Abstract
After reading this chapter, you will be able to add forces to lattice Boltzmann simulations while retaining their accuracy. You will know how a forcing scheme can be derived by including forces in the derivation of the lattice Boltzmann equation, though you will also know that there are a number of other forcing schemes available. You will understand how to investigate forcing models and their errors through the Chapman-Enskog analysis, and how initial and boundary conditions can be affected by the presence of forces.
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Notes
- 1.
Showing that these forcing schemes are equivalent to leading order is straightforward but involves lengthy calculations. We will not delve into details here and refer to [36] for a more qualitative analysis.
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- 5.
The sign convention for the normal momentum correction is in line with the tangential case, cf. (5.43). If \({\boldsymbol n}\) and \({\boldsymbol t}\) denote the wall normal and the wall tangential vectors and if their positive sign coincides with the positive sign of the Cartesian axis, then the normal and tangential momentum corrections appear in the algorithm as \(f_{\bar{i}}^{\mathrm{neq}}({\boldsymbol x}_{\text{B}},t) = f_{i}^{\mathrm{neq}}({\boldsymbol x}_{\text{B}},t) - ({\boldsymbol n} \cdot {\boldsymbol c}_{i})N_{n} - ({\boldsymbol t} \cdot {\boldsymbol c}_{i})N_{t}\).
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Krüger, T., Kusumaatmaja, H., Kuzmin, A., Shardt, O., Silva, G., Viggen, E.M. (2017). Forces. In: The Lattice Boltzmann Method. Graduate Texts in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-44649-3_6
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