CN115600070B - Method for predicting polar orbit satellite encountering polar photoelectrons - Google Patents

Method for predicting polar orbit satellite encountering polar photoelectrons Download PDF

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CN115600070B
CN115600070B CN202211262559.2A CN202211262559A CN115600070B CN 115600070 B CN115600070 B CN 115600070B CN 202211262559 A CN202211262559 A CN 202211262559A CN 115600070 B CN115600070 B CN 115600070B
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呼延奇
修志杰
左平兵
沈自才
曲少杰
张志平
李佳英
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Abstract

本发明公开了一种极轨卫星遭遇极光电子的预示方法,包括:按固定的时间间隔,计算极轨卫星在轨运行的空间位置地理坐标;将极轨卫星的空间位置地理坐标转换为地磁坐标;基于极光带边界模型,输入地磁活动Kp指数,确定极光带区域的极向和赤道向边界;基于极轨卫星的地磁坐标和极光带区域,确定极轨卫星位于极光带区域内的轨道位置,得到极轨卫星位于极光带区域中的最长持续时间以及极轨卫星遭遇极光电子的概率。本发明可以实现对近地极轨卫星在不同地磁活动条件下遭遇极光电子的空间位置、持续时间及遭遇概率进行快速分析,为评估极轨卫星充放电风险提供依据。

Figure 202211262559

The invention discloses a prediction method for a polar-orbiting satellite encountering an aurora electron, comprising: calculating the spatial position geographic coordinates of the polar-orbiting satellite in orbit at a fixed time interval; converting the spatial position geographic coordinates of the polar-orbiting satellite into geomagnetic coordinates ; Based on the auroral belt boundary model, input the geomagnetic activity Kp index to determine the polar and equatorial boundaries of the auroral belt area; based on the geomagnetic coordinates of the polar orbiting satellite and the auroral belt area, determine the orbital position of the polar orbiting satellite in the auroral belt area, The longest duration of polar-orbiting satellites in the auroral belt area and the probability of polar-orbiting satellites encountering auroral electrons are obtained. The invention can quickly analyze the spatial position, duration and encounter probability of polar-orbiting satellites encountering auroral electrons under different geomagnetic activity conditions, and provide a basis for evaluating the charging and discharging risks of polar-orbiting satellites.

Figure 202211262559

Description

一种极轨卫星遭遇极光电子的预示方法A Forecasting Method for Polar Orbiting Satellites Encountering Auroral Electrons

技术领域technical field

本发明涉及极轨卫星技术领域,具体涉及一种极轨卫星遭遇极光电子的预示方法。The invention relates to the technical field of polar-orbiting satellites, in particular to a method for predicting when a polar-orbiting satellite encounters aurora electrons.

背景技术Background technique

极光是磁层粒子进入大气层激发大气发光的一种现象,在卫星俯拍的极光照片中可以清楚地看到,极光出现在一个环绕地磁极的卵圆形条带内,称做极光带。极光带距离地磁极约20°,略向夜晚一侧移动,其中,子夜附近极光出现最频繁,强度也最大。在南北两极区,可以同时观测到形态类似、演化过程也类似的南极光和北极光,这是磁层粒子沿同一磁力线分别沉降到南北极区所激发的共轭极光现象。The aurora is a phenomenon in which particles in the magnetosphere enter the atmosphere and stimulate the atmosphere to emit light. It can be clearly seen in the aurora photos taken by satellites. The aurora appears in an oval strip surrounding the magnetic poles of the earth, called the auroral belt. The auroral belt is about 20° away from the geomagnetic pole and moves slightly to the night side. Among them, the aurora appears most frequently and has the greatest intensity near midnight. In the northern and southern polar regions, the southern and northern lights with similar shapes and similar evolution processes can be observed at the same time. This is the phenomenon of conjugate aurora excited by magnetospheric particles falling to the north and south poles along the same magnetic force line.

引发极光的沉降粒子(尤其是电子)可以作用到运行于近地极轨的卫星表面,带来表面充放电效应风险。Fallout particles (especially electrons) that cause aurora can act on the surface of satellites operating in low-Earth polar orbits, bringing the risk of surface charging and discharging effects.

