2016
DOI: 10.1103/physreve.94.061102
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Coupled continuous-time random walks for fluid stretching in two-dimensional heterogeneous media

Abstract: We study the relation between flow structure and fluid deformation in steady flows through two-dimensional heterogeneous media, which are characterized by a broad spectrum of stretching behaviors, ranging from sub- to superlinear. We analyze these behaviors from first principles, which uncovers intermittent shear events to be at the origin of subexponential stretching. We derive explicit expressions for Lagrangian deformation and demonstrate that stretching obeys a coupled continuous-time random walk, which fo… Show more

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Cited by 26 publications
(52 citation statements)
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References 56 publications
(94 reference statements)
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“…In the wait first model [19,37,38], where the particle is localized in space, and then makes an instantaneous displacement, big jumps can be generated only by the second process since the particle is at rest at the moment of observation T , and the tail of P (R, T ) is given by B 1 only. Another possible extension where the big jump principle can be applied is the model where the motion of the particle is not ballistic [39] . An important example of accelerated motion will be discussed in detail in Section III.…”
Section: Lévy Walks: the Jump Rate And The Big Jumpmentioning
confidence: 99%
“…In the wait first model [19,37,38], where the particle is localized in space, and then makes an instantaneous displacement, big jumps can be generated only by the second process since the particle is at rest at the moment of observation T , and the tail of P (R, T ) is given by B 1 only. Another possible extension where the big jump principle can be applied is the model where the motion of the particle is not ballistic [39] . An important example of accelerated motion will be discussed in detail in Section III.…”
Section: Lévy Walks: the Jump Rate And The Big Jumpmentioning
confidence: 99%
“…In order to investigate the impact of strong heterogeneity of velocity point values, we consider a velocity distribution that is characterized by power-law behavior at low velocities [77,72]…”
Section: Heterogeneitymentioning
confidence: 99%
“…As shall be shown, we observe three main types of transport structures (open, closed, and chaotic) in periodically forced aquifers over the flow parameter space Q ¼ T×G×C. In this section we briefly review these visualization tools, classify and describe these transport structures, and show how they change with T, G, and C. In the absence of sources and sinks, steady Darcy flow is typified by open streamlines and an absence of stagnation points (Bear, 1972), leading to slow mixing and limited transport dynamics (Dentz et al, 2016;Sposito, 2001). Conversely, unsteady Darcy flows can break these topological constraints due to transient switching of streamlines (Lester et al, 2009Metcalfe, Lester, Ord, Kulkarni, Rudman, et al, 2010;Neupauer et al, 2014;Trefry et al, 2012), leading to a much richer set of possible transport structures.…”
Section: Transport Structures Of Periodically Forced Aquifersmentioning
confidence: 99%