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首页> 外文期刊>Review of Scientific Instruments >Rubidium Vapor Magnetometer for Near Earth Orbiting Spacecraft
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Rubidium Vapor Magnetometer for Near Earth Orbiting Spacecraft

机译:用于近地轨道航天器的Va蒸气磁强计

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This paper describes the instrumentation and in‐flight performance of the rubidium vapor magnetometers being flown by the National Aeronautics and Space Administration on the POGO satellites. An optically pumped, self‐oscillating rubidium magnetometer was selected as being most compatible with the objectives of the study and with the spacecraft capabilities. A four absorption cell configuration is used to reduce the effect of the null zones inherent in these instruments and to obtain accuracies compatible with the scientific objectives of the program. Scalar magnetic field data are obtained in both digital (PCM) and analog (frequency multiplex) form. Instrument performance parameters are monitored through both main frame and subcommutated PCM data. The first instrument orbited was aboard OGO‐II which was launched on 14 October 1965. This instrument has returned a large quantity of data, and is still operating when sufficient spacecraft power is available. The accuracy of the data is determined, apart from orbit accuracy, by spurious phase shifts within the instrument. These arise from such sources as optical axis misalignment, electronic nonlinearities and frequency dependence, and propagation delay over the long cables connecting sensor and electronics. The magnitude of the resulting error is inversely proportional to the phase slope of the dual cell absorption line. The total effect in the POGO instrument of these sources of error is an accuracy of better than 1.5γ over the entire instrument range of 15 000 to 64 000γ.
机译:本文介绍了美国国家航空航天局在POGO卫星上飞行的vapor蒸气磁力计的仪器和飞行中的性能。选择了一种光泵浦,自激振荡的magnet磁力计,因为它与研究目的和航天器功能最兼容。四个吸收池配置用于减少这些仪器固有的零位区域的影响,并获得与程序的科学目标兼容的精度。标量磁场数据以数字(PCM)和模拟(频率复用)形式获得。仪器性能参数通过主机架和子换相PCM数据进行监控。第一个绕行仪器是1965年10月14日发射的OGO-II号。该仪器返回了大量数据,并且在有足够的航天器功率时仍在运行。除轨道精度外,数据的精度还取决于仪器内部的伪相移。这些是由于光轴未对准,电子非线性和频率依赖性以及连接传感器和电子设备的长电缆上的传播延迟等原因引起的。结果误差的大小与双电池吸收线的相位斜率成反比。这些误差源在POGO仪器中的总效果是,在15 000至64 000γ的整个仪器范围内,其精度均优于1.5γ。

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