Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction
Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It i...
Ausführliche Beschreibung
Autor*in: |
Shah, S. K. D. [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
1969 |
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Schlagwörter: |
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Anmerkung: |
© Società Italiana di Fisica 1969 |
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Übergeordnetes Werk: |
Enthalten in: Il nuovo cimento - [S.l.] : Italian Physical Soc., 1965, 63(1969), 1 vom: Sept., Seite 105-114 |
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Übergeordnetes Werk: |
volume:63 ; year:1969 ; number:1 ; month:09 ; pages:105-114 |
Links: |
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DOI / URN: |
10.1007/BF02711047 |
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Katalog-ID: |
SPR020656815 |
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100 | 1 | |a Shah, S. K. D. |e verfasserin |4 aut | |
245 | 1 | 0 | |a Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
264 | 1 | |c 1969 | |
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500 | |a © Società Italiana di Fisica 1969 | ||
520 | |a Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. | ||
650 | 4 | |a Magnetic Field |7 (dpeaa)DE-He213 | |
650 | 4 | |a Dispersive Medium |7 (dpeaa)DE-He213 | |
650 | 4 | |a Magnetic Pressure |7 (dpeaa)DE-He213 | |
650 | 4 | |a Compressible Fluid |7 (dpeaa)DE-He213 | |
650 | 4 | |a Inhomogeneous Magnetic Field |7 (dpeaa)DE-He213 | |
700 | 1 | |a Srivastava, K. M. |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Il nuovo cimento |d [S.l.] : Italian Physical Soc., 1965 |g 63(1969), 1 vom: Sept., Seite 105-114 |w (DE-627)627248705 |w (DE-600)2556218-6 |x 1826-9877 |7 nnns |
773 | 1 | 8 | |g volume:63 |g year:1969 |g number:1 |g month:09 |g pages:105-114 |
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952 | |d 63 |j 1969 |e 1 |c 09 |h 105-114 |
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1969 |
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1969 |
allfields |
10.1007/BF02711047 doi (DE-627)SPR020656815 (SPR)BF02711047-e DE-627 ger DE-627 rakwb eng Shah, S. K. D. verfasserin aut Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 Srivastava, K. M. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 63(1969), 1 vom: Sept., Seite 105-114 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:63 year:1969 number:1 month:09 pages:105-114 https://dx.doi.org/10.1007/BF02711047 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 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_4277 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 63 1969 1 09 105-114 |
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10.1007/BF02711047 doi (DE-627)SPR020656815 (SPR)BF02711047-e DE-627 ger DE-627 rakwb eng Shah, S. K. D. verfasserin aut Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 Srivastava, K. M. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 63(1969), 1 vom: Sept., Seite 105-114 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:63 year:1969 number:1 month:09 pages:105-114 https://dx.doi.org/10.1007/BF02711047 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 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_4277 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 63 1969 1 09 105-114 |
allfields_unstemmed |
10.1007/BF02711047 doi (DE-627)SPR020656815 (SPR)BF02711047-e DE-627 ger DE-627 rakwb eng Shah, S. K. D. verfasserin aut Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 Srivastava, K. M. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 63(1969), 1 vom: Sept., Seite 105-114 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:63 year:1969 number:1 month:09 pages:105-114 https://dx.doi.org/10.1007/BF02711047 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 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_4277 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 63 1969 1 09 105-114 |
allfieldsGer |
10.1007/BF02711047 doi (DE-627)SPR020656815 (SPR)BF02711047-e DE-627 ger DE-627 rakwb eng Shah, S. K. D. verfasserin aut Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 Srivastava, K. M. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 63(1969), 1 vom: Sept., Seite 105-114 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:63 year:1969 number:1 month:09 pages:105-114 https://dx.doi.org/10.1007/BF02711047 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 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_4277 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 63 1969 1 09 105-114 |
allfieldsSound |
10.1007/BF02711047 doi (DE-627)SPR020656815 (SPR)BF02711047-e DE-627 ger DE-627 rakwb eng Shah, S. K. D. verfasserin aut Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction 1969 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Società Italiana di Fisica 1969 Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 Srivastava, K. M. aut Enthalten in Il nuovo cimento [S.l.] : Italian Physical Soc., 1965 63(1969), 1 vom: Sept., Seite 105-114 (DE-627)627248705 (DE-600)2556218-6 1826-9877 nnns volume:63 year:1969 number:1 month:09 pages:105-114 https://dx.doi.org/10.1007/BF02711047 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_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_121 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_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_374 GBV_ILN_602 GBV_ILN_647 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_2018 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_2043 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 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_2158 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2193 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_2808 GBV_ILN_4012 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_4277 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_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4346 GBV_ILN_4367 GBV_ILN_4393 GBV_ILN_4700 GBV_ILN_4753 AR 63 1969 1 09 105-114 |
