Regarding the Theory of Power Lines Emission Propagation to the Space
The analytical theory is presented that describes the propagation of power lines emission (PLE) with frequency of 50/60 Hz in the heights range from the Earth surface to the magnetosphere. Validation of the theory is made by the comparison with earlier published results of numerical modeling. It is...
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description | The analytical theory is presented that describes the propagation of power lines emission (PLE) with frequency of 50/60 Hz in the heights range from the Earth surface to the magnetosphere. Validation of the theory is made by the comparison with earlier published results of numerical modeling. It is shown that the actual source of emission is a magnetic dipole formed by the power line current and by the secondary image current in the ground. The emission is propagating to the lower boundary of ionosphere, where its main part is reflected back, but some of the energy (a few percent) penetrates into the ionosphere. There it is transformed into a quasi‐flat whistler wave. The generation of current in ground and the reflection from the ionosphere are the main factors that reduce the emission into space. In the ionosphere wave fronts propagate approximately vertically, and the energy propagates in a certain direction that depends on the geomagnetic field inclination. Thus, the ionosphere acts as a focusing system that collects PLE into a unidirectional beam. The PLE intensity does not change with altitude within the total range of ionospheric heights. In the magnetosphere PLE is transformed to both magnetosonic and Alfvén waves and the emission splits into two rays: one propagates along the wave vector and the other one—along the geomagnetic field lines. A set of analytical solutions is presented allowing determining the change in PLE parameters with altitude depending on the source parameters and ionospheric conditions.
Plain Language Summary
The Earth's electromagnetic environment is influenced by both natural and human activities. Currently, there is a noticeable increase in human‐induced activity in the near space, and its potential environmental effects are hard to predict. Among the various forms of electromagnetic waves in the extra‐low frequency range that travel from Earth into space, the most common is the emission from power lines operating at industrial frequencies of 50/60 Hz. Recently, satellites have been able to detect this emission, offering a promising opportunity for remotely observing and assessing the characteristics of terrestrial sources of electrical energy, including those that are hidden. This paper presents an analytical theory that describes the propagation of this emission from the Earth's surface to the magnetosphere. Initially, the emission behaves like a conventional radio wave, traveling through the neutral atmosphere at nearly t |
doi_str_mv | 10.1029/2023JA031668 |
format | Article |
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Plain Language Summary
The Earth's electromagnetic environment is influenced by both natural and human activities. Currently, there is a noticeable increase in human‐induced activity in the near space, and its potential environmental effects are hard to predict. Among the various forms of electromagnetic waves in the extra‐low frequency range that travel from Earth into space, the most common is the emission from power lines operating at industrial frequencies of 50/60 Hz. Recently, satellites have been able to detect this emission, offering a promising opportunity for remotely observing and assessing the characteristics of terrestrial sources of electrical energy, including those that are hidden. This paper presents an analytical theory that describes the propagation of this emission from the Earth's surface to the magnetosphere. Initially, the emission behaves like a conventional radio wave, traveling through the neutral atmosphere at nearly the speed of light. However, as it ascends and undergoes multiple transformations in the ionosphere layers, it transitions into slow plasma waves of the magnetohydrodynamic nature. The paper provides a set of analytical solutions that enable the determination of emission parameters based on source characteristics and conditions along the wave's propagation path.
