Partial Differential Equations - Modelling and ... - ResearchGate
Partial Differential Equations - Modelling and ... - ResearchGate
Partial Differential Equations - Modelling and ... - ResearchGate
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62 E.J. Dean <strong>and</strong> R. Glowinski<br />
Assuming that Ω is simply connected, we introduce:<br />
u = {u 1 ,u 2 } = {∂ψ/∂x 2 , −∂ψ/∂x 1 },<br />
v = {v 1 ,v 2 } = {∂ϕ/∂x 2 , −∂ϕ/∂x 1 },<br />
ω = ∂u 2 /∂x 1 − ∂u 1 /∂x 2 ,<br />
θ = ∂v 2 /∂x 1 − ∂v 1 /∂x 2 ,<br />
V g = {v | v ∈ (H 1 (Ω)) 2 , ∇ · v =0, v · n = dg/ds on Γ },<br />
V 0 = {v | v ∈ (H 1 (Ω)) 2 , ∇ · v =0, v · n =0onΓ },<br />
( )<br />
0 1<br />
L = .<br />
−1 0<br />
Above, n is the unit vector of the outward normal at Γ <strong>and</strong> s is a counterclockwise<br />
curvilinear abscissa on Γ . The formulation (71) is equivalent to<br />
⎧<br />
∫<br />
Find u(t) ∈ V g for<br />
∫<br />
all t>0 such that<br />
∫<br />
⎪⎨<br />
∂ω/∂t θ dx + ∇u:∇v dx = Lp : ∇v dx, ∀v ∈ V 0 ,<br />
Ω<br />
Ω<br />
Ω<br />
(72)<br />
∂p/∂t + p + ∂I Qf (p)+L∇u =0,<br />
⎪⎩<br />
{u(0), p(0),ω(0)} = {u 0 , p 0 ,ω 0 }.<br />
The problem (72) has a visco-elasticity flavor, −Lp playing here the role<br />
of the so-called extra-stress tensor. Ast → +∞, we obtain thus at the limit a<br />
(kind of) viscosity solution.<br />
Acknowledgement. The authors would like to thank J. D. Benamou, Y. Brenier,<br />
L. A. Caffarelli <strong>and</strong> P.-L. Lions for assistance <strong>and</strong> helpful comments <strong>and</strong> suggestions.<br />
The support of NSF (grant DMS-0412267) is also acknowledged.<br />
References<br />
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Verlag, Berlin, 1998.<br />
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nonlinear elliptic equations. Discrete Contin. Dyn. Syst., 8(2):331–359,<br />
2002.<br />
[CC95] L. A. Caffarelli <strong>and</strong> X. Cabré. Fully Nonlinear Elliptic <strong>Equations</strong>.<br />
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