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David McComb

Publications and source records attributed to David McComb.

4 recordsLinked to original sources

What is isotropic turbulence and why is it important?

This article begins with an overview, then gives the precise definition of isotropic turbulence, and follows that with the basic conservation equations, in both real space and wavenumber space. These provide the foundations of all theoretical approaches, both fundamental and phenomenological. After that, my intention is to try to highlight the main unresolved issues and give some indication of what progress there has been over decades (in all cases), and what still needs to be done. I should emphasise that I am not trying to provide either a conventional review or even a pedagogical treatment. Instead I am giving concise summaries, supplemented (where I can) by my own observations, which make substantial points that I believe are original, and which have not been made in the literature. To take just one example, it is known by some people that Kolmogorov's 1962 theory is not correctly described as a 'refinement' of his 1941 theory. This was pointed out by Kraichnan in 1974. However, what does not appear to have been recognized is that the 1962 theory is physically invalid, and also that a plausible implementation of it destroys the Kolmogorov (1941) scaling of energy spectra which has been widely observed over many years. This is discussed in Section 4 below. Lastly, I have tried to give an informal treatment in order to make everything easily accessible, to reach the widest possible audience. In particular, the section on renormalization methods is written without giving the equations of the various theories, merely stating in words what has been done, what are the different methods and also what still needs to be done.

math-ph

Taylor's dissipation surrogate and its associated anomaly

It is shown that, for stationary isotropic turbulence, Taylor's well known surrogate for the dissipation can be derived directly from the Karman-Howarth equation and is in fact a surrogate for inertial transfer, which becomes equal to the dissipation rate as the Reynolds number tends to infinity.

physics.flu-dyn

Investigation of renormalization group methods for the numerical simulation of isotropic turbulence

Renormalization group has enjoyed successes in other areas of statistical physics. However, its application to turbulence faces several technical difficulties, which have had to be circumvented by uncontrolled approximations. Indeed, in view of the deterministic nature of the Navier-Stokes equations, it is clear that the operation of averaging out the high-wavenumber modes while keeping the low-wavenumber modes constant, cannot be done rigorously and in itself can only be an approximation. With points like this in mind, we have recently adopted direct numerical simulation as a tool for probing the basic feasibility of using RG techniques to reduce the number of degrees of freedom requiring to be numerically simulated. In this paper, we present some of the first results of this approach.

physics.flu-dyn

Explict-scales projections of the partitioned non-linear term in direct numerical simulation of the Navier-Stokes equation

In this paper we consider the properties of the internal partitions of the nonlinear term, obtained when a filter with a sharp cutoff is introduced in wavenumber space. We see what appears to be some degree of independence of the choice of the position of the cutoff wavenumber for both instantaneous and time-integrated partitioned nonlinearities. We also investigate the basic idea of an eddy-viscosity model for subgrid terms and have found that while phase modelling will be very poor, amplitude modelling can be far more successful.

physics.flu-dyn