A particle-in-Burgers model: theory and numerics - Laboratoire de ...
A particle-in-Burgers model: theory and numerics - Laboratoire de ...
A particle-in-Burgers model: theory and numerics - Laboratoire de ...
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Mo<strong>de</strong>l <strong>and</strong> motivation Auxiliary steps Results h = 0: coupl<strong>in</strong>g h = 0: <strong>de</strong>f<strong>in</strong>ition, uniqueness h = 0: <strong>numerics</strong>, existence The coupled problem<br />
Case h = h(t): existence, uniqueness<br />
Theorem (well-posedness for mov<strong>in</strong>g but <strong>de</strong>coupled <strong>particle</strong>)<br />
Given h(·) a C 1 path, there exists a unique entropy solution to the <strong>Burgers</strong><br />
equation with s<strong>in</strong>gular drag term −λ(u − h ′ (t))δ0(x − h(t)); (localized) L 1<br />
contraction property holds.<br />
Def<strong>in</strong>ition :<br />
– the germ Gλ changes <strong>in</strong>to (h ′ (t), h ′ (t))+Gλ;<br />
– versions B. (“with traces”) <strong>and</strong> D. (“adapted entropy <strong>in</strong>equalities with<br />
rema<strong>in</strong><strong>de</strong>r term”) permit to <strong>de</strong>f<strong>in</strong>e entropy solutions.<br />
Arguments :<br />
– for uniqueness, comparison, L 1 contraction: same technique;<br />
– for existence: use characterization D. (it is stable by passage to the limit!) ;<br />
– approximate h(·) by a family (hn)n of piecewise aff<strong>in</strong>e paths<br />
– construction of solutions for “<strong>particle</strong> at hn” is straightforward: h ′ n be<strong>in</strong>g<br />
piecewise constant, one changes variables to reduce to the “drag<br />
force-at-zero” case. Procedure restarted at each time where h ′ n jumps.<br />
– because h ′ n → h ′ , the associated germs converge; thus we pass to the limit<br />
<strong>in</strong> characterization D..