2021
DOI: 10.1016/j.physd.2021.132930
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Persisting asymmetry in the probability distribution function for a random advection–diffusion equation in impermeable channels

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Cited by 6 publications
(6 citation statements)
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“…With our established evolution equation of ensemble average, we studied the passive scalar transport problem with two different types of flows, the periodic flow, and strain flow. For the periodic flow, by using the homogenization method, we show that the N-point correlation function of the random scalar flow is governed by a diffusion equation at long times, which generalized the conclusion in [10,14] from time-independent case to time-dependent case. For the strain flow, we have explicitly calculated the mean of the random scalar field and shown the statistic of this random field is related to the time integral of geometric Brownian motion.…”
Section: Conclusion and Discussionsupporting
confidence: 63%
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“…With our established evolution equation of ensemble average, we studied the passive scalar transport problem with two different types of flows, the periodic flow, and strain flow. For the periodic flow, by using the homogenization method, we show that the N-point correlation function of the random scalar flow is governed by a diffusion equation at long times, which generalized the conclusion in [10,14] from time-independent case to time-dependent case. For the strain flow, we have explicitly calculated the mean of the random scalar field and shown the statistic of this random field is related to the time integral of geometric Brownian motion.…”
Section: Conclusion and Discussionsupporting
confidence: 63%
“…The diffusion tensor would be extremely simplified. In this case, we have Λ 2N = I 2N + Pe 2 v(y, τ ) T v(y, τ ) y,τ , which reproduces the result in [10,14,7]. Then one can compute the PDF of the scalar field by using the procedure described in [14,6].…”
Section: Therefore We Havesupporting
confidence: 64%
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“…The function u(y, t) vanishes on the boundary wall and exhibits periodic time-varying behaviour with period L t . While steady pressure-driven flow is common in many applications (Price 1988;Leaist & Hao 1993;Rodrigo et al 2021), we maintain the general form and time dependence of the flow to ensure the theoretical framework's applicability to various scenarios, including blood flow (Marbach & Alim 2019) and scalar intermittency (Majda & Kramer 1999;Camassa et al 2021). We impose the no-flux boundary condition for the concentration fields of the ion species n…”
Section: Advection Nernst-planck Equationmentioning
confidence: 99%