(S1-S2)/(S1 + S2)。 然后可以根据等式S =(a * PAC + b * 1)/(c * PDC + d)从交流信号分量PAC和强度归一化信号的直接信号分量PDC导出温度补偿测量信号 * 1)。 因此,温度敏感度可以降低10倍。
    • 55. 发明申请
    • SYSTEM FOR DETERMINING EXHAUST GAS VOLUME
    • 用于确定排气量的系统
    • US20120180548A1
    • 2012-07-19
    • US13498727
    • 2010-09-28
    • Thomas Bosselmann
    • Thomas Bosselmann
    • G01F1/00G01N21/00
    • G01F1/6884G01P5/10G01P5/26
    • A system is disclosed, including: a plurality of Bragg gratings distributed in positions transversely to the direction of flow of an exhaust gas in an exhaust gas channel of the device; an optical wave guide structure including at least one optical wave guide and in which the Bragg gratings are embodied; a heating device arranged adjacently to the Bragg gratings and through which the Bragg gratings are subjected to heat, or a cooling device arranged adjacently to the Bragg gratings, through which the Bragg gratings are subjected to cold; at least one light source for irradiating light into the optical wave guide structure; and at least one signal processing device which determines, from light backscattered from Bragg gratings in the optical wave guide structure against its original direction of diffusion, the speed of the flow of the exhaust gas.
    • 公开了一种系统,包括:多个布拉格光栅,其布置在横向于设备的废气通道中的废气流动方向的位置; 包括至少一个光波导的光波导结构,其中实现布拉格光栅; 与布拉格光栅相邻设置的加热装置,布拉格光栅通过其加热,或布拉格光栅相邻设置的冷却装置,布拉格光栅通过该装置经受冷; 用于将光照射到所述光波导结构中的至少一个光源; 以及至少一个信号处理装置,其从光波导结构中的布拉格光栅的光背散射抵抗其原始扩散方向确定废气流的速度。
    • 56. 发明授权
    • Method of non-destructively testing a work piece and non-destructive testing arrangement
    • 非破坏性测试工件和无损检测方法
    • US07908923B2
    • 2011-03-22
    • US11998394
    • 2007-11-29
    • Thomas BosselmannHenrik Stiesdal
    • Thomas BosselmannHenrik Stiesdal
    • G01H1/00
    • G01B15/00G01N29/2493G01N29/4427G01N2291/044G01N2291/2693G01S13/878
    • A method of non-destructively testing a work piece is disclosed, wherein the work piece is placed within an active field of a positioning system; a frame of reference of the work piece is established based on the geometry of the work piece in the coordinates of the positioning system; the geometry of the work piece is detected by determining the position of specific transponders, which are fixed to the work piece, by the positioning system or the geometry of the work piece is detected by scanning at least parts of the contour of the work piece with a transponder of the positioning system; testing data is acquired for the work piece with a non-destructive testing probe, which comprises a transponder of the positioning system, while the position of the testing probe is recorded by the positioning system; the position of the testing probe is transformed into an intrinsic position defined with respect to the frame of reference of the work piece; and the intrinsic position of the testing probe is assigned to the testing data recorded at the respective position. Moreover, a non-destructive testing arrangement is provided.
    • 公开了一种对工件进行非破坏性测试的方法,其中工件被放置在定位系统的有效区域内; 基于在定位系统的坐标中的工件的几何形状建立工件的参考系; 通过定位系统确定固定在工件上的特定转发器的位置来检测工件的几何形状,或者通过用工件的几何形状扫描至少部分工件的轮廓来检测工件的几何形状, 定位系统的应答器; 使用非破坏性测试探针对工件获取测试数据,该测试探头包括定位系统的应答器,同时由定位系统记录测试探针的位置; 测试探针的位置被转换成相对于工件的参考框架限定的固有位置; 并且将测试探针的固有位置分配给记录在相应位置的测试数据。 此外,还提供了非破坏性的测试装置。