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    • 2. 发明申请
    • PROCESS AND DEVICE FOR MEASURING AN ALTERNATING ELECTRIC QUANTITY WITH TEMPERATURE COMPENSATION
    • 方法和装置用于测量电气变化,SIZE带温度补偿
    • WO1996011409A1
    • 1996-04-18
    • PCT/DE1995001332
    • 1995-09-26
    • SIEMENS AKTIENGESELLSCHAFTBOSSELMANN, ThomasMENKE, Peter
    • SIEMENS AKTIENGESELLSCHAFT
    • G01R15/24
    • G01R15/247
    • Polarised measuring light (L) is coupled into a sensor device (3) and, after passing through the sensor device (3), divided into two differently linearly polarised partial light signals (L1, L2) in an analyser (7). The intensity of the corresponding electric intensity signals (I1, I2) is standardised by the division of their alternating signal component by their direct signal component. From the two standardised intensity signals S1 and S2 is derived a temperature-compensated measurement signal M in accordance with the two equations S1 = f1(T)*M and S2 = f2(T)*M in which f1(T) and f2(T) are predetermined, especially linear, squared or exponential fit functions of the temperature T. The measurement signal M = A*S1+B*S2 is obtained in particular with linear fit functions f1(T) and f2(T).
    • 偏振测量光(L)被耦合到传感器装置(3)和通过传感器装置(3)到分析器(7)在拆开两个不同的线性偏振光的部分信号(L1,L2)之后。 相应的电场强度信号(I1,I2)的强度归一化,通过它们各自的直射信号分量除以它们各自的交变信号的部分。 从两个强度归一化的信号S1和S2中,根据两个方程S1 = F1(T)* M S2衍生= F2(T)* M,其中,f1(T)和f2(T)规定,特别是直链的温度补偿测量信号M 是温度T的方形或指数拟合函数 对于线性拟合函数F1(T)和f2(T)的结果特别是作为一个测量信号M = A * S1 + B * S2。
    • 5. 发明申请
    • PROCESS AND DEVICE FOR MEASURING AN ALTERNATING ELECTRIC CURRENT WITH TEMPERATURE COMPENSATION
    • 方法和设备测量电流交换带温度补偿
    • WO1996007922A1
    • 1996-03-14
    • PCT/DE1995001138
    • 1995-08-25
    • SIEMENS AKTIENGESELLSCHAFTBOSSELMANN, ThomasMENKE, Peter
    • SIEMENS AKTIENGESELLSCHAFT
    • G01R15/24
    • G01R15/246
    • After passing through a Faraday sensor device (3), linearly polarised measuring light (L) is broken down in an analyser (7) into two diffently polarised partial light signals (L1, L2). The intensity of the corresponding electric signals (I1, I2) is normal by dividing their alternating signal component by their direct signal component. A measuring signal S = (2*S1*S2)/((S2-S1)+K*(S1+S2)) is derived from the two normalised intensity signals, in which cos(2 theta +2 eta )=-2/(3K) and sin(2 theta -2 eta )=1 stand for a correction factor K, an injection angle eta between the polarisation plane of the injected measurement light (L) and a proper axis of the linear double-fraction in the sensor device (3) and a decoupling angle theta between this proper axis and a natural axis of the analyser (7).
    • 穿过法拉第传感器装置(3)进入分解(7)分成两个不同地极化的部分光信号(L1,L2)的分析仪后线性偏振的测量光(L)。 相应的电场强度信号(I1,I2)的强度归一化,通过它们各自的直射信号分量除以它们各自的交变信号的部分。 从两个强度归一化的信号S1和S2中,测量的信号S =(2 * S1 * S2)/((S2-S1)+ K *(S1 + S2))的导出,其中COS(2θ处2 ETA)= - 2 /(3K)和sin(2θ处-2 ETA)= 1适用于校正因子K,的偏振平面之间的输入耦合角度ETA耦合测量光(L),以在所述传感器装置中的线性双折射的固有轴(3)和这之间的输出耦合THETA 征轴和分析仪(7)的固有轴线。