Geospace Perturbations that Accompanied Rocket Launches from the Baikonur Cosmodrome

IF 0.5 4区 物理与天体物理 Q4 ASTRONOMY & ASTROPHYSICS Kinematics and Physics of Celestial Bodies Pub Date : 2022-12-08 DOI:10.3103/S0884591322060046
Y. Luo, L. F. Chernogor, Y. H. Zhdanko
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Abstract

The launch of a rocket requires an energy comparable to the energy of many natural processes. For large rockets, the energy release reaches 10–100 TJ, and the power of engines reaches 0.1–1 TW. The energy release per unit volume is much higher than the specific energy content and energy release of all natural processes. During the launch and flight of a large rocket, disturbances in the substratum, the atmosphere, the ionosphere, and even in the magnetosphere occur. Effects from rocket engine burns have been studied for more than 60 years. Research results have been published in hundreds of articles, handbooks, and monographs. It turns out that the effects produced exhibit diverse geophysical phenomena. The effects near the rocket trajectory, namely, the regions of depressed electron density (ionospheric holes), and the generation of infrasound and atmospheric gravity waves (density waves) are investigated better than other effects. Great attention has been paid to studying the geomagnetic effect. The following methods have been used in studies: the Doppler effect, the Faraday, incoherent scattering, ionosonde, magnetometric methods, etc. The effects accompanying the launches and flights of rockets are being actively studied even now. For many years, large-scale (1 to 10 Mm) disturbances that occur after rocket launches have been studied. Their study makes it possible to better understand the mechanisms of the propagation of disturbances from a rocket over global distances, the interaction of subsystems in the Earth–atmosphere–ionosphere–magnetosphere system, and the ecological consequences of rocket engine burns. Disturbances occurring in the atmosphere and geospace substantially depend on the state of the atmospheric–space weather, time of day, season, and phase of the solar cycle. Even with the launch of two identical rockets, disturbances in the mentioned system can be very different. It should be borne in mind that rockets differ in power, trajectories, fuel composition, and the location of cosmodromes. Therefore, studying the response of subsystems to rocket launches and flights remains an urgent problem. The purpose of this study is to describe the results of an analysis of the ionospheric effects of the Soyuz and Proton rockets launched during the 24th cycle of solar activity from the Baikonur Cosmodrome. To observe the effects in the ionosphere caused by the launch of the Soyuz and Proton rockets from the Baikonur Cosmodrome, a vertical sounding Doppler radar was used. As a rule, measurements are carried out at two fixed frequencies of 3.2 and 4.2 MHz. The smaller of them is effective when studying the dynamic processes in the E and F1 layers, and the larger one is effective when studying the F1 and F2 layers. The parameters of ionospheric disturbances that followed the launches of 81 Soyuz rockets and 53 Proton rockets from the Baikonur Cosmodrome in 2009–2021 are analyzed. It is confirmed that there are several groups of delay times for the possible reaction of the ionosphere to the launch and flight of the rockets. These delay times varied widely (from 10 to 300 min). The delay time groups correspond to several groups of apparent horizontal velocities of disturbance propagation (100–200, 390 ± 23 m/s, 0.97 ± 0.10, 1.28 ± 0.13, 1.68 ± 0.13, 2.07 ± 0.13 km/s, and approximately 8 km/s). Slow atmospheric gravity waves, atmospheric gravity waves of man-made origin, density shock waves, slow, and ordinary MHD waves have such velocities. As a rule, the generated perturbations (except for shock waves) are quasi-periodic in behavior with a period in the range from 5 to 20 min. The amplitude of the Doppler shift is 0.1–0.3 Hz. The relative amplitude of quasi-periodic variations in the electron density is typically 1‒10% and rarely reaches 20%.

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伴随火箭从拜科努尔航天发射场发射的地球空间扰动
发射火箭所需的能量与许多自然过程的能量相当。对于大型火箭,能量释放达到10-100 TJ,发动机功率达到0.1-1 TW。单位体积释放的能量远远高于所有自然过程的比能含量和能量释放。在大型火箭的发射和飞行过程中,基底、大气、电离层甚至磁层都会发生扰动。火箭发动机燃烧的影响已经研究了60多年。研究成果已发表在数百篇文章、手册和专著中。事实证明,产生的影响表现出多种地球物理现象。在火箭轨道附近,即电子密度下降区域(电离层空穴)、次声和大气重力波(密度波)的产生等方面的影响较好。地磁效应的研究一直受到人们的高度重视。研究中常用的方法有:多普勒效应、法拉第、非相干散射、离子探空、磁强法等。伴随火箭发射和飞行的影响至今仍在积极研究中。多年来,人们一直在研究火箭发射后发生的大尺度(1至10毫米)扰动。他们的研究使人们有可能更好地理解火箭在全球范围内传播干扰的机制,地球-大气-电离层-磁层系统中子系统的相互作用,以及火箭发动机燃烧的生态后果。发生在大气和地球空间的扰动在很大程度上取决于大气-空间天气的状态、一天中的时间、季节和太阳活动周期的阶段。即使发射两枚相同的火箭,上述系统中的干扰也可能非常不同。应当铭记,火箭在功率、轨迹、燃料组成和航天发射场的位置上各不相同。因此,研究子系统对火箭发射和飞行的响应是一个迫切需要解决的问题。本研究的目的是描述在太阳活动第24个周期从拜科努尔航天发射场发射的联盟号和质子号火箭的电离层效应分析的结果。为了观测从拜科努尔航天发射场发射的联盟号和质子号火箭对电离层的影响,使用了垂直探测多普勒雷达。通常,测量是在3.2和4.2 MHz两个固定频率下进行的。其中较小的一个在研究E层和F1层的动态过程时有效,较大的一个在研究F1层和F2层的动态过程时有效。分析了2009-2021年拜科努尔航天发射场发射81枚联盟号火箭和53枚质子号火箭后的电离层扰动参数。证实了电离层对火箭发射和飞行的可能反应有几组延迟时间。这些延迟时间变化很大(从10分钟到300分钟)。延迟时间组对应于扰动传播的几组视水平速度(100 - 200,390±23 m/s, 0.97±0.10,1.28±0.13,1.68±0.13,2.07±0.13 km/s和约8 km/s)。大气慢重力波、人造大气重力波、密度激波、慢重力波和普通MHD波都有这样的速度。通常,产生的扰动(激波除外)具有准周期行为,周期范围为5至20分钟。多普勒频移的幅度为0.1-0.3 Hz。电子密度准周期变化的相对幅度一般为1-10%,很少达到20%。
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来源期刊
Kinematics and Physics of Celestial Bodies
Kinematics and Physics of Celestial Bodies ASTRONOMY & ASTROPHYSICS-
CiteScore
0.90
自引率
40.00%
发文量
24
审稿时长
>12 weeks
期刊介绍: Kinematics and Physics of Celestial Bodies is an international peer reviewed journal that publishes original regular and review papers on positional and theoretical astronomy, Earth’s rotation and geodynamics, dynamics and physics of bodies of the Solar System, solar physics, physics of stars and interstellar medium, structure and dynamics of the Galaxy, extragalactic astronomy, atmospheric optics and astronomical climate, instruments and devices, and mathematical processing of astronomical information. The journal welcomes manuscripts from all countries in the English or Russian language.
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