Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors
Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of e...
Ausführliche Beschreibung
Autor*in: |
Petrov, A. S. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2012 |
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Schlagwörter: |
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Anmerkung: |
© Pleiades Publishing, Ltd. 2012 |
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Übergeordnetes Werk: |
Enthalten in: Journal of communications technology and electronics - Moscow : MAIK Nauka/Interperiodica Publ., 1996, 57(2012), 6 vom: Juni, Seite 564-571 |
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Übergeordnetes Werk: |
volume:57 ; year:2012 ; number:6 ; month:06 ; pages:564-571 |
Links: |
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DOI / URN: |
10.1134/S1064226912050075 |
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Katalog-ID: |
SPR020081391 |
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520 | |a Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. | ||
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700 | 1 | |a Kovaleva, M. V. |4 aut | |
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10.1134/S1064226912050075 doi (DE-627)SPR020081391 (SPR)S1064226912050075-e DE-627 ger DE-627 rakwb eng Petrov, A. S. verfasserin aut Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 Kovaleva, M. V. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 57(2012), 6 vom: Juni, Seite 564-571 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:57 year:2012 number:6 month:06 pages:564-571 https://dx.doi.org/10.1134/S1064226912050075 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 57 2012 6 06 564-571 |
spelling |
10.1134/S1064226912050075 doi (DE-627)SPR020081391 (SPR)S1064226912050075-e DE-627 ger DE-627 rakwb eng Petrov, A. S. verfasserin aut Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 Kovaleva, M. V. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 57(2012), 6 vom: Juni, Seite 564-571 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:57 year:2012 number:6 month:06 pages:564-571 https://dx.doi.org/10.1134/S1064226912050075 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 57 2012 6 06 564-571 |
allfields_unstemmed |
10.1134/S1064226912050075 doi (DE-627)SPR020081391 (SPR)S1064226912050075-e DE-627 ger DE-627 rakwb eng Petrov, A. S. verfasserin aut Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 Kovaleva, M. V. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 57(2012), 6 vom: Juni, Seite 564-571 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:57 year:2012 number:6 month:06 pages:564-571 https://dx.doi.org/10.1134/S1064226912050075 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 57 2012 6 06 564-571 |
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10.1134/S1064226912050075 doi (DE-627)SPR020081391 (SPR)S1064226912050075-e DE-627 ger DE-627 rakwb eng Petrov, A. S. verfasserin aut Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 Kovaleva, M. V. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 57(2012), 6 vom: Juni, Seite 564-571 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:57 year:2012 number:6 month:06 pages:564-571 https://dx.doi.org/10.1134/S1064226912050075 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 57 2012 6 06 564-571 |
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10.1134/S1064226912050075 doi (DE-627)SPR020081391 (SPR)S1064226912050075-e DE-627 ger DE-627 rakwb eng Petrov, A. S. verfasserin aut Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Pleiades Publishing, Ltd. 2012 Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 Kovaleva, M. V. aut Enthalten in Journal of communications technology and electronics Moscow : MAIK Nauka/Interperiodica Publ., 1996 57(2012), 6 vom: Juni, Seite 564-571 (DE-627)350782261 (DE-600)2083436-6 1555-6557 nnns volume:57 year:2012 number:6 month:06 pages:564-571 https://dx.doi.org/10.1134/S1064226912050075 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 57 2012 6 06 564-571 |
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Enthalten in Journal of communications technology and electronics 57(2012), 6 vom: Juni, Seite 564-571 volume:57 year:2012 number:6 month:06 pages:564-571 |
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Petrov, A. S. @@aut@@ Kovaleva, M. V. @@aut@@ |
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author |
Petrov, A. S. |
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Petrov, A. S. misc Reflection Coefficient misc Input Impedance misc Insertion Loss misc Reactive Element misc Magnetic Monopole Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors |
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Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors Reflection Coefficient (dpeaa)DE-He213 Input Impedance (dpeaa)DE-He213 Insertion Loss (dpeaa)DE-He213 Reactive Element (dpeaa)DE-He213 Magnetic Monopole (dpeaa)DE-He213 |
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misc Reflection Coefficient misc Input Impedance misc Insertion Loss misc Reactive Element misc Magnetic Monopole |
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misc Reflection Coefficient misc Input Impedance misc Insertion Loss misc Reactive Element misc Magnetic Monopole |
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misc Reflection Coefficient misc Input Impedance misc Insertion Loss misc Reactive Element misc Magnetic Monopole |
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Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors |
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Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors |
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Petrov, A. S. Kovaleva, M. V. |
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Petrov, A. S. |
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10.1134/S1064226912050075 |
title_sort |
matching of an impedance to a feeder with the help of γ sections consisting of reactive lc elements with finite q factors |
title_auth |
Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors |
abstract |
Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. © Pleiades Publishing, Ltd. 2012 |
abstractGer |
Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. © Pleiades Publishing, Ltd. 2012 |
abstract_unstemmed |
Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented. © Pleiades Publishing, Ltd. 2012 |
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Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors |
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https://dx.doi.org/10.1134/S1064226912050075 |
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S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Matching of an impedance to a feeder with the help of Γ sections consisting of reactive LC elements with finite Q factors</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Pleiades Publishing, Ltd. 2012</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Relationships for calculation of the elements of Γ sections, which consist of reactive LC elements with finite Q factors and are used for matching of the load impedance to the resistance of a generator are derived. Recommendations on the choice of a particular type of the Γ section out of eight possible design versions for an arbitrary position of the point representing the load impedance on the Smith chart are given. It is shown that, in the case of a high level of the load standing-wave ratio (more than 100), the dissipative insertion loss of a matching Γ section with imperfect elements experiences substantial oscillations, which depend on the phase of the reflection coefficient and the relationships between the Q factors of reactive LC elements. As an example, the results on matching of small electric and magnetic monopoles with lengths of (0.2–0.9)λ/4 to a circuit with a characteristic impedance of 50 Ω are presented.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Reflection Coefficient</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Input Impedance</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Insertion Loss</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Reactive Element</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Magnetic Monopole</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kovaleva, M. 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