在低地球轨道上,太阳紫外辐射可以电离地球中性大气中的氧和氮原子,形成等离子体。由于LEO轨道上的等离子体主要来源于太阳紫外辐射的电离作用,故等离子体密度随太阳活动周以及地方时不同而存在差异。通常情况下,在LEO轨道上的电离层冷等离子体一般不会造成严重的卫星充电问题,但是在地磁活动期间,从磁尾注入的keV量级的热等离子体可以沿着地球磁力线注入到极区很低的高度上,近地极轨卫星可能会遭遇这些热等离子体,尤其是其中的电子则可能对卫星带来严重的充电问题。目前运行于近地极轨的美国国防气象卫星DMSP(轨道约840km、倾角99°)在轨实测的数据显示,在两极极光带区域(地磁纬度55°-75°)可能遭遇的极光沉降电子能量可以达到数keV量级。需要特别指出的是,由于地球两极磁力线的汇聚作用,使得极光沉降电子的通量可能会明显超过GEO轨道。In low Earth orbit, solar ultraviolet radiation can ionize oxygen and nitrogen atoms in Earth's neutral atmosphere, forming a plasma. Since the plasma in the LEO orbit mainly comes from the ionization of solar ultraviolet radiation, the plasma density varies with the solar cycle and local time. Normally, the ionospheric cool plasma in the LEO orbit generally does not cause serious satellite charging problems, but during geomagnetic activity, the hot plasma of the keV level injected from the magnetotail can be injected into the poles along the Earth's magnetic field lines. At very low altitudes, low-Earth polar-orbiting satellites may encounter these hot plasmas, and especially the electrons in them may cause serious charging problems for the satellites. The on-orbit data measured by the U.S. Defense Meteorological Satellite DMSP (orbit about 840km, inclination 99°) currently operating in a near-Earth polar orbit shows that the energy of auroral sedimentation electrons that may be encountered in the two-pole auroral belt area (magnetic latitude 55°-75°) It can reach the order of several keV. It should be pointed out that due to the convergence of the magnetic field lines at the two poles of the earth, the flux of electrons deposited in the aurora may obviously exceed the GEO orbit.

目前在工程应用领域,缺少对极轨卫星在两极区可能遭遇极光沉降电子位置及持续时间的预示方法。At present, in the field of engineering applications, there is a lack of prediction methods for the location and duration of polar-orbiting satellites that may encounter auroral sinking electrons in the polar regions.

发明内容Contents of the invention

针对现有技术中存在的上述问题,本发明提供一种极轨卫星遭遇极光电子的预示方法。Aiming at the above-mentioned problems existing in the prior art, the present invention provides a method for predicting when a polar-orbiting satellite encounters an auroral electron.

本发明公开了一种极轨卫星遭遇极光电子的预示方法,包括:The invention discloses a method for predicting that a polar-orbiting satellite encounters an aurora electron, comprising:

按固定的时间间隔,计算极轨卫星在轨运行的空间位置地理坐标;Calculate the geographic coordinates of the space position of the polar-orbiting satellite in orbit at a fixed time interval;

将极轨卫星的空间位置地理坐标转换为地磁坐标;Convert the spatial location geographic coordinates of polar-orbiting satellites into geomagnetic coordinates;

基于极光带边界模型,输入地磁活动Kp指数,确定极光带区域的极向和赤道向边界;Based on the boundary model of the auroral zone, the geomagnetic activity Kp index is input to determine the polar and equatorial boundaries of the auroral zone;

基于极轨卫星的地磁坐标和极光带区域坐标,确定极轨卫星位于极光带内的轨道位置,统计得出极轨卫星位于极光带内的最长持续时间以及极轨卫星遭遇极光电子的概率。Based on the geomagnetic coordinates of the polar-orbiting satellites and the coordinates of the auroral belt area, the orbital position of the polar-orbiting satellites in the auroral belt is determined, and the longest duration of the polar-orbiting satellites in the auroral belt and the probability of polar-orbiting satellites encountering auroral electrons are obtained statistically.

