The importance of random galilean transformation invariance in modelling dispersed particle flows
Authors
Michael W Reeks, Sean McKee
Categories
Abstract
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 <W(\mathbf{v},\mathbf{x},t)> 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.
The importance of random galilean transformation invariance in modelling dispersed particle flows
Categories
Abstract
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 <W(\mathbf{v},\mathbf{x},t)> 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.
Authors
Michael W Reeks, Sean McKee
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