Characteristic Features of the Magnetic and Ionospheric Storms on December 21–24, 2016

IF 0.5 4区 物理与天体物理 Q4 ASTRONOMY & ASTROPHYSICS Kinematics and Physics of Celestial Bodies Pub Date : 2022-09-19 DOI:10.3103/S0884591322050051
Y. Luo, L. F. Chernogor
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This will contribute to a process of their adequate simulation and, in the long term, forecasting. The purpose of this article is to describe the observed features of the ionospheric and magnetic storms accompanying the geospace storm on December 21–24, 2016. The state of the geomagnetic field has been observed via the fluxgate magnetometer located at the Magnetometer Observatory of the Karazin Kharkiv National University (49°38′ N, 36°56′ E). The dynamics of the ionospheric plasma has been monitored by a vertical incidence Doppler radar and a digisonde located at the Radio Physics Observatory of the Karazin Kharkiv National University (49°38′ N, 36°20′ E). The Doppler radar operate at 3.2 and 4.2 MHz; however, only measurements performed at 3.2 MHz are given below, since a frequency of 4.2 MHz turned out to be inefficient at nighttime when F2 layer critical frequency median <i>f</i><sub>0 F2</sub> ≈ 2 MHz, which prevented signal reflection from the ionosphere even at 3.2 MHz. Prior to the beginning of the magnetic storm on December 20, 2016, the level of the <i>H</i> and <i>D</i> components rarely exceeded 0.2–0.7 nT. The sudden commencement of a storm between 06:00 and 10:00 UTC virtually did not affect this level. During the second half of the day on December 21, 2016, the level of exhibited sporadic fluctuations increased from approximately 1 to 3–4 nT. During the next few days, up to December 25, 2016, their level showed variations mostly from approximately 1 nT to approximately 2 nT. Increases in the level were predominantly observed in the period from 05:00 to 15:00 UTC for the <i>H</i> component and from 10:00 to 20:00 UTC for the <i>D</i> component. The weak (power 20 GJ/s and energy approximately 0.45 PJ) geospace storm in the period of December 21–24, 2016, was accompanied by a moderate positive ionospheric storm, as well as by three negative ionospheric storms, one of which was very strong, and the other two were strong and moderate. The geospace storm was accompanied by a moderate magnetic storm with an energy of approximately 2 PJ and a power of approximately 56 GW. The positive ionospheric storm barely affects the level of the signal reflected from the ionosphere, whereas the reflected signal may be very weak or totally absent during the negative ionospheric storms. The positive ionospheric storm has a substantial effect on the Doppler shift when the wave activity enhanced in the ionosphere. The relative amplitude of disturbances in the electron density increases from a few percent to approximately 50%, and their period increases from 6–12 to 40 min. It is impossible to follow wave activity during the negative ionospheric storms. In the course of a long magnetic storm, the level of <i>D</i> and <i>H</i> components in a subrange of 200–1000 s of the period increased from 0.2–0.3 and 0.3–0.5 nT to 1.0–2.0 and 1.0–1.8 nT, respectively. In a subrange of 50–200 s of the period, the corresponding levels increased from 0.3–0.5 and 0.3–0.5 nT to 0.5–1.0 and 1.5–2.0 nT, respectively. Within a subrange of 10–50 s the period, the corresponding levels increased from 0.05–0.06 and 0.10–0.15 nT to 0.20–0.30 and 0.5–1.0 nT, respectively. Comparative studies of two geospace storms that occurred on December 21–24, 2016, and March 21–23, 2017, show that their ionospheric and magnetic effects are comparable, even if the storms are different.</p>","PeriodicalId":681,"journal":{"name":"Kinematics and Physics of Celestial Bodies","volume":null,"pages":null},"PeriodicalIF":0.5000,"publicationDate":"2022-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Kinematics and Physics of Celestial Bodies","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.3103/S0884591322050051","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
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Abstract

