2004
DOI: 10.1007/s00161-003-0146-0
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Nonlinear wave propagation in binary mixtures of Euler fluids

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Cited by 9 publications
(4 citation statements)
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“…is the adiabatic speed of sound. Moreover, it follows straightforward that the eigenvectors of the Jacobian matrix A(U) constitute a complete set and therefore the system of balance equations (1-4) is hyperbolic, as expected when the hydrodynamic equations are closed at the Euler level (see [22]). In this case, the single-temperature model for such Euler fluid can be regarded as a principal subsystem of a multi-temperature model in the sense of extended thermodynamics (see [23,24]).…”
Section: Reactive Euler Equations and Their Hyperbolicitymentioning
confidence: 68%
“…is the adiabatic speed of sound. Moreover, it follows straightforward that the eigenvectors of the Jacobian matrix A(U) constitute a complete set and therefore the system of balance equations (1-4) is hyperbolic, as expected when the hydrodynamic equations are closed at the Euler level (see [22]). In this case, the single-temperature model for such Euler fluid can be regarded as a principal subsystem of a multi-temperature model in the sense of extended thermodynamics (see [23,24]).…”
Section: Reactive Euler Equations and Their Hyperbolicitymentioning
confidence: 68%
“…Instead, in the case of a ST system, the evaluation of the velocities is very difficult also in an equilibrium state due to the fact that the characteristic polynomial is, in general, irreducible (see e.g. [3,23]), but thanks to the subcharacteristic property (41) of principal subsystems, we are able now to establish the following lower and upper bound for the characteristic velocities of the ST model: (7) is a particular case of a system of balance laws (8) and it is dissipative due to the presence of the productions that satisfy the entropy principle. Moreover, we have verified that h 0 is a convex function of the densities u ≡ F 0 .…”
Section: Characteristic Velocities and Their Upper Bound In The St Modelmentioning
confidence: 99%
“…T 1 = T 2 = T and = 0, one obtains T (c) ≡ T from (51) 2 , while (51) 3 is reduced to the average ratio of specific heats introduced in [23]. Hence, the mixture now appears as a single fluid but besides the usual fields ( , v, T ), we have also the extended new ones (c, J, ).…”
mentioning
confidence: 92%
“…Instead, in the case of a ST system the evaluation of the velocities is very difficult also in an equilibrium state due to the fact that the characteristic polynomial is, in general, irreducible (see e.g. [2], [15]) but thanks to the subcharacteristic property (18) of principal subsystems we are able now to establish the following lower and upper bound for the characteristic velocities of the ST model:…”
Section: Characteristic Velocities and Their Upper Bound In The St Modelmentioning
confidence: 99%