作为本发明的进一步改进,所述计算极轨卫星在轨运行的空间位置地理坐标,包括:As a further improvement of the present invention, the calculation of the spatial position geographical coordinates of the polar-orbiting satellite in orbit includes:

获取极轨卫星的轨道参数;其中,所述轨道参数包括近地点高度、远地点高度和倾角;Obtaining orbit parameters of polar-orbiting satellites; wherein, the orbit parameters include perigee height, apogee height and inclination;

将极轨卫星的轨道参数输入到SGP4轨道计算程序中,按照固定的时间间隔,输出极轨卫星在轨道上不同时刻的空间位置地理坐标;其中,所述空间位置地理坐标包括经度、纬度和高度;优选,固定的时间间隔为60s,一天输出1440个极轨卫星在轨道上的空间位置地理坐标点。Input the orbit parameters of the polar-orbiting satellites into the SGP4 orbit calculation program, and output the spatial position geographic coordinates of the polar-orbiting satellites at different times on the orbit according to a fixed time interval; wherein, the spatial position geographic coordinates include longitude, latitude and altitude ; Preferably, the fixed time interval is 60s, and 1440 geographic coordinate points of the spatial positions of polar-orbiting satellites in orbit are output in one day.

作为本发明的进一步改进,所述将极轨卫星的空间位置地理坐标转换为地磁坐标,包括:As a further improvement of the present invention, the conversion of the spatial position geographic coordinates of the polar-orbiting satellites into geomagnetic coordinates includes:

基于地磁坐标计算程序将极轨卫星的空间位置地理坐标转换为极光带模型所采用的地磁坐标,获得极轨卫星在地磁坐标系下的磁地方时信息;优选,可在地磁坐标系上转换得到1440个极轨卫星的地磁坐标点。Based on the geomagnetic coordinate calculation program, the spatial position geographic coordinates of the polar-orbiting satellites are converted into the geomagnetic coordinates adopted by the aurora belt model, and the magnetic local time information of the polar-orbiting satellites in the geomagnetic coordinate system is obtained; preferably, it can be converted on the geomagnetic coordinate system. Geomagnetic coordinate points of 1440 polar orbiting satellites.

作为本发明的进一步改进,极光带区域的极向和赤道向边界的计算公式为:As a further improvement of the present invention, the calculation formulas for the polar and equatorial boundaries of the auroral belt region are:

θm=A0m+A1m cos[15(t+α1m)]+A2m cos[15(2t+α2m)]+A3m cos[15(3t+α3m)]θ m =A 0m +A 1m cos[15(t+α 1m )]+A 2m cos[15(2t+α 2m )]+A 3m cos[15(3t+α 3m )]

Figure BDA0003891781820000031
Figure BDA0003891781820000031

AL=18-12.3Kp+27.2Kp2-2Kp3 AL=18-12.3Kp+27.2Kp 2 -2Kp 3

式中,m=0或1,分别对应极向和赤道向;θm为极向或赤道向边界地磁纬度,即θ0为极光带区域的极向边界地磁纬度,θ1为极光带区域的赤道向边界地磁纬度;t是磁地方时,Aim和αim分别表示随地磁纬度的振幅和以十进制数小时数表示的相位,方程的系数Aim和αim为AL指数的三阶多项式,i取0~3,表示阶数,对于每一个Aim和αim都有一系列系数bim值。;AL指数用于描述极光活动期间的地磁扰动强度,AL指数可以通过Kp指数计算得出,Kp指数的范围为0到9,0表示地磁活动十分平静,5或者大于5表示处于地磁暴状态; Kp指数为中纬度全球范围3小时地磁场水平分量最大扰动的平均值;输入的地磁Kp指数可根据实际需求进行选择,若需实现对未来某天(如明天)的预测,可采用未来地磁Kp指数得预报值,并基于Kp指数,确定极光带区域的极向和赤道向边界;若需实现对极轨卫星遭遇极光电子的最长持续时间及概率的最坏情况评估,则可选取Kp指数的最大值作为输入参数。In the formula, m = 0 or 1 , corresponding to the polar direction and the equatorial direction respectively; The geomagnetic latitude of the equator toward the boundary; when t is the magnetic place, A im and α im respectively represent the amplitude with the geomagnetic latitude and the phase expressed in decimal hours, and the coefficients A im and α im of the equation are third-order polynomials of the AL index, i takes 0-3, which means the order, and there are a series of coefficient b im values for each A im and α im . ;The AL index is used to describe the intensity of geomagnetic disturbance during the auroral activity. The AL index can be calculated by the Kp index. The Kp index ranges from 0 to 9. 0 means that the geomagnetic activity is very calm, and 5 or greater than 5 means that it is in a state of geomagnetic storm; The Kp index is the average value of the maximum disturbance of the horizontal component of the geomagnetic field in mid-latitudes for 3 hours around the world; the input geomagnetic Kp index can be selected according to actual needs. If you need to realize the prediction of a certain day in the future (such as tomorrow), you can use the future geomagnetic Kp The predicted value of the index, and based on the Kp index, determine the polar and equatorial boundaries of the auroral belt area; if it is necessary to realize the worst-case assessment of the longest duration and probability of polar-orbiting satellites encountering auroral electrons, the Kp index can be selected The maximum value of is used as an input parameter.

