首页> 外文会议>Conference on Asteroids, Comets, Meteors ACM 2002 Jul 29-Aug 2, 2002 Berlin, Germany >THE SIMULATION APPROACH TOWARDS DEFINING THE TRANSITION FACTOR BETWEEN THE NUMBER OF RADIO REFLECTIONS OF THE REGISTRATION THRESHOLD PRESET ABOVE AND THE DENSITY OF THE METEORIC PARTICLE FLOW OF THE ABOVE SET MASS
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THE SIMULATION APPROACH TOWARDS DEFINING THE TRANSITION FACTOR BETWEEN THE NUMBER OF RADIO REFLECTIONS OF THE REGISTRATION THRESHOLD PRESET ABOVE AND THE DENSITY OF THE METEORIC PARTICLE FLOW OF THE ABOVE SET MASS

机译:确定上述登记阈值的无线电反射次数与上述设定质量的平均粒子流密度之间的转换因子的模拟方法

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This work presents the solution of a problem occurring when the density distribution of the meteoric particle Q(m_0, ε, ψ) flow obtained by the radar method is calculated. Normally, the initial distribution is a distribution of a number of registrations with the amplitude higher that the threshold value N (U>U_0 , ε, ψ) throughout the entire coelosphere or in its northern part for a radar located in the northern hemisphere. In the course of transition to the above set mass a physical model of a meteor and meteoric radio reflection is introduced. When the deterministic method of solving the problem is used it is necessary to fix some characteristics, e.g. the initial radius value r_0 or evaporation height of the meteoroid h_0. It is almost impossible to consider the effect of these simplifications. In the approach that we suggest the transition between the numbers of radio reflection is implemented by the simulation method using the simulation computer model "KAMET" thus avoiding ungrounded simplifications.
机译:这项工作提出了一个问题的解决方案,该问题是在计算通过雷达方法获得的流变粒子Q(m_0,ε,ψ)流的密度分布时出现的。通常,初始分布是在整个北半球或其北部的雷达中,位于北半球的,数量级高于阈值N(U> U_0,ε,ψ)的多个配准的分布。在过渡到上述设定质量的过程中,引入了流星和流星无线电反射的物理模型。当使用确定性的方法来解决问题时,有必要固定一些特性,例如初始半径值r_0或流星体h_0的蒸发高度。几乎不可能考虑这些简化的效果。在我们建议的方法中,通过使用模拟计算机模型“ KAMET”的模拟方法可以实现无线电反射次数之间的转换,从而避免了不切实际的简化。

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