∂ρ∂t+∇⋅(ρu)=0 \dfrac{\partial\rho}{\partial t} + \nabla \cdot (\rho\mathbf{u}) = 0

27-29 January 2021, University of Canterbury

∂(ρu)∂t+∇⋅(ρuu)=−∇p+∇⋅τ‾+ρg \dfrac{\partial(\rho\mathbf{u})}{\partial t} + \nabla \cdot (\rho\mathbf{u}\mathbf{u}) = -\nabla p + \nabla \cdot \underline{\boldsymbol \tau} + \rho \mathbf{g}

Organising Committeeφ {}^\varphi

James N. Hewett
Department of Mechanical Engineering
University of Canterbury, New Zealand

Mathieu Sellier
Department of Mechanical Engineering
University of Canterbury, New Zealand

Phillip L. Wilson
School of Mathematics and Statistics
University of Canterbury, New Zealand

Elizabeth K. McGeorge
School of Mathematics and Statistics
University of Canterbury, New Zealand

Alan Caughley
Callaghan Innovation
Christchurch, New Zealand