作为本发明的进一步改进,所述极轨卫星位于极光带区域中的最长持续时间的计算方法,包括:As a further improvement of the present invention, the calculation method for the longest duration of the polar-orbiting satellite in the auroral belt region includes:

统计极光带内卫星空间位置连续地磁坐标点;Count the continuous geomagnetic coordinate points of the satellite space position in the auroral belt;

选择卫星空间位置连续地磁坐标点最多的轨迹段;Select the track segment with the most continuous geomagnetic coordinate points in the satellite space position;

基于设定的固定时间间隔(60s)确定该轨迹段的总时长,即为极轨卫星位于极光带区域中的最长持续时间。The total duration of the trajectory segment is determined based on the set fixed time interval (60s), which is the longest duration of the polar-orbiting satellite in the auroral zone.

作为本发明的进一步改进,所述极轨卫星遭遇极光电子的概率的计算方法,包括:As a further improvement of the present invention, the calculation method of the probability that the polar-orbiting satellite encounters the auroral electrons includes:

获取一天内,极轨卫星所生成的所有空间位置地磁坐标点数量M;Obtain the number M of geomagnetic coordinate points of all spatial positions generated by polar-orbiting satellites within a day;

统计一天内,位于极光带区域内极轨卫星的所有坐标点N;Count all coordinate points N of polar-orbiting satellites located in the auroral belt area within one day;

计算极轨卫星遭遇极光电子的概率P=N/M。Calculate the probability P=N/M that the polar-orbiting satellite encounters the auroral electron.

与现有技术相比,本发明的有益效果为:Compared with prior art, the beneficial effect of the present invention is:

本发明通过确定不同地磁活动条件下极光带边界的位置,将极轨卫星轨道空间位置坐标转换为极光带分布的地磁坐标;基于此,可以实现对近地极轨卫星在不同地磁活动条件下遭遇极光电子的空间位置、持续时间及遭遇概率进行快速分析,为评估极轨卫星充放电风险提供依据。The present invention converts the space position coordinates of the polar-orbiting satellite into the geomagnetic coordinates of the distribution of the auroral belt by determining the position of the boundary of the auroral zone under different geomagnetic activity conditions; The spatial position, duration and encounter probability of Aurora Electronics are quickly analyzed to provide a basis for assessing the risk of charging and discharging of polar-orbiting satellites.

附图说明Description of drawings

图1为本发明一种实施例公开的极轨卫星遭遇极光电子的预示方法的流程图;Fig. 1 is a flow chart of a method for predicting a polar-orbiting satellite encountering an aurora electron disclosed in an embodiment of the present invention;

图2为本发明一种实施例公开的极光带边界与极轨卫星轨道运动星下点;Fig. 2 is the boundary of the aurora belt and the sub-satellite point of the orbital motion of the polar orbiting satellite disclosed by an embodiment of the present invention;

图3为本发明一种实施例公开的Kp=5条件下极轨卫星遭遇极光带情况。Fig. 3 is a situation where a polar-orbiting satellite encounters an auroral belt under the condition of Kp=5 disclosed by an embodiment of the present invention.