language |
English |
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Enthalten in Il nuovo cimento 63(1969), 1 vom: Sept., Seite 105-114 volume:63 year:1969 number:1 month:09 pages:105-114 |
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Enthalten in Il nuovo cimento 63(1969), 1 vom: Sept., Seite 105-114 volume:63 year:1969 number:1 month:09 pages:105-114 |
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Magnetic Field Dispersive Medium Magnetic Pressure Compressible Fluid Inhomogeneous Magnetic Field |
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Il nuovo cimento |
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Shah, S. K. D. @@aut@@ Srivastava, K. M. @@aut@@ |
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1969-09-01T00:00:00Z |
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D.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1969</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">© Società Italiana di Fisica 1969</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. 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|
author |
Shah, S. K. D. |
spellingShingle |
Shah, S. K. D. misc Magnetic Field misc Dispersive Medium misc Magnetic Pressure misc Compressible Fluid misc Inhomogeneous Magnetic Field Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
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1826-9877 |
topic_title |
Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction Magnetic Field (dpeaa)DE-He213 Dispersive Medium (dpeaa)DE-He213 Magnetic Pressure (dpeaa)DE-He213 Compressible Fluid (dpeaa)DE-He213 Inhomogeneous Magnetic Field (dpeaa)DE-He213 |
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misc Magnetic Field misc Dispersive Medium misc Magnetic Pressure misc Compressible Fluid misc Inhomogeneous Magnetic Field |
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misc Magnetic Field misc Dispersive Medium misc Magnetic Pressure misc Compressible Fluid misc Inhomogeneous Magnetic Field |
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misc Magnetic Field misc Dispersive Medium misc Magnetic Pressure misc Compressible Fluid misc Inhomogeneous Magnetic Field |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
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title_full |
Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
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Shah, S. K. D. |
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Shah, S. K. D. Srivastava, K. M. |
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Elektronische Aufsätze |
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Shah, S. K. D. |
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10.1007/BF02711047 |
title_sort |
hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
title_auth |
Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
abstract |
Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. © Società Italiana di Fisica 1969 |
abstractGer |
Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. © Società Italiana di Fisica 1969 |
abstract_unstemmed |
Summary Propagation of hydromagnetic waves in an inviscid, infinitely conducting, compressible fluid, at rest in the equilibrium state, is studied in a linear approximation. The fluid is immersed in an inhomogeneous magnetic field of constant direction, normal to the direction of its variation. It is shown that two types of waves i) Alfvén waves, with the local Alfvén velocityVA=H(x)/(4πϱ0)1/2 and ii) hydromagnetic waves with exponentially decaying amplitude propagate along the lines of force. In particular, it is shown that if the magnetic pressureP=αx+const, linearization of the equations is valid for all values ofx and that waves of all frequencies and wave numbers, exceptω/k=√2/3·Cs, propagate throughout the medium. Also ifP=const+βexp[−αx], waves for all values ofω andk propagate throughout the medium. It is also found that the medium does not behave as a dispersive medium. © Società Italiana di Fisica 1969 |
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title_short |
Hydromagnetic waves in an infinitely conducting compressible fluid with an inhomogeneous magnetic field of constant direction |
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https://dx.doi.org/10.1007/BF02711047 |
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Srivastava, K. M. |
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Srivastava, K. M. |
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10.1007/BF02711047 |
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2024-07-03T17:26:03.559Z |
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score |
7.397339 |