Abstract
In this paper, the derivation of the convected derivatives for the heat flux and stress tensor is revisited. A kinematic approach is adopted based on material invariance. These upper-convected derivatives are used in the literature to generalize Newton's law of viscosity and Fourier's heat law of heat. The former constitutive law represents the behaviour of a viscoelastic fluid of the Boger type obeying the Oldroyd-B model, and the latter represents fluids obeying the Maxwell-Cattaneo's heat equation. The invariance of the derivatives under orthogonal transformation is also shown. Although the presentation here is limited to the derivatives of vector and second-rank tensor fluxes, the formulation can be generalized to generate the convected derivative of a tensor flux of arbitrary rank. Finally, the connection with micro- or nano-channel flow is noted.
| Original language | English (US) |
|---|---|
| Pages (from-to) | 991-998 |
| Number of pages | 8 |
| Journal | Discrete and Continuous Dynamical Systems - Series B |
| Volume | 15 |
| Issue number | 4 |
| DOIs | |
| State | Published - Jun 2011 |
Keywords
- Frame-indifference
- Heat flux
- Non-Newtonian fluid
- Objective rate
- Stress flux
ASJC Scopus subject areas
- Discrete Mathematics and Combinatorics
- Applied Mathematics