具体实施方式Detailed ways

为使本发明实施例的目的、技术方案和优点更加清楚,下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明的一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动的前提下所获得的所有其他实施例,都属于本发明保护的范围。In order to make the purpose, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the drawings in the embodiments of the present invention. Obviously, the described embodiments It is a part of embodiments of the present invention, but not all embodiments. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

下面结合附图且以1100km/86.4°的近地极轨卫星为例,对本发明做进一步的详细描述:Below in conjunction with accompanying drawing and take the low earth polar orbit satellite of 1100km/86.4 ° as an example, the present invention is described in further detail:

如图1所示,本发明提供一种1100km/86.4°的近地极轨卫星遭遇极光电子的预示方法,包括:As shown in Fig. 1, the present invention provides a kind of 1100km/86.4 ° low-Earth polar-orbiting satellite encounters the prediction method of aurora electron, comprises:

步骤1、获取近地极轨卫星的近地点高度、远地点高度和倾角等轨道参数;并将其顺序输入到SGP4轨道计算程序中,按60s的时间间隔,得到近地极轨卫星在轨道上不同时刻空间位置对应的经度、纬度和高度信息。Step 1. Obtain orbital parameters such as perigee height, apogee height, and inclination angle of the near-Earth polar-orbiting satellite; and input them into the SGP4 orbit calculation program in sequence, and obtain the orbital parameters of the near-Earth polar-orbiting satellite at different times in the orbit at a time interval of 60s The longitude, latitude, and altitude information corresponding to the spatial location.

步骤2、利用地磁坐标计算程序,将近地极轨卫星的空间位置地理坐标转换为地磁坐标,即基于近地极轨卫星在地理坐标系下的经度、纬度和高度信息得到近地极轨卫星在地磁坐标系下的磁地方时信息;其中,一天可得到1440 个极轨卫星的地磁坐标点。Step 2. Use the geomagnetic coordinate calculation program to convert the geographical coordinates of the spatial position of the near-Earth polar-orbiting satellite into geomagnetic coordinates, that is, based on the longitude, latitude and height information of the near-Earth polar-orbiting satellite in the geographic coordinate system, the position of the near-Earth polar-orbiting satellite is obtained. Magnetic local time information under the geomagnetic coordinate system; among them, the geomagnetic coordinate points of 1440 polar-orbiting satellites can be obtained in one day.

步骤3、利用Starkov提出的极光带边界模型,计算地磁Kp指数条件下,极光带区域的极向和赤道向边界;其中,Step 3. Using the auroral belt boundary model proposed by Starkov, calculate the polar and equatorial boundaries of the auroral belt region under the condition of the geomagnetic Kp index; where,

极光带边界模型依赖的地磁参数是AL指数,它描述极光活动期间的地磁扰动强度;AL指数可以由Kp指数计算得出,公式如下:The geomagnetic parameter that the auroral belt boundary model relies on is the AL index, which describes the intensity of geomagnetic disturbance during auroral activity; the AL index can be calculated from the Kp index, and the formula is as follows:

AL=18-12.3Kp+27.2Kp2-2Kp3 AL=18-12.3Kp+27.2Kp 2 -2Kp 3

模型给出的极光带边界θ(地磁纬度)可以表示为:The auroral belt boundary θ (geomagnetic latitude) given by the model can be expressed as:

θm=A0m+A1m cos[15(t+α1m)]+A2m cos[15(2t+α2m)]+A3m cos[15(3t+α3n)]θ m =A 0m +A 1m cos[15(t+α 1m )]+A 2m cos[15(2t+α 2m )]+A 3m cos[15(3t+α 3n )]

其中,Aim和αim分别表示随地磁纬度的振幅和以十进制数小时数表示的相位,t是磁地方时。m=0/1分别对应极向、赤道向极光边界。方程的系数Aim和αim为AL指数的三阶多项式:Among them, A im and α im represent the amplitude with geomagnetic latitude and the phase expressed in decimal hours, respectively, and t is the magnetic local time. m=0/1 correspond to polar and equatorial auroral boundaries respectively. The coefficients A im and α im of the equation are third-order polynomials of the AL index:

Figure BDA0003891781820000051
Figure BDA0003891781820000051

对于每一个Aim和αim都有一系列系数bim值;具体见表1所示。There are a series of coefficient b im values for each A im and α im ; see Table 1 for details.

