Impedance of a Spacecraft-Borne Antenna in the Magnetospheric Plasma and Quasi-Equilibrium Noise EMF in the Lower-Hybrid Frequency Band
We present analytical and numerical estimations of the value and frequency dependence of the impedance and noise electromotive force (EMF) in the context of the conditions which correspond to the trajectories and parameters of the antennas borne by geophysical monitoring satellites. The estimations...
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description | We present analytical and numerical estimations of the value and frequency dependence of the impedance and noise electromotive force (EMF) in the context of the conditions which correspond to the trajectories and parameters of the antennas borne by geophysical monitoring satellites. The estimations were obtained for two circular orbits at altitudes of 600 and 1200 km over the Earth’s surface in the frequency range from 20 to 120 kHz, which corresponded to the area of the lower-hybrid resonance, where a higher level of noise emissions is observed at the altitudes under consideration. It is shown that near the lower-hybrid resonance frequency, the real part of the antenna impedance is determined by the resonant “monopole” loss by radiation of quasipotential waves. In the nonresonant frequency band (at the frequencies below the frequency of the lowerhybrid resonance), the antenna reactance is determined by the transit loss, which is, however, low as compared with the resonant loss. When the noise was calculated, the medium was assumed to be a two-temperature plasma. The spectral density of the power of the noise EMF lies in the range
and is determined mainly by suprathermal electrons. In the nonresonant frequency band, the efficient temperature of noise radiation is equal to the temperature of the “cold” plasma component, and the antenna reactance is determined by the transit loss, i.e., the level of the noise EMF is low as compared with the EMF in the resonant frequency band. |
doi_str_mv | 10.1007/s11141-013-9416-2 |
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and is determined mainly by suprathermal electrons. In the nonresonant frequency band, the efficient temperature of noise radiation is equal to the temperature of the “cold” plasma component, and the antenna reactance is determined by the transit loss, i.e., the level of the noise EMF is low as compared with the EMF in the resonant frequency band.</description><identifier>ISSN: 0033-8443</identifier><identifier>EISSN: 1573-9120</identifier><identifier>DOI: 10.1007/s11141-013-9416-2</identifier><identifier>CODEN: RPQEAC</identifier><language>eng</language><publisher>Boston: Springer US</publisher><subject>Antennas ; Antennas (Electronics) ; Astronomy ; Astrophysics and Astroparticles ; EMF ; Frequency bands ; Hadrons ; Heavy Ions ; Impedance ; Lasers ; Mathematical analysis ; Mathematical and Computational Physics ; Noise ; Nuclear Physics ; Observations and Techniques ; Optical Devices ; Optics ; Orbits ; Photonics ; Physics ; Physics and Astronomy ; Quantum Optics ; Reactance ; Space ships ; Space vehicles ; Theoretical ; Transit</subject><ispartof>Radiophysics and quantum electronics, 2013-07, Vol.56 (2), p.61-77</ispartof><rights>Springer Science+Business Media New York 2013</rights><rights>COPYRIGHT 2013 Springer</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c340t-9c331efe1aace7d7826f5f8eb8f7b7365d6a4c7f11b348fa828564729a512dc93</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11141-013-9416-2$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11141-013-9416-2$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,41488,42557,51319</link.rule.ids></links><search><creatorcontrib>Chugunov, Yu. V.</creatorcontrib><creatorcontrib>Grach, V. S.</creatorcontrib><creatorcontrib>Pasmanik, D. L.</creatorcontrib><title>Impedance of a Spacecraft-Borne Antenna in the Magnetospheric Plasma and Quasi-Equilibrium Noise EMF in the Lower-Hybrid Frequency Band</title><title>Radiophysics and quantum electronics</title><addtitle>Radiophys Quantum El</addtitle><description>We present analytical and numerical estimations of the value and frequency dependence of the impedance and noise electromotive force (EMF) in the context of the conditions which correspond to the trajectories and parameters of the antennas borne by geophysical monitoring satellites. The estimations were obtained for two circular orbits at altitudes of 600 and 1200 km over the Earth’s surface in the frequency range from 20 to 120 kHz, which corresponded to the area of the lower-hybrid resonance, where a higher level of noise emissions is observed at the altitudes under consideration. It is shown that near the lower-hybrid resonance frequency, the real part of the antenna impedance is determined by the resonant “monopole” loss by radiation of quasipotential waves. In the nonresonant frequency band (at the frequencies below the frequency of the lowerhybrid resonance), the antenna reactance is determined by the transit loss, which is, however, low as compared with the resonant loss. When the noise was calculated, the medium was assumed to be a two-temperature plasma. The spectral density of the power of the noise EMF lies in the range