Key Points
The analytical theory of the propagation of 50/60 Hz electromagnetic emission from the Earth surface to the magnetosphere is presented
At ionospheric heights this emission turns into whistler‐wave, and then, in the magnetosphere, into magnetohydrodynamic waves
The generation of image current in ground and the reflection from the bottom of the ionosphere are the factors that reduce energy emission to space</description><identifier>ISSN: 2169-9380</identifier><identifier>EISSN: 2169-9402</identifier><identifier>DOI: 10.1029/2023JA031668</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Alfven waves ; Altitude ; Earth ; Earth magnetosphere ; Earth surface ; Electromagnetic radiation ; ELF ; Emission analysis ; Emissions ; Environmental effects ; Exact solutions ; Frequency ranges ; Geomagnetic field ; Geomagnetism ; Ionosphere ; Ionospheric conditions ; Ionospheric propagation ; Line current ; Magnetic dipoles ; Magnetohydrodynamic waves ; Numerical models ; Parameters ; Plasma waves ; Power lines ; power lines emission ; Propagation ; Radio waves ; Remote observing ; space electrodynamics ; Wave fronts ; Whistler waves</subject><ispartof>Journal of geophysical research. Space physics, 2023-12, Vol.128 (12), p.n/a</ispartof><rights>2023. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3076-1649dad63ce5c677cbb0d5394c3659036a09805c82e049a9cc26a37ad313b4183</citedby><cites>FETCH-LOGICAL-c3076-1649dad63ce5c677cbb0d5394c3659036a09805c82e049a9cc26a37ad313b4183</cites><orcidid>0000-0002-3399-7623 ; 0000-0002-4922-1248 ; 0000-0001-8260-1720</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2023JA031668$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2023JA031668$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1417,27924,27925,45574,45575</link.rule.ids></links><search><creatorcontrib>Lizunov, G.</creatorcontrib><creatorcontrib>Korepanov, V.</creatorcontrib><creatorcontrib>Piankova, O.</creatorcontrib><title>Regarding the Theory of Power Lines Emission Propagation to the Space</title><title>Journal of geophysical research. Space physics</title><description>The analytical theory is presented that describes the propagation of power lines emission (PLE) with frequency of 50/60 Hz in the heights range from the Earth surface to the magnetosphere. Validation of the theory is made by the comparison with earlier published results of numerical modeling. It is shown that the actual source of emission is a magnetic dipole formed by the power line current and by the secondary image current in the ground. The emission is propagating to the lower boundary of ionosphere, where its main part is reflected back, but some of the energy (a few percent) penetrates into the ionosphere. There it is transformed into a quasi‐flat whistler wave. The generation of current in ground and the reflection from the ionosphere are the main factors that reduce the emission into space. In the ionosphere wave fronts propagate approximately vertically, and the energy propagates in a certain direction that depends on the geomagnetic field inclination. Thus, the ionosphere acts as a focusing system that collects PLE into a unidirectional beam. The PLE intensity does not change with altitude within the total range of ionospheric heights. In the magnetosphere PLE is transformed to both magnetosonic and Alfvén waves and the emission splits into two rays: one propagates along the wave vector and the other one—along the geomagnetic field lines. A set of analytical solutions is presented allowing determining the change in PLE parameters with altitude depending on the source parameters and ionospheric conditions.
Plain Language Summary
The Earth's electromagnetic environment is influenced by both natural and human activities. Currently, there is a noticeable increase in human‐induced activity in the near space, and its potential environmental effects are hard to predict. Among the various forms of electromagnetic waves in the extra‐low frequency range that travel from Earth into space, the most common is the emission from power lines operating at industrial frequencies of 50/60 Hz. Recently, satellites have been able to detect this emission, offering a promising opportunity for remotely observing and assessing the characteristics of terrestrial sources of electrical energy, including those that are hidden. This paper presents an analytical theory that describes the propagation of this emission from the Earth's surface to the magnetosphere. Initially, the emission behaves like a conventional radio wave, traveling through the neutral atmosphere at nearly the speed of light. However, as it ascends and undergoes multiple transformations in the ionosphere layers, it transitions into slow plasma waves of the magnetohydrodynamic nature. The paper provides a set of analytical solutions that enable the determination of emission parameters based on source characteristics and conditions along the wave's propagation path.