表1Table 1

Figure BDA0003891781820000052
Figure BDA0003891781820000052

其中,如图2所示,本发明得到的上下两条波浪线(粗黑点)形成的区间分别为南北两极的极光带,细黑点为卫星轨道运动星下点,共计1440个星下点。如图3所示,其为Kp=5条件下卫星遭遇极光带情况,图中2条卵圆形条带围成极光带区域,*点为卫星轨道运动星下点。Wherein, as shown in Figure 2, the intervals formed by the upper and lower wavy lines (thick black dots) obtained by the present invention are respectively the auroral belts of the north and south poles, and the thin black dots are sub-satellite points of satellite orbital motion, a total of 1440 sub-satellite points . As shown in Figure 3, it is the case of the satellite encountering the auroral belt under the condition of Kp=5. In the figure, two oval strips enclose the auroral belt area, and the * point is the sub-satellite point of satellite orbital motion.

步骤4、基于极轨卫星的地磁坐标和极光带区域,确定极轨卫星位于极光带区域内的轨道位置,得到极轨卫星位于极光带区域中的最长持续时间以及极轨卫星遭遇极光电子的概率;Step 4. Based on the geomagnetic coordinates of the polar-orbiting satellite and the auroral belt area, determine the orbital position of the polar-orbiting satellite in the auroral belt area, and obtain the longest duration of the polar-orbiting satellite in the auroral belt area and the time at which the polar-orbiting satellite encounters aurora electrons probability;

具体的:specific:

极轨卫星位于极光带区域中的最长持续时间的计算方法,包括:The calculation method for the longest duration of a polar-orbiting satellite in the auroral belt area, including:

统计极光带区域内极轨卫星的空间位置连续地磁坐标点;Count the continuous geomagnetic coordinate points of the space position of the polar orbiting satellite in the auroral belt area;

选择卫星空间位置连续地磁坐标点最多的轨迹段;Select the track segment with the most continuous geomagnetic coordinate points in the satellite space position;

基于设定的固定时间间隔(60s)确定该轨迹段的总时长,即为极轨卫星位于极光带区域中的最长持续时间。The total duration of the trajectory segment is determined based on the set fixed time interval (60s), which is the longest duration of the polar-orbiting satellite in the auroral zone.

极轨卫星遭遇极光电子的概率的计算方法,包括:The calculation method for the probability of a polar-orbiting satellite encountering an auroral electron, including:

获取一天内,极轨卫星所生成的所有空间位置地磁坐标点数量M;Obtain the number M of geomagnetic coordinate points of all spatial positions generated by polar-orbiting satellites within a day;

统计一天内,位于极光带区域内极轨卫星的所有坐标点N;Count all coordinate points N of polar-orbiting satellites located in the auroral belt area within one day;

计算极轨卫星遭遇极光电子的概率P=N/M。Calculate the probability P=N/M that the polar-orbiting satellite encounters the auroral electron.

不同地磁Kp条件下,极轨卫星位于极光带区域中的最长持续时间以及极轨卫星遭遇极光沉降电子概率,如表2所示:Under different geomagnetic Kp conditions, the longest duration of polar-orbiting satellites in the auroral belt area and the probability of polar-orbiting satellites encountering auroral sedimentation electrons are shown in Table 2:

表2Table 2

最长持续时间maximum duration 遭遇极光带概率Probability of Encountering the Aurora Belt Kp=0Kp=0 4分钟4 minutes 3.9%3.9% Kp=5Kp=5 10分钟10 minutes 8.6%8.6% Kp=9Kp=9 10分钟10 minutes 10.3% 10.3%

本发明的优点为:The advantages of the present invention are:

本发明通过确定不同地磁活动条件下极光带边界的位置,将极轨卫星轨道空间位置坐标转换为极光带分布的地磁坐标;基于此,可以实现对近地极轨卫星在不同地磁活动条件下遭遇极光电子的空间位置、持续时间及遭遇概率进行快速分析,为评估极轨卫星充放电风险提供依据。The present invention converts the space position coordinates of the polar-orbiting satellite into the geomagnetic coordinates of the distribution of the auroral belt by determining the position of the boundary of the auroral zone under different geomagnetic activity conditions; The spatial position, duration and encounter probability of Aurora Electronics are quickly analyzed to provide a basis for assessing the risk of charging and discharging of polar-orbiting satellites.

