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Mesospheric positive ion concentrations, mobilities, and loss rates obtained from rocket-borne Gerdien condenser measurements

机译:从火箭载格登冷凝器测量获得的中层阳离子浓度,迁移率和损失率

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摘要

The theory and operation of a Gerdien condenser in a collision-controlled regime is reviewed. Its operation under supersonic flow conditions is then presented and the results of calibration of the instrument in a wind tunnel are discussed. The theory of mobility is reviewed and the importance of a mean-free-path or mean-free-time model between ion-neutral collisions is discussed. Experimental positive ion mobility data are presented and compared with the data of Rose and Widdel [1972] and the extrapolated values of small ion laboratory results. The assumption of chemically frozen flow is then considered concerning the equilibrium distribution of the water cluster ions and their temperature-dependent decomposition rates. It is shown for flow at Mach 3 that when the shock is detached the dominant cluster ions are not frozen. However, when the shock is swallowed the H(H2O)3 ion is frozen at all altitudes above 40 km and the H(H2O)4 ion is frozen above 65 km. The predicted mobility of the dominant positive ions, i.e., H(H2O)3 and H(H2O)4, based on a mobility dispersion curve for nitrogen, is compared with experimental data. Positive ion density data are presented for four rocket flights during a PCA and one flight during an auroral absorption event. Finally, positive ion loss rates are shown based on the positive ion measurements and proton flux data obtained from rockets and satellites.
机译:本文综述了Gerdien冷凝器在碰撞控制下的理论和操作。然后介绍了它在超音速流动条件下的操作,并讨论了在风洞中仪器的校准结果。审查了迁移率的理论,并讨论了离子中性碰撞之间的平均路径或平均时间模型的重要性。给出了实验性阳离子迁移率数据,并将其与Rose和Widdel [1972]的数据以及小离子实验室结果的外推值进行了比较。然后考虑化学冻结流动的假设,涉及水簇离子的平衡分布及其与温度有关的分解速率。对于马赫数3处的流动显示,当消除冲击时,主要的簇离子不会冻结。但是,吞没电击时,H(H2O)3离子在高于40 km的所有海拔高度都被冻结,而H(H2O)4离子则被冻结在65 km以上的高度。基于氮的迁移率散布曲线,将占优势的正离子(即H(H2O)3和H(H2O)4)的预测迁移率与实验数据进行了比较。给出了PCA期间四次火箭飞行和极光吸收事件中一次飞行的正离子密度数据。最后,根据从火箭和卫星获得的正离子测量值和质子通量数据,显示正离子损失率。

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