Solar storms accompanied by solar flares, coronal mass ejections, and high-speed flows result in considerable disturbances in the Sun–interplanetary medium–magnetosphere–ionosphere–atmosphere–Earth (internal geospheres) system. As a result, geospace storms with synergistically interacting magnetic, ionospheric, atmospheric, and electrical storms arise in our planet. Magnetic and ionospheric storms have been studied for a long time, but atmospheric storms and electrical storms have been studied considerably to a less extent. Geospace storms and their components exhibit significant variability. It may be asserted that no identical two storms exist. Therefore, a comprehensive study of each new geospace storm and its manifestations and features is an urgent scientific issue. This will contribute to a process of their adequate simulation and, in the long term, forecasting. The purpose of this article is to describe the observed features of the ionospheric and magnetic storms accompanying the geospace storm on December 21–24, 2016. The state of the geomagnetic field has been observed via the fluxgate magnetometer located at the Magnetometer Observatory of the Karazin Kharkiv National University (49°38′ N, 36°56′ E). The dynamics of the ionospheric plasma has been monitored by a vertical incidence Doppler radar and a digisonde located at the Radio Physics Observatory of the Karazin Kharkiv National University (49°38′ N, 36°20′ E). The Doppler radar operate at 3.2 and 4.2 MHz; however, only measurements performed at 3.2 MHz are given below, since a frequency of 4.2 MHz turned out to be inefficient at nighttime when F2 layer critical frequency median f0 F2 ≈ 2 MHz, which prevented signal reflection from the ionosphere even at 3.2 MHz. Prior to the beginning of the magnetic storm on December 20, 2016, the level of the H and D components rarely exceeded 0.2–0.7 nT. The sudden commencement of a storm between 06:00 and 10:00 UTC virtually did not affect this level. During the second half of the day on December 21, 2016, the level of exhibited sporadic fluctuations increased from approximately 1 to 3–4 nT. During the next few days, up to December 25, 2016, their level showed variations mostly from approximately 1 nT to approximately 2 nT. Increases in the level were predominantly observed in the period from 05:00 to 15:00 UTC for the H component and from 10:00 to 20:00 UTC for the D component. The weak (power 20 GJ/s and energy approximately 0.45 PJ) geospace storm in the period of December 21–24, 2016, was accompanied by a moderate positive ionospheric storm, as well as by three negative ionospheric storms, one of which was very strong, and the other two were strong and moderate. The geospace storm was accompanied by a moderate magnetic storm with an energy of approximately 2 PJ and a power of approximately 56 GW. The positive ionospheric storm barely affects the level of the signal reflected from the ionosphere, whereas the reflected signal may be very weak or totally absent during the negative ionospheric storms. The positive ionospheric storm has a substantial effect on the Doppler shift when the wave activity enhanced in the ionosphere. The relative amplitude of disturbances in the electron density increases from a few percent to approximately 50%, and their period increases from 6–12 to 40 min. It is impossible to follow wave activity during the negative ionospheric storms. In the course of a long magnetic storm, the level of D and H components in a subrange of 200–1000 s of the period increased from 0.2–0.3 and 0.3–0.5 nT to 1.0–2.0 and 1.0–1.8 nT, respectively. In a subrange of 50–200 s of the period, the corresponding levels increased from 0.3–0.5 and 0.3–0.5 nT to 0.5–1.0 and 1.5–2.0 nT, respectively. Within a subrange of 10–50 s the period, the corresponding levels increased from 0.05–0.06 and 0.10–0.15 nT to 0.20–0.30 and 0.5–1.0 nT, respectively. Comparative studies of two geospace storms that occurred on December 21–24, 2016, and March 21–23, 2017, show that their ionospheric and magnetic effects are comparable, even if the storms are different.

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2016年12月21-24日磁暴和电离层风暴特征
伴随着太阳耀斑、日冕物质抛射和高速流的太阳风暴在太阳-行星际介质-磁层-电离层-大气-地球(内部地圈)系统中造成相当大的干扰。因此,地球空间风暴与磁场、电离层、大气和电风暴协同作用,在我们的星球上出现。对磁暴和电离层风暴的研究已经有很长一段时间了,但是对大气风暴和电风暴的研究相对较少。地球空间风暴及其成分表现出显著的可变性。可以断言,不存在完全相同的两个风暴。因此,全面研究每一次新的地球空间风暴及其表现和特征是一个迫切需要解决的科学问题。这将有助于对它们进行充分的模拟,并在长期内进行预测。本文的目的是描述2016年12月21日至24日伴随地球空间风暴的电离层和磁暴的观测特征。通过位于卡拉津哈尔科夫国立大学磁力计观测站(49°38 ' N, 36°56 ' E)的磁通门磁强计观测了地磁场的状态。电离层等离子体的动力学由位于卡拉津哈尔科夫国立大学射电物理观测站(49°38 ' N, 36°20 ' E)的垂直入射多普勒雷达和digisonde监测。多普勒雷达工作在3.2和4.2 MHz;然而,下面只给出了在3.2 MHz下进行的测量,因为4.2 MHz的频率在夜间F2层临界频率中值f0 F2≈2 MHz时被证明是低效的,这即使在3.2 MHz时也阻止了电离层的信号反射。在2016年12月20日磁暴开始之前,H和D分量的水平很少超过0.2-0.7 nT,在UTC时间06:00 - 10:00之间突然开始的磁暴几乎没有影响到这个水平。在2016年12月21日的下半日,其水平表现出零星波动,从约1 nT增加到3-4 nT。在接下来的几天里,直到2016年12月25日,其水平变化主要在约1 nT到约2 nT之间。H分量的水平增加主要发生在05:00 - 15:00 UTC和10:00 - 20:00 UTC。在2016年12月21日至24日期间,弱地球空间风暴(功率20 GJ/s,能量约0.45 PJ)伴有1次中等正电离层风暴,以及3次负电离层风暴,其中1次很强,另外2次为强中。地球空间风暴伴随着中等强度的磁暴,能量约为2 PJ,功率约为56 GW。正电离层风暴几乎不影响电离层反射信号的水平,而负电离层风暴期间反射信号可能非常弱或完全没有。当电离层波活动增强时,正电离层风暴对多普勒频移有显著影响。电子密度扰动的相对振幅从几个百分点增加到大约50%,其周期从6-12分钟增加到40分钟。在负电离层风暴期间,不可能跟踪波的活动。在长时间磁暴过程中,200 ~ 1000s区间内D分量和H分量的水平分别由0.2 ~ 0.3和0.3 ~ 0.5 nT增加到1.0 ~ 2.0和1.0 ~ 1.8 nT。在50 ~ 200s的区间内,相应的水平分别从0.3 ~ 0.5和0.3 ~ 0.5 nT上升到0.5 ~ 1.0和1.5 ~ 2.0 nT。在10 ~ 50 s的区间内,相应的水平分别从0.05 ~ 0.06和0.10 ~ 0.15 nT上升到0.20 ~ 0.30和0.5 ~ 1.0 nT。对2016年12月21日至24日和2017年3月21日至23日发生的两次地球空间风暴的对比研究表明,即使风暴不同,它们的电离层和磁效应也具有可比性。
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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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