2001
DOI: 10.1016/s0375-9601(00)00834-3
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Symmetries of fluid dynamics with polytropic exponent

Abstract: The symmetries of the general Euler equations of fluid dynamics with polytropic exponent are determined using the Kaluza-Klein type framework of Duval et al . In the standard polytropic case the recent results of O'Raifeartaigh and Sreedhar are confirmed. Similar results are proved for polytropic exponent γ = −1, which corresponds to the dimensional reduction of d-branes. The relation between the duality transformation used in describing supernova explosion and Cosmology is explained.

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Cited by 38 publications
(23 citation statements)
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“…which generate the centre-free optical Lie algebra, i.e., the Galilei Lie algebra augmented with time dilations, found earlier as a symmetry of the Chaplygin gas with viscosity [36]. Finally, the vector fields (VII.13) preserving the Carroll space C viewed as the t = 0 slice of B, are of the form…”
Section: B Massless Systemsmentioning
confidence: 87%
“…which generate the centre-free optical Lie algebra, i.e., the Galilei Lie algebra augmented with time dilations, found earlier as a symmetry of the Chaplygin gas with viscosity [36]. Finally, the vector fields (VII.13) preserving the Carroll space C viewed as the t = 0 slice of B, are of the form…”
Section: B Massless Systemsmentioning
confidence: 87%
“…It states that the motion may be regarded as the projection of the motion of light rays moving in a fivedimensional extended spacetime and obtain for the first time Kepler For further details and applications of conformal symmetries for gravitational waves, see [15,16]. Other examples of Chrono-Projective transformations include the Schrödinger-Newton equations [17], hydrodynamics [18], Schrödinger operators [19] and projective dynamics [20]. where l the total angular momentum and n is the principal quantum number, respectively.…”
Section: Discussionmentioning
confidence: 99%
“…We list the commutation relations of this algebra 4 , and the action of its generators on the velocity fields, in detail in the next section. The conformal symmetry algebra described above is just subset of the full infinte dimensonal symmetry algebra of the Navier Stokes equations [16] (see also [17][18][19] for other related work) . The additional generators of the full symmetry algebra are very easy to describe; they consist of boosts to a reference frame whose velocity is homogeneous in space but an arbitrary function of time.…”
Section: Introduction and Discussionmentioning
confidence: 99%