Abstract:In this paper we provide converge rates for the homogenization of the Poisson problem with Dirichlet boundary conditions in a randomly perforated domain of R d , d 3. We assume that the holes that perforate the domain are spherical and are generated by a rescaled marked point process (Φ, R). The point process Φ generating the centres of the holes is either a Poisson point process or the lattice Z d ; the marks R generating the radii are unbounded i.i.d random variables having finite (d − 2 + β)-moment, for β >… Show more
“…We divide the proof into steps. The strategy of this proof is similar to the one for [11][Theorem 2.1, (b)].…”
Section: 13)mentioning
confidence: 99%
“…In the remaining part of the proof we tackle inequalities (3.25). We follow the same lines of [11][Theorem 1.1, (b)]. and thus only sketch the main steps for the argument.…”
Section: 13)mentioning
confidence: 99%
“…The explicit formulation of the harmonic functions {w ε,z } z∈n ε (D) defined in (3.16) (c.f. also [11][(2.24)]) implies that for every z ∈ n ε (D)…”
Section: 13)mentioning
confidence: 99%
“…It thus remains to pass from (3.27) to (3.26): We do this by taking the expectation and arguing as for [11][Inequality (4.22)]. We rely on the stationarity of (φ, R), the properties of the Poisson point process and the fact that z ∈ n ε implies that ε α ρ z ε 1+γ and R ε,z ε 1+ 1 2 γ .…”
Section: 13)mentioning
confidence: 99%
“…These allow to pass to the limit in the equation and identify the effective problem. We stress that a crucial ingredient in these arguments is given by the quantitative bounds obtained in [11] in the case α = 3. These bounds may indeed also be extended to the current setting sot that the rate of convergence of the measures −σ −2 ε ∆w ε ∈ H −1 (D) is quantified.…”
We consider the homogenization of a Poisson problem or a Stokes system in a randomly punctured domain with Dirichlet boundary conditions. We assume that the holes are spherical and have random centres and radii. We impose that the average distance between the balls is of size ε and their average radius is ε α , α ∈ (1; 3). We prove that, as in the periodic case [2], the solutions converge to the solution of Darcy's law (or its scalar analogue in the case of Poisson). In the same spirit of [12,14], we work under minimal conditions on the integrability of the random radii. These ensure that the problem is well-defined but do not rule out the onset of clusters of holes.
“…We divide the proof into steps. The strategy of this proof is similar to the one for [11][Theorem 2.1, (b)].…”
Section: 13)mentioning
confidence: 99%
“…In the remaining part of the proof we tackle inequalities (3.25). We follow the same lines of [11][Theorem 1.1, (b)]. and thus only sketch the main steps for the argument.…”
Section: 13)mentioning
confidence: 99%
“…The explicit formulation of the harmonic functions {w ε,z } z∈n ε (D) defined in (3.16) (c.f. also [11][(2.24)]) implies that for every z ∈ n ε (D)…”
Section: 13)mentioning
confidence: 99%
“…It thus remains to pass from (3.27) to (3.26): We do this by taking the expectation and arguing as for [11][Inequality (4.22)]. We rely on the stationarity of (φ, R), the properties of the Poisson point process and the fact that z ∈ n ε implies that ε α ρ z ε 1+γ and R ε,z ε 1+ 1 2 γ .…”
Section: 13)mentioning
confidence: 99%
“…These allow to pass to the limit in the equation and identify the effective problem. We stress that a crucial ingredient in these arguments is given by the quantitative bounds obtained in [11] in the case α = 3. These bounds may indeed also be extended to the current setting sot that the rate of convergence of the measures −σ −2 ε ∆w ε ∈ H −1 (D) is quantified.…”
We consider the homogenization of a Poisson problem or a Stokes system in a randomly punctured domain with Dirichlet boundary conditions. We assume that the holes are spherical and have random centres and radii. We impose that the average distance between the balls is of size ε and their average radius is ε α , α ∈ (1; 3). We prove that, as in the periodic case [2], the solutions converge to the solution of Darcy's law (or its scalar analogue in the case of Poisson). In the same spirit of [12,14], we work under minimal conditions on the integrability of the random radii. These ensure that the problem is well-defined but do not rule out the onset of clusters of holes.
We study the homogenization of the Dirichlet problem for the Stokes equations in $$\mathbb {R}^3$$
R
3
perforated by m spherical particles. We assume the positions and velocities of the particles to be identically and independently distributed random variables. In the critical regime, when the radii of the particles are of order $$m^{-1}$$
m
-
1
, the homogenization limit u is given as the solution to the Brinkman equations. We provide optimal rates for the convergence $$u_m \rightarrow u$$
u
m
→
u
in $$L^2$$
L
2
, namely $$m^{-\beta }$$
m
-
β
for all $$\beta < 1/2$$
β
<
1
/
2
. Moreover, we consider the fluctuations. In the central limit scaling, we show that these converge to a Gaussian field, locally in $$L^2(\mathbb {R}^3)$$
L
2
(
R
3
)
, with an explicit covariance. Our analysis is based on explicit approximations for the solutions $$u_m$$
u
m
in terms of u as well as the particle positions and their velocities. These are shown to be accurate in $$\dot{H}^1(\mathbb {R}^3)$$
H
˙
1
(
R
3
)
to order $$m^{-\beta }$$
m
-
β
for all $$\beta < 1$$
β
<
1
. Our results also apply to the analogous problem regarding the homogenization of the Poisson equations.
We consider the homogenization of a Poisson problem or a Stokes system in a randomly punctured domain with Dirichlet boundary conditions. We assume that the holes are spherical and have random centres and radii. We impose that the average distance between the balls is of size $$\varepsilon $$
ε
and their average radius is $$\varepsilon ^{\alpha }$$
ε
α
, $$\alpha \in (1; 3)$$
α
∈
(
1
;
3
)
. We prove that, as in the periodic case (Allaire, G., Arch. Rational Mech. Anal. 113(113):261–298, 1991), the solutions converge to the solution of Darcy’s law (or its scalar analogue in the case of Poisson). In the same spirit of (Giunti, A., Höfer, R., Ann. Inst. H. Poincare’- An. Nonl. 36(7):1829–1868, 2019; Giunti, A., Höfer, R., Velàzquez, J.J.L., Comm. PDEs 43(9):1377–1412, 2018), we work under minimal conditions on the integrability of the random radii. These ensure that the problem is well-defined but do not rule out the onset of clusters of holes.
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