Spectral Exponents of Kinetic and Magnetic Energy Spectra in Solar Wind Turbulence
By J. Podesta, D. Roberts, M. Goldstein. 2007
203 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics, Molecular Biology
View Paper: https://www.semanticscholar.org/paper/11986685b6afc3e3ec6cf584e134b4774176eaca
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In Astronomy and Astrophysics
In Molecular Biology
- C. Chen
- B. T. MacBride
- G. T'oth
- Tamas I. Gombosi
- B. Chandran
- A. Mallet
- Charles W. Smith
- Igor M. Sokolov
Citations in the corpus
- The Turbulent Cascade at 1 AU: Energy Transfer and the Third-Order Scaling for MHD (2007, background): “See Podesta et al. (2007a) for a more complete discussion.”
- Solar Wind Turbulence and the Role of Ion Instabilities (2013, background): “Velocity fluctuations in the solar wind appear to have a spectrum significantly shallower than the magnetic field, with a spectral index near −3/2 (Grappin et al. 1991; Salem 2000; Mangeney et al. 2001; Podesta et al. 2007; Salem et al. 2009; Chen et al. 2011b, 2013b; Boldyrev et al. 2011; Borovsky ”
- DEPENDENCE OF SOLAR-WIND POWER SPECTRA ON THE DIRECTION OF THE LOCAL MEAN MAGNETIC FIELD (2009, background): “…analysis shows that solar-wind velocity fluctuations have typical spectral exponents around 3/2, magnetic field fluctuations have typical spectral exponents around 5/3, and the spectral exponents for the total energy (kinetic plus magnetic) lie somewhere between these two (Podesta et al. 2007).”
- INCORPORATING KINETIC PHYSICS INTO A TWO-FLUID SOLAR-WIND MODEL WITH TEMPERATURE ANISOTROPY AND LOW-FREQUENCY ALFVÉN-WAVE TURBULENCE (2011, background): “…AW correlation length (outer scale)L⊥, the rms amplitude of the AW velocity fluctuations at perpendicular scaleλ is ∝ λ1/4 as in observations atr = 1 AU (Podesta et al. 2007; Chen et al. 2011), direct numerical simulations of AW turbulence in the presence of a strong background magnetic field…”
- PERPENDICULAR ION HEATING BY LOW-FREQUENCY ALFVÉN-WAVE TURBULENCE IN THE SOLAR WIND (2010, background): “The valuec3 = 3/2 is motivated by a different set of theoretical and numerical studies (Boldyrev 2006; Mason et al. 2006; Perez and Boldyrev 2009), as well as recent in situ observations of the velocity power spectrum in the solar wind (Podesta et al. 2007; Podesta and Bhattacharjee 2009).”
- Anisotropy of Alfvénic turbulence in the solar wind and numerical simulations (2010, background): “…occurs only in the decaying period of our RMHD simulation, while solar wind observations show rA < 1 (e.g. Matthaeus & Goldstein 1982; Marsch & Tu 1990; Bruno et al. 2007; Podesta et al. 2007; Salem et al. 2009), suggests that solar wind turbulence may be better described by a forced model.”
- ALFVÉN WAVE SOLAR MODEL (AWSoM): CORONAL HEATING (2013, result): “The above scaling is compatible with the 1 AU observations of Podesta et al. (2007).”