Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/4860
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dc.contributor.authorSridhar, S.-
dc.contributor.authorGoldreich, P.-
dc.date.accessioned2012-07-11T06:04:31Z-
dc.date.available2012-07-11T06:04:31Z-
dc.date.issued1994-09-
dc.identifier.citationAstrophysical Journal, 1994, vol.432, p612-621en
dc.identifier.issn0004-637X-
dc.identifier.issn1538-4357 (Online)-
dc.identifier.urihttp://hdl.handle.net/2289/4860-
dc.descriptionOpen Accessen
dc.description.abstractWe study weak Alfvenic turbulence of an incompressible, magnetized fluid in some detail, with a view to developing a firm theoretical basis for the dynamics of small-scale turbulence in the interstellar medium. We prove that resonant 3-wave interactions are absent. We also show that the Iroshnikov-Kraichnan theory of incompressible, magnetohydrodynamic turbulence -- which is widely accepted -- describes weak 3-wave turbulence; consequently, it is incorrect. Physical arguments, as well as detailed calculations of the coupling coefficients are used to demonstrate that these interactions are empty. We then examine resonant 4-wave interactions, and show that the resonance relations forbid energy transport to small spatial scales along the direction of the mean magnetic field, for both the shear Alfven wave and the pseudo Alfven wave. The three-dimensional inertial-range energy spectrum of 4-wave shear Alfven turbulence guessed from physical arguments reads E(kz, kperpendicular) approximately VAvLL-1/3kperpendicular-10/3, where VA is the Alfven speed, and vL is the velocity difference across the outer scale L. Given this spectrum, the velocity difference across lambdaperpendicular approximately kperpendicular exp -1 is vlambda (sub perpendicular) is approximately vL(lambdaperpendicular/L)2/3. We derive a kinetic equation, and prove that this energy spectrum is a stationary solution and that it implies a positive flux of energy in k-space, along directions perpendicular to the mean magnetic field. Using this energy spectrum, we deduce that 4-wave interactions strengthen as the energy cascades to small, perpendicular spatial scales; beyond an upper bound in perpendicular wavenumber, kperpendicularL is approximately (VA/vL)3/2, weak turbulence theory ceases to be valid. Energy excitation amplitudes must be very small for the 4-wave inertial-range to be substantial. When the excitation is strong, the width of the 4-wave inertial-range shrinks to zero. This seems likely to be the case in the interstellar medium.en
dc.language.isoenen
dc.publisherThe University of Chicago Press for the American Astronomical Societyen
dc.relation.urihttp://adsabs.harvard.edu/doi/10.1086/174600en
dc.relation.urihttp://dx.doi.org/10.1086/174600en
dc.rights1994 American Astronomical Societyen
dc.subjectcollisionless plasmasen
dc.subjectincompressible flowen
dc.subjectincompressible fluidsen
dc.subjectinterstellar matteren
dc.subjectmagnetohydrodynamic flowen
dc.subjectmagnetohydrodynamic turbulenceen
dc.subjectmagnetohydrodynamic wavesen
dc.subjectradio wavesen
dc.subjectvariational principlesen
dc.subject, energy spectraen
dc.titleToward a theory of interstellar turbulence. 1: weak alfvenic turbulenceen
dc.typeArticleen
Appears in Collections:Research Papers (A&A)

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