Resonance Electromagnetic Effect of the Kamchatka Meteoroid

IF 0.5 4区 物理与天体物理 Q4 ASTRONOMY & ASTROPHYSICS
Y. Luo, L. F. Chernogor
{"title":"Resonance Electromagnetic Effect of the Kamchatka Meteoroid","authors":"Y. Luo,&nbsp;L. F. Chernogor","doi":"10.3103/S0884591323010051","DOIUrl":null,"url":null,"abstract":"<p>A large meteoroid entered the terrestrial atmosphere and exploded at an altitude of 26 km between the Kamchatka Peninsula and Alaska (geographic coordinates 56.9° N, 172.4° E) over the Bering Sea at 23:48:20 UT on December 18, 2018. The meteoroid has been named the Kamchatka (or Bering Sea) meteoroid. Its basic parameters are as follows: calculated total impact energy 173 kt of TNT, total optical radiated energy 1.3 × 10<sup>14</sup> J, mass 1.41 kt, speed 32 km/s, size 9.4 m, and the trajectory directed at an angle of 68.6° with respect to the horizon. The entry of the Kamchatka meteoroid into the atmosphere was accompanied by the generation of a transient resonance electromagnetic signal in the 25–35 mHz band observable in the vicinity of the meteoroid explosion and in the magnetically conjugate region. Oscillations with amplitudes of 0.2–0.8 nT were observed over a 7-min interval. This study is aimed at analyzing the observations of the resonance electromagnetic effect from the Kamchatka meteoroid and discussing a mechanism for this effect. The resonance effect in the Earth’s magnetic field is analyzed using data with a time resolution of 1 s and an amplitude resolution of 1 nT from the database collected by the Intermagnet magnetometer network of magnetic observatories. The distance between the site of the meteoroid explosion and the magnetic observatories ranges from 1000 to 5000 km in the Northern Hemisphere and from 9010 to 12 425 km in the Southern Hemisphere. It is established that the only feasible mechanism is associated with the magnetic field displacement in the magnetosphere by the explosive impact of the celestial body, whereas only a negligibly small part of the meteoroid’s energy is spent on the generation of magnetic field perturbations. The meteoroid’s energy losses are similar to the losses in the reactive components of the radio frequency circuits, i.e., they return into the system. The oscillations cease after the meteoroid flies by, and the system returns into the initial state. The main results are summarized as follows. The resonance electromagnetic oscillations arose at 13 and 3 min prior to the Kamchatka meteoroid explosion. The duration of each observed perturbation is close to 7 min. The parameters of the quasi-periodic perturbations are similar to the parameters of magnetic Pc3 pulsations; however, they occured in the <i>Y</i> component of the magnetic field rather than in the <i>X</i> component of the magnetic field. Their observed periods are in the range of 33–36 s, and the amplitudes are in the range of 0.4–0.9 nT. Similar resonance oscillations were also recorded in the magnetically conjugate region. A mechanism for generating the resonance oscillations is proposed. The essence of the mechanism is that the meteoroid explosively impacts the magnetosphere and deforms the magnetic field lines that begin to oscillate at their eigenfrequencies. Depending on the McIlwain <i>L</i>-shell, the calculated period of oscillations is 19–169 s. For example, a period of 28–34 s is obtained with setting <i>L</i> <i>≈</i> 3–3.2, which is close to the observed period of 30 s. The generation of the resonance oscillations consumes approximately 10<sup>–4</sup> parts of the meteoroid kinetic energy.</p>","PeriodicalId":681,"journal":{"name":"Kinematics and Physics of Celestial Bodies","volume":"39 1","pages":"1 - 9"},"PeriodicalIF":0.5000,"publicationDate":"2023-03-20","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/S0884591323010051","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}
引用次数: 0