Key Points
The analytical theory of the propagation of 50/60 Hz electromagnetic emission from the Earth surface to the magnetosphere is presented
At ionospheric heights this emission turns into whistler‐wave, and then, in the magnetosphere, into magnetohydrodynamic waves
The generation of image current in ground and the reflection from the bottom of the ionosphere are the factors that reduce energy emission to space</description><subject>Alfven waves</subject><subject>Altitude</subject><subject>Earth</subject><subject>Earth magnetosphere</subject><subject>Earth surface</subject><subject>Electromagnetic radiation</subject><subject>ELF</subject><subject>Emission analysis</subject><subject>Emissions</subject><subject>Environmental effects</subject><subject>Exact solutions</subject><subject>Frequency ranges</subject><subject>Geomagnetic field</subject><subject>Geomagnetism</subject><subject>Ionosphere</subject><subject>Ionospheric conditions</subject><subject>Ionospheric propagation</subject><subject>Line current</subject><subject>Magnetic dipoles</subject><subject>Magnetohydrodynamic waves</subject><subject>Numerical models</subject><subject>Parameters</subject><subject>Plasma waves</subject><subject>Power lines</subject><subject>power lines emission</subject><subject>Propagation</subject><subject>Radio waves</subject><subject>Remote observing</subject><subject>space electrodynamics</subject><subject>Wave fronts</subject><subject>Whistler waves</subject><issn>2169-9380</issn><issn>2169-9402</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kEFrAjEQhUNpoWK99QcEeu22k0w2mxxFrFaEirXnJWajruhmm6yI_75rbaGnzmUew_fmwSPknsETA66fOXCc9AGZlOqKdDiTOtEC-PWvRgW3pBfjFtpR7YmlHTKcu7UJRVmtabNxdLFxPpyoX9GZP7pAp2XlIh3uyxhLX9FZ8LVZm-asG__teK-NdXfkZmV20fV-dpd8vAwXg3EyfRu9DvrTxCJkMmFS6MIUEq1Lrcwyu1xCkaIWFmWqAaUBrSC1ijsQ2mhruTSYmQIZLgVT2CUPl7918J8HF5t86w-haiNzrkGkGjMQLfV4oWzwMQa3yutQ7k045Qzyc1f5365aHC_4sdy5079sPhnN-6liWuIXf_toAA</recordid><startdate>202312</startdate><enddate>202312</enddate><creator>Lizunov, G.</creator><creator>Korepanov, V.</creator><creator>Piankova, O.</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>8FD</scope><scope>H8D</scope><scope>KL.</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-3399-7623</orcidid><orcidid>https://orcid.org/0000-0002-4922-1248</orcidid><orcidid>https://orcid.org/0000-0001-8260-1720</orcidid></search><sort><creationdate>202312</creationdate><title>Regarding the Theory of Power Lines Emission Propagation to the Space</title><author>Lizunov, G. ; Korepanov, V. ; Piankova, O.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3076-1649dad63ce5c677cbb0d5394c3659036a09805c82e049a9cc26a37ad313b4183</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Alfven waves</topic><topic>Altitude</topic><topic>Earth</topic><topic>Earth magnetosphere</topic><topic>Earth surface</topic><topic>Electromagnetic radiation</topic><topic>ELF</topic><topic>Emission analysis</topic><topic>Emissions</topic><topic>Environmental effects</topic><topic>Exact solutions</topic><topic>Frequency ranges</topic><topic>Geomagnetic field</topic><topic>Geomagnetism</topic><topic>Ionosphere</topic><topic>Ionospheric conditions</topic><topic>Ionospheric propagation</topic><topic>Line current</topic><topic>Magnetic dipoles</topic><topic>Magnetohydrodynamic waves</topic><topic>Numerical models</topic><topic>Parameters</topic><topic>Plasma waves</topic><topic>Power lines</topic><topic>power lines emission</topic><topic>Propagation</topic><topic>Radio waves</topic><topic>Remote observing</topic><topic>space electrodynamics</topic><topic>Wave fronts</topic><topic>Whistler waves</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Lizunov, G.</creatorcontrib><creatorcontrib>Korepanov, V.</creatorcontrib><creatorcontrib>Piankova, O.</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of geophysical research. Space physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Lizunov, G.</au><au>Korepanov, V.</au><au>Piankova, O.