and is determined mainly by suprathermal electrons. In the nonresonant frequency band, the efficient temperature of noise radiation is equal to the temperature of the “cold” plasma component, and the antenna reactance is determined by the transit loss, i.e., the level of the noise EMF is low as compared with the EMF in the resonant frequency band.</description><subject>Antennas</subject><subject>Antennas (Electronics)</subject><subject>Astronomy</subject><subject>Astrophysics and Astroparticles</subject><subject>EMF</subject><subject>Frequency bands</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Impedance</subject><subject>Lasers</subject><subject>Mathematical analysis</subject><subject>Mathematical and Computational Physics</subject><subject>Noise</subject><subject>Nuclear Physics</subject><subject>Observations and Techniques</subject><subject>Optical Devices</subject><subject>Optics</subject><subject>Orbits</subject><subject>Photonics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Optics</subject><subject>Reactance</subject><subject>Space ships</subject><subject>Space vehicles</subject><subject>Theoretical</subject><subject>Transit</subject><issn>0033-8443</issn><issn>1573-9120</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><sourceid>AFKRA</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kd1qHCEYhofSQrdpL6BnQk96YuqnzoxzuAm7TWDTH9oei-t8bgwzutEZwl5Bb7uGSaAUqgeiPo--8FbVe2DnwFj7KQOABMpA0E5CQ_mLagV1W3bA2ctqxZgQVEkpXldvcr5jrFhSrarf1-MRexMskuiIIT-OxqJNxk30IqaAZB0mDMEQH8h0i-TGHAJOMR9vMXlLvg0mj4aY0JPvs8mebu5nP_h98vNIvkSfkWxuts_yLj5golenct2TbcL7GYM9kYuiv61eOTNkfPe0nlW_tpufl1d09_Xz9eV6R62QbKKdFQLQIZgSs-1bxRtXO4V75dp9K5q6b4y0rQPYC6mcUVzVjWx5Z2rgve3EWfVxefeYYvk-T3r02eIwmIBxzhpqzjrJG6UK-uEf9C7OKZR0Gpq6DCV5XajzhTqYAbUPLk7J2DJ7HL2NAZ0v52shhShBaigCLIJNMeeETh-TH006aWD6sUu9dKlLl_qxS82LwxcnFzYcMP0V5b_SH5zAoMA</recordid><startdate>20130701</startdate><enddate>20130701</enddate><creator>Chugunov, Yu. 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L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c340t-9c331efe1aace7d7826f5f8eb8f7b7365d6a4c7f11b348fa828564729a512dc93</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><topic>Antennas</topic><topic>Antennas (Electronics)</topic><topic>Astronomy</topic><topic>Astrophysics and Astroparticles</topic><topic>EMF</topic><topic>Frequency bands</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Impedance</topic><topic>Lasers</topic><topic>Mathematical analysis</topic><topic>Mathematical and Computational Physics</topic><topic>Noise</topic><topic>Nuclear Physics</topic><topic>Observations and Techniques</topic><topic>Optical Devices</topic><topic>Optics</topic><topic>Orbits</topic><topic>Photonics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Optics</topic><topic>Reactance</topic><topic>Space ships</topic><topic>Space vehicles</topic><topic>Theoretical</topic><topic>Transit</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chugunov, Yu. 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V.</au><au>Grach, V. S.</au><au>Pasmanik, D. L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Impedance of a Spacecraft-Borne Antenna in the Magnetospheric Plasma and Quasi-Equilibrium Noise EMF in the Lower-Hybrid Frequency Band</atitle><jtitle>Radiophysics and quantum electronics</jtitle><stitle>Radiophys Quantum El</stitle><date>2013-07-01</date><risdate>2013</risdate><volume>56</volume><issue>2</issue><spage>61</spage><epage>77</epage><pages>61-77</pages><issn>0033-8443</issn><eissn>1573-9120</eissn><coden>RPQEAC</coden><abstract>We present analytical and numerical estimations of the value and frequency dependence of the impedance and noise electromotive force (EMF) in the context of the conditions which correspond to the trajectories and parameters of the antennas borne by geophysical monitoring satellites. The estimations were obtained for two circular orbits at altitudes of 600 and 1200 km over the Earth’s surface in the frequency range from 20 to 120 kHz, which corresponded to the area of the lower-hybrid resonance, where a higher level of noise emissions is observed at the altitudes under consideration. It is shown that near the lower-hybrid resonance frequency, the real part of the antenna impedance is determined by the resonant “monopole” loss by radiation of quasipotential waves. In the nonresonant frequency band (at the frequencies below the frequency of the lowerhybrid resonance), the antenna reactance is determined by the transit loss, which is, however, low as compared with the resonant loss. When the noise was calculated, the medium was assumed to be a two-temperature plasma. The spectral density of the power of the noise EMF lies in the range
and is determined mainly by suprathermal electrons. In the nonresonant frequency band, the efficient temperature of noise radiation is equal to the temperature of the “cold” plasma component, and the antenna reactance is determined by the transit loss, i.e., the level of the noise EMF is low as compared with the EMF in the resonant frequency band.</abstract><cop>Boston</cop><pub>Springer US</pub><doi>10.1007/s11141-013-9416-2</doi><tpages>17</tpages></addata></record> |
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subjects | Antennas Antennas (Electronics) Astronomy Astrophysics and Astroparticles EMF Frequency bands Hadrons Heavy Ions Impedance Lasers Mathematical analysis Mathematical and Computational Physics Noise Nuclear Physics Observations and Techniques Optical Devices Optics Orbits Photonics Physics Physics and Astronomy Quantum Optics Reactance Space ships Space vehicles Theoretical Transit |
title | Impedance of a Spacecraft-Borne Antenna in the Magnetospheric Plasma and Quasi-Equilibrium Noise EMF in the Lower-Hybrid Frequency Band |
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