Abstract

A large meteoroid entered the terrestrial atmosphere and exploded at an altitude of 26 km between the Kamchatka Peninsula and Alaska (geographic coordinates 56.9° N, 172.4° E) over the Bering Sea at 23:48:20 UT on December 18, 2018. The meteoroid has been named the Kamchatka (or Bering Sea) meteoroid. Its basic parameters are as follows: calculated total impact energy 173 kt of TNT, total optical radiated energy 1.3 × 1014 J, mass 1.41 kt, speed 32 km/s, size 9.4 m, and the trajectory directed at an angle of 68.6° with respect to the horizon. The entry of the Kamchatka meteoroid into the atmosphere was accompanied by the generation of a transient resonance electromagnetic signal in the 25–35 mHz band observable in the vicinity of the meteoroid explosion and in the magnetically conjugate region. Oscillations with amplitudes of 0.2–0.8 nT were observed over a 7-min interval. This study is aimed at analyzing the observations of the resonance electromagnetic effect from the Kamchatka meteoroid and discussing a mechanism for this effect. The resonance effect in the Earth’s magnetic field is analyzed using data with a time resolution of 1 s and an amplitude resolution of 1 nT from the database collected by the Intermagnet magnetometer network of magnetic observatories. The distance between the site of the meteoroid explosion and the magnetic observatories ranges from 1000 to 5000 km in the Northern Hemisphere and from 9010 to 12 425 km in the Southern Hemisphere. It is established that the only feasible mechanism is associated with the magnetic field displacement in the magnetosphere by the explosive impact of the celestial body, whereas only a negligibly small part of the meteoroid’s energy is spent on the generation of magnetic field perturbations. The meteoroid’s energy losses are similar to the losses in the reactive components of the radio frequency circuits, i.e., they return into the system. The oscillations cease after the meteoroid flies by, and the system returns into the initial state. The main results are summarized as follows. The resonance electromagnetic oscillations arose at 13 and 3 min prior to the Kamchatka meteoroid explosion. The duration of each observed perturbation is close to 7 min. The parameters of the quasi-periodic perturbations are similar to the parameters of magnetic Pc3 pulsations; however, they occured in the Y component of the magnetic field rather than in the X component of the magnetic field. Their observed periods are in the range of 33–36 s, and the amplitudes are in the range of 0.4–0.9 nT. Similar resonance oscillations were also recorded in the magnetically conjugate region. A mechanism for generating the resonance oscillations is proposed. The essence of the mechanism is that the meteoroid explosively impacts the magnetosphere and deforms the magnetic field lines that begin to oscillate at their eigenfrequencies. Depending on the McIlwain L-shell, the calculated period of oscillations is 19–169 s. For example, a period of 28–34 s is obtained with setting L 3–3.2, which is close to the observed period of 30 s. The generation of the resonance oscillations consumes approximately 10–4 parts of the meteoroid kinetic energy.

Abstract Image

堪察加流星体的共振电磁效应
2018年12月18日23时48分20秒,一颗大型流星体进入地球大气层,在白令海上空堪察加半岛和阿拉斯加(地理坐标56.9°N, 172.4°E)之间26公里的高空爆炸。该流星体被命名为堪察加(或白令海)流星体。其基本参数为:计算TNT总冲击能173 kt,总光辐射能1.3 × 1014 J,质量1.41 kt,速度32 km/s,尺寸9.4 m,弹道与地平线夹角68.6°。堪察加流星体进入大气层时,在流星体爆炸附近和磁共轭区产生了25-35 mHz频段的瞬态共振电磁信号。在7分钟的时间间隔内观察到振幅为0.2-0.8 nT的振荡。本研究旨在分析堪察加流星体的共振电磁效应观测结果,并探讨这种效应的机制。利用地磁观测站磁体间磁强计网络采集的时间分辨率为1 s、幅值分辨率为1 nT的数据,分析了地球磁场的共振效应。流星体爆炸地点与磁观测站之间的距离在北半球为1000至5000公里,在南半球为9010至12425公里。确定了唯一可行的机制与由天体爆炸撞击引起的磁层磁场位移有关,而流星体能量中只有很小一部分用于产生磁场扰动。流星体的能量损失类似于射频电路中无功元件的损失,即它们会返回到系统中。流星体经过后振荡停止,系统恢复到初始状态。主要研究结果总结如下:在堪察加流星体爆炸前13分钟和3分钟出现了共振电磁振荡。每次观测到的扰动持续时间接近7 min。准周期扰动的参数与磁性Pc3脉动的参数相似;然而,它们发生在磁场的Y分量,而不是磁场的X分量。它们的周期在33 ~ 36s之间,振幅在0.4 ~ 0.9 nT之间,在磁共轭区也记录到了类似的共振振荡。提出了产生共振振荡的机理。该机制的本质是流星体爆炸性地撞击磁层,使磁力线变形,使磁力线开始以其特征频率振荡。根据McIlwain l -壳的不同,计算出的振荡周期为19 ~ 169 s。例如,设L≈3-3.2,得到28-34 s的周期,与观测到的30 s的周期接近。共振振荡的产生大约消耗了流星体动能的10-4倍。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 求助全文
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.
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
确定
请完成安全验证×
copy
已复制链接
快去分享给好友吧!
我知道了
右上角分享
点击右上角分享
0
联系我们:info@booksci.cn Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。 Copyright © 2023 布克学术 All rights reserved.
京ICP备2023020795号-1
ghs 京公网安备 11010802042870号
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术官方微信