以上仅为本发明的优选实施例而已,并不用于限制本发明,对于本领域的技术人员来说,本发明可以有各种更改和变化。凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。The above are only preferred embodiments of the present invention, and are not intended to limit the present invention. For those skilled in the art, the present invention may have various modifications and changes. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of the present invention shall be included within the protection scope of the present invention.

Claims (7)

1. A method for predicting polar satellite encounter with polar photoelectrons, comprising:
calculating the geographic coordinates of the in-orbit running space position of the polar orbit satellite according to a fixed time interval;
converting the space position geographic coordinates of the polar orbit satellite into geomagnetic coordinates;
inputting a geomagnetic activity Kp index based on the polar band boundary model, and determining polar and equatorial boundaries of a polar band region;
and determining the orbit position of the polar orbit satellite in the polar light band area based on the geomagnetic coordinates and the polar light band area coordinates of the polar orbit satellite, and counting the longest duration time of the polar orbit satellite in the polar light band and the probability of the polar orbit satellite encountering polar light electrons.
2. The method of predicting when a polar orbiting satellite encounters an aurora electronic as in claim 1, wherein said calculating the geospatial position of the orbital motion of the polar orbiting satellite comprises:
acquiring the orbit parameters of the polar orbit satellite; wherein the orbit parameters include a perigee height, a apogee height, and an inclination angle;
inputting the orbit parameters of the polar orbit satellite into an SGP4 orbit calculation program, and outputting the spatial position geographical coordinates of the polar orbit satellite at different moments on the orbit according to a fixed time interval; wherein the spatial location geographic coordinates include longitude, latitude, and altitude.
3. A method of predicting exposure of a polar satellite to an aurora of claim 2, wherein the fixed time interval is 60s.
4. The method of predicting polar orbiting satellite encounter with polar photoelectrons of claim 1, wherein said converting the spatial position geographical coordinates of the polar orbiting satellite into geomagnetic coordinates comprises:
and converting the space position geographical coordinates of the polar orbit satellite into geomagnetic coordinates adopted by the polar light band model based on a geomagnetic coordinate calculation program to obtain magnetic geotime information of the polar orbit satellite in a geomagnetic coordinate system.
5. The method of predicting the encounter of a polar satellite with an aurora electron according to claim 1, wherein the polar and equatorial boundaries of the aurora zone are calculated by the formula:
θ m =A 0m +A 1m cos[15(t+α 1m )]+A 2m cos[15(2t+α 2m )]+A 3m cos[15(3t+α 3m )]
Figure FDA0003891781810000011
AL=18-12.3Kp+27.2Kp 2 -2Kp 3
wherein m =0 or 1, respectively corresponding to the polar and equatorial directions; theta.theta. m The magnetic latitude of the polar or equatorial boundary, A im And alpha im Respectively representing the amplitude of the satellite magnetic latitude and the phase represented by decimal hours, and when t is the magnetic place, i is 0-3 to represent the order; AL is the intensity of the geomagnetic disturbance for each A im And alpha im All have a series of coefficients b im The value is obtained.
6. The method of predicting the encounter of a polar satellite with an aurora of claim 1, wherein the method of calculating the longest duration that the polar satellite is in an aurora zone comprises:
counting continuous geomagnetic coordinate points of the space positions of polar orbit satellites in the polar light band region;
selecting a track section with the most continuous geomagnetic coordinate points in the satellite space position;
the total duration of the trajectory segment is determined based on a set fixed time interval, i.e., the longest duration of the polar orbiting satellite in the polar band region.
7. The method for predicting the polar orbiting satellite encountering an aurora electron according to claim 1, wherein the method for calculating the probability that the polar orbiting satellite encounters an aurora electron comprises:
acquiring the number M of geomagnetic coordinate points of all spatial positions generated by a polar orbit satellite in one day;
counting all coordinate points N in the polar light band region within one day;
and calculating the probability P = N/M that the polar orbit satellite encounters the polar light electrons.
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