Abstract
The current understanding of solidification phenomena is based largely on the differential formulation of the mechanics of the continuum and the associated conservation of mass, energy, species, and momentum equations. Thus, a short introduction to the fundamentals of transport phenomena as applied to solidification is deemed necessary to facilitate engaging in the intricacies of the subject.
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Notes
- 1.
The del operator (or the gradient) of a function u is: \(\nabla u\equiv \frac{\partial u}{\partial x}\mathbf{i}+\frac{\partial u}{\partial y}\mathbf{j}+\frac{\partial u}{\partial z}\mathbf{k}\). Note that ∇u is ∇ operating on u, while ∇ · A is the vector dot product of del with A (or the divergence): \(\nabla \cdot \mathbf{A}=\partial {{\mathbf{A}}_{x}}/\partial x+\partial {{\mathbf{A}}_{y}}/\partial y+\partial {{\mathbf{A}}_{z}}/\partial z\). Furthermore, ∇2 u is the product of the del operator with itself, or \(\nabla \cdot \nabla =\frac{\partial }{\partial x}\left(\frac{\partial }{\partial x} \right)+\frac{\partial }{\partial y}\left(\frac{\partial }{\partial y} \right)+\frac{\partial }{\partial z}\left(\frac{\partial }{\partial z} \right)\) operating on u.
- 2.
The substantial derivative of a function u is given by: \(\frac{Du}{Dt}=\frac{\partial u}{\partial t}+{{u}_{x}}\frac{\partial {{u}_{x}}}{\partial x}+{{u}_{y}}\frac{\partial u}{\partial y}+{{u}_{z}}\frac{\partial u}{\partial z}\). It can be applied to any property of a fluid, the magnitude of which varies with time and position.
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Stefanescu, D. (2015). Fundamentals of Transport Phenomena as Applied to Solidification Processing. In: Science and Engineering of Casting Solidification. Springer, Cham. https://doi.org/10.1007/978-3-319-15693-4_4
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DOI: https://doi.org/10.1007/978-3-319-15693-4_4
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