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Additional Reminders: Compressible Turbulence Description

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Homogeneous Turbulence Dynamics
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Abstract

This chapter presents the specific features of the description of compressible turbulent flows: governing equations, Favre-averaging and Kovasznay decomposition of compressible disturbances as the sum of vortical, acoustic and entropy modes, along with Rankine–Hugoniot jump relations. Linearized jump relations are also discussed.

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Notes

  1. 1.

    Extensions to mixtures of perfect gas and reactive shock waves with chemical reactions will be discussed in devoted sections in Chaps. 15 and 16.

  2. 2.

    The discussion in the present chapter is restricted to the case of single-phase, non-reactive, single-species flows of divariant fluids. The case of binary mixtures of perfect gas is addressed in Sect. 16.9.2.

  3. 3.

    It is recalled that the first non-dimensional parameter \(\epsilon \) is related to the amplitude of the perturbations.

  4. 4.

    Considering \(\nu _0 = 0.15\cdot 10^{-4}\,\mathrm{m^2 s}^{-1}\) and \(a_0 = 300\,\mathrm{m s}^{-1}\), one obtains \(\nu _0/a_0 = 5 \cdot 10^{-8}\,\mathrm{m}\) which is of the order of the mean-free path of the molecules in the gas. For a frequency equal to 1 Hz, one has \(1/k = 300\,\mathrm{m}\) and \(\epsilon ' =1.66 \cdot 10^{-10}\). For 1 kHz one has \(\epsilon ' =1.66 \cdot 10^{-7}\) and \(\epsilon ' =1.66 \cdot 10^{-4}\) at 1 MHz. Even at 1 GHz, one obtains \(\epsilon '=1.66 \cdot 10^{-1} < 1\) !

  5. 5.

    But let us notice that the density-weighted average was introduced by Osborne Reynolds in is seminal paper in 1884!

  6. 6.

    This term was coined by Chassaing and coworkers (see Chassaing et al. 2002), who developed the alternative ternary regrouping approach.

  7. 7.

    This assumption is relevant for most high-speed non-reactive flows.

  8. 8.

    In non-homogeneous flows a third contribution must be taken into account, which is defined as

    $$ {\bar{\varepsilon }}_n = 2 \frac{{\bar{\mu }}}{{\bar{\rho }}} \left( \frac{\partial ^2 }{\partial x_i \partial x_j} \overline{u'_iu'_j} - 2 \frac{\partial }{\partial x_j} \left( \overline{ {u}^{\prime }_j \frac{\partial {u}^{\prime }_i}{\partial x_i} } \right) \right) . $$

References

  • Bayly, B.J., Levermore, C.D., Passot, T.: Density variations in weakly compressible flows. Phys. Fluids 4(5), 945–954 (1992)

    Article  ADS  MathSciNet  MATH  Google Scholar 

  • Chassaing, P., Antonia, R.A., Anselmet, F., Joly, L., Sarkar, S.: Variable density turbulence. Springer, Berlin (2002)

    Book  MATH  Google Scholar 

  • Chomaz, J.M.: Global instabilities in spatially developing flows: Non-normality and non-linearity. Ann. Rev. Fluid Mech. 37, 357–392 (2005)

    Article  ADS  MATH  Google Scholar 

  • Chu, B.T.: On the energy transfer to small disturbances in fluid flow (part 1). Acta Mechanica 1, 215–234 (1965)

    Article  Google Scholar 

  • Chu, B.T., Kovasznay, L.S.G.: Non-linear interactions in a viscous heat-conducting compressible gas. J. Fluid Mech. 3, 494–514 (1957)

    Article  ADS  MathSciNet  Google Scholar 

  • Feiereisen, W.J., Reynolds, W.C., Ferziger, J.H.: Numerical simulation of compressible homogeneous turbulent shear flow, Report No TF 13, Stanford University (1981)

    Google Scholar 

  • Hayes, W.D.: The vorticity jump across a gasdynamic discontinuity. J. Fluid Mech. 2, 595–600 (1957)

    Article  ADS  MATH  Google Scholar 

  • Joseph George, K., Sujith, R.I.: On Chu’s disturbance energy. J. Sound Vib. 330, 5280–5291 (2011)

    Article  ADS  Google Scholar 

  • Kovasznay, L.S.G.: Turbulence in supersonic flow. J. Aero. Sci. 20, 657–682 (1953)

    Article  MATH  Google Scholar 

  • Zank, G.P., Matthaeus, W.H.: Nearly incompressible hydrodynamics and heat conduction. Phys. Rev. Lett. 64(11), 1243–1245 (1990)

    Article  ADS  Google Scholar 

  • Zank, G.P., Matthaeus, W.H.: The equations of nearly incompressible fluids. I. Hydrodynamics, turbulence and waves. Phys. Fluids 3(1), 69–82 (1991)

    Article  ADS  MathSciNet  MATH  Google Scholar 

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Correspondence to Pierre Sagaut .

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Sagaut, P., Cambon, C. (2018). Additional Reminders: Compressible Turbulence Description. In: Homogeneous Turbulence Dynamics. Springer, Cham. https://doi.org/10.1007/978-3-319-73162-9_3

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