Implicit Large Eddy Simulation: Computing Turbulent Fluid Dynamics

Section C: Verification and Validation

Chapter List

Chapter 7: Simulating Compressible Turbulent Flow with PPM
Chapter 8: Vortex Dynamics and Transition to Turbulence in Free Shear Flows
Chapter 9: Symmetry Bifurcation and Instabilities
Chapter 10: Incompressible Wall-Bounded Flows
Chapter 11: Compressible Turbulent Shear Flows
Chapter 12: Turbulent Flow Simulations Using Vorticity Confinement
Chapter 13: Rayleigh Taylor and Richtmyer Meshkov Mixing

David H. Porter and Paul R. Woodward

7.1 Introduction

The use of the piecewise parabolic method (PPM) gas dynamics simulation scheme is described in detail in Chapter 4b and used in Chapter 15 (see also Woodward and Colella 1981, 1984; Collela and Woodward 1984; Woodward 1986, 2005). Here we review applications of PPM to turbulent flow problems. In particular, we focus our attention on simulations of homogeneous, compressible, periodic, decaying turbulence. The motivation for this focus is that if the phenomenon of turbulence is indeed universal, we should find within this single problem a complete variety of particular circumstances. If we choose to ignore any potential dependence on the gas equation of state, choosing to adopt the gamma law with ? = 1.4 that applies to air, we are then left with a one-parameter family of turbulent flows. This single parameter is the root-mean-square (rms) Mach number of the flow. We note that a decaying turbulent flow that begins at, say, Mach 1 will, as it decays, pass through all Mach numbers between that value and zero. Of course, we will have arbitrary possible entropy variations to deal with, but turbulence itself will tend to mix...

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