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Regarding the Theory of Power Lines Emission Propagation to the Space</atitle><jtitle>Journal of geophysical research. Space physics</jtitle><date>2023-12</date><risdate>2023</risdate><volume>128</volume><issue>12</issue><epage>n/a</epage><issn>2169-9380</issn><eissn>2169-9402</eissn><abstract>The analytical theory is presented that describes the propagation of power lines emission (PLE) with frequency of 50/60 Hz in the heights range from the Earth surface to the magnetosphere. Validation of the theory is made by the comparison with earlier published results of numerical modeling. It is shown that the actual source of emission is a magnetic dipole formed by the power line current and by the secondary image current in the ground. The emission is propagating to the lower boundary of ionosphere, where its main part is reflected back, but some of the energy (a few percent) penetrates into the ionosphere. There it is transformed into a quasi‐flat whistler wave. The generation of current in ground and the reflection from the ionosphere are the main factors that reduce the emission into space. In the ionosphere wave fronts propagate approximately vertically, and the energy propagates in a certain direction that depends on the geomagnetic field inclination. Thus, the ionosphere acts as a focusing system that collects PLE into a unidirectional beam. The PLE intensity does not change with altitude within the total range of ionospheric heights. In the magnetosphere PLE is transformed to both magnetosonic and Alfvén waves and the emission splits into two rays: one propagates along the wave vector and the other one—along the geomagnetic field lines. A set of analytical solutions is presented allowing determining the change in PLE parameters with altitude depending on the source parameters and ionospheric conditions.
Plain Language Summary
The Earth's electromagnetic environment is influenced by both natural and human activities. Currently, there is a noticeable increase in human‐induced activity in the near space, and its potential environmental effects are hard to predict. Among the various forms of electromagnetic waves in the extra‐low frequency range that travel from Earth into space, the most common is the emission from power lines operating at industrial frequencies of 50/60 Hz. Recently, satellites have been able to detect this emission, offering a promising opportunity for remotely observing and assessing the characteristics of terrestrial sources of electrical energy, including those that are hidden. This paper presents an analytical theory that describes the propagation of this emission from the Earth's surface to the magnetosphere. Initially, the emission behaves like a conventional radio wave, traveling through the neutral atmosphere at nearly the speed of light. However, as it ascends and undergoes multiple transformations in the ionosphere layers, it transitions into slow plasma waves of the magnetohydrodynamic nature. The paper provides a set of analytical solutions that enable the determination of emission parameters based on source characteristics and conditions along the wave's propagation path.
Key Points
The analytical theory of the propagation of 50/60 Hz electromagnetic emission from the Earth surface to the magnetosphere is presented
At ionospheric heights this emission turns into whistler‐wave, and then, in the magnetosphere, into magnetohydrodynamic waves
The generation of image current in ground and the reflection from the bottom of the ionosphere are the factors that reduce energy emission to space</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1029/2023JA031668</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0002-3399-7623</orcidid><orcidid>https://orcid.org/0000-0002-4922-1248</orcidid><orcidid>https://orcid.org/0000-0001-8260-1720</orcidid></addata></record> |
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subjects | Alfven waves Altitude Earth Earth magnetosphere Earth surface Electromagnetic radiation ELF Emission analysis Emissions Environmental effects Exact solutions Frequency ranges Geomagnetic field Geomagnetism Ionosphere Ionospheric conditions Ionospheric propagation Line current Magnetic dipoles Magnetohydrodynamic waves Numerical models Parameters Plasma waves Power lines power lines emission Propagation Radio waves Remote observing space electrodynamics Wave fronts Whistler waves |
title | Regarding the Theory of Power Lines Emission Propagation to the Space |
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