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Sean McKee

Publications and source records attributed to Sean McKee.

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The importance of random galilean transformation invariance in modelling dispersed particle flows

The principle of Random Galilean Transformation (RGT) Invariance is applied to the random motion of particles in a turbulent gas to construct a kinetic equation for the transport of the particle phase space probability where \mathbf{v} and \mathbf{x} are the velocity and position of a particle at time t. The essential problem is to find closed expressions for the phase space dispersion current \left\langle \boldsymbol{f}W\right\rangle , where \boldsymbol{f} is the fluctuating aerodynamic force at \mathbf{v} and \mathbf{x} at time t. The simplest form consistent with RGT invariance, the correct equation of state ancl form for the inter-phase momentum transfer tern is shown to be \left\langle \boldsymbol{f}W\right\rangle =-\left(\boldsymbolμ\cdot\frac{\partial}{\partial\mathbf{v}}+\boldsymbolλ\cdot\frac{\partial}{\partial\mathbf{x}}\right)\left\langle W\right\rangle in which \text{\textbf{\ensuremath{\boldsymbol{\,μ}}}\ensuremath{=<\boldsymbol{f}(t)\mathbf{v}(t)>}} and \boldsymbolλ=<\boldsymbol{f}(t)\boldsymbol{\mathbf{x}}(t)>.This approach to modeling gas-solid flows is currently being used to investigate the behavior of radioactive aerosols inside gas-cooled nuclear reactors.

physics.flu-dyn

Asymptotic analysis of drug dissolution in two layers having widely differing diffusion coefficients

This paper is concerned with a diffusion-controlled moving-boundary problem in drug dissolution, in which the moving front passes from one medium to another for which the diffusion coefficient is many orders of magnitude smaller. It has been shown in an earlier paper that a similarity solution exists while the front is passing through the first layer, but that this breaks down in the second layer. Asymptotic methods are used to understand what is happening in the second layer. Although this necessitates numerical computation, one interesting outcome is that only one calculation is required, no matter what the diffusion coefficient is for the second layer.

physics.flu-dyn