2021
DOI: 10.1017/jfm.2020.957
|View full text |Cite
|
Sign up to set email alerts
|

The diffusing-velocity random walk: a spatial-Markov formulation of heterogeneous advection and diffusion

Abstract: Abstract

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
35
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
7

Relationship

5
2

Authors

Journals

citations
Cited by 12 publications
(36 citation statements)
references
References 51 publications
1
35
0
Order By: Relevance
“…Future work will also aim to generalize the approach to higher-order reactions involving multiple transported components, multiple simultaneous reactions, and heterogeneity (spatial and temporal variability) in the solid-phase reactant distribution along the interface. The PTRW method used here is based on that employed in [85] to simulate conservative transport in a number of stratified flows, where it was validated against theoretical predictions for dispersion, concentration distributions, breakthrough curves (first passage times across a plane), and Lagrangian velocity distributions. The conservative transport algorithm consists in discretizing the Langevin equation ( 1) for a set of Lagrangian particles, or trajectories, with prescribed initial conditions.…”
Section: Discussionmentioning
confidence: 99%
“…Future work will also aim to generalize the approach to higher-order reactions involving multiple transported components, multiple simultaneous reactions, and heterogeneity (spatial and temporal variability) in the solid-phase reactant distribution along the interface. The PTRW method used here is based on that employed in [85] to simulate conservative transport in a number of stratified flows, where it was validated against theoretical predictions for dispersion, concentration distributions, breakthrough curves (first passage times across a plane), and Lagrangian velocity distributions. The conservative transport algorithm consists in discretizing the Langevin equation ( 1) for a set of Lagrangian particles, or trajectories, with prescribed initial conditions.…”
Section: Discussionmentioning
confidence: 99%
“…We thus approximate the flow rate decay along the depth as qd(zfalse|)q0ez/amH(z), ${q}_{\mathrm{d}}(z\vert \ell )\approx {q}_{\mathrm{0}}{e}^{-z/{a}_{\mathrm{m}}}H(\ell -z),$ where q 0 = q d (0| ℓ ) is the flow rate at the contact with the backbone and H is the Heaviside step function. Since this flow rate profile is monotonically decreasing, the associated PDF for a given q 0 and ℓ can be computed as (Aquino & Le Borgne, 2021) pQd(qfalse|,q0)=|dqnormaldfalse(z|false)dzz=znormalqfalse(qfalse)1, ${p}_{\mathrm{Q}}^{d}(q\vert \ell ,{q}_{\mathrm{0}})={\left(\ell {\left.\frac{d{q}_{\mathrm{d}}(z\vert \ell )}{dz}\right\vert }_{z={z}_{\mathrm{q}}(q)}\right)}^{-1},$ where z q ( q ) is the point at which the flow has a given value q , that is, q d [ z q ( q )| ℓ ] = q . Thus, inverting Equation for depth as a function of flow rate, computing dq d ( z | ℓ )/ dz , and substituting, Equation becomes pQd(qfalse|,q0)=anormalmqH(q0q)H(qq0e/am), ${p}_{\mathrm{Q}}^{d}(q\vert \ell ,{q}_{\mathrm{0}})=\frac{{a}_{\mathrm{m}}}{\ell q}H({q}_{0}-q)H(q-{q}_{0}{e}^{-\ell /{a}_{\mathrm{m}}}),$ for the dead‐end flow rate PDF pQd(false|…”
Section: Prediction Of Unsaturated Flow Distributionmentioning
confidence: 99%
“…6b). The flux-weighted velocity PDF of the composite domain was used to compute the velocity correlations because it provides a reliable analog for the Lagrangian velocities (trajectories) (Dentz et al, 2016;Aquino & Le Borgne, 2021). S-Lagrangian velocity correlation (Le Borgne et al, 2008) was computed throughout the composite domain, evaluated at a distance of one model cell-size (i.e.…”
Section: Numerical Examplementioning
confidence: 99%