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Partial differential equations (PDEs): Existence and uniqueness, regularity, boundary conditions, linear and non-linear operators, stability, soliton theory, integrable PDEs, conservation laws, qualitative dynamics.

1 vote

Finding Free surface elevation in semi-infinite channel

What I seem to understand is that the bottom is at $y=-h+v(x-ct)$ where $v$ has compact support. That corresponds to an obstacle moving at a constant speed towards the infinite end. But it might mean …
Jean Duchon's user avatar
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2 votes

Stationary Navier-Stokes solutions

Tai-Peng Tsai's book Lectures on Navier-Stokes Equations (2018) cites as Theorem 8.3 (p.149) a theorem of V. Sverak (2011) that excludes the existence of minus one homogeneous solutions on $\mathbb R^ …
Jean Duchon's user avatar
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5 votes
1 answer
314 views

Obstruction to Navier-Stokes blowup with cylindrical symmetry

Is there a known obstruction to cylindrically symmetric solutions (with swirl) of incompressible 3D Navier-Stokes blowing up in finite time ? EDIT: in the whole space $\mathbb R^3$, I forgot to say. …
Jean Duchon's user avatar
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6 votes
1 answer
423 views

Stationary Navier-Stokes solutions

Are there known nontrivial ($u\neq0$) stationary solutions to Navier-Stokes equations in $\mathbb R^3$ ? Not square integrable of course (that's impossible), but with self-similar amplitudes of Fourie …
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0 votes

Dirichlet problem for capillary equation over convex domain

Prescribed mean curvature (of the graph of $u$) would be$$\nabla\cdot\frac{\nabla u}{\sqrt{1+|\nabla u|^2}}=c$$For an elliptic domain with $\phi$ linear in the direction of the smaller axis, the graph …
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1 vote

On solutions of the continuity equation

If $j$ has compact support in $\mathbb R_t\times\mathbb R^3_x$, $\rho$ will have compact support iff $\int_{-\infty}^\infty\nabla\cdot j_s\ ds\equiv0$. The set of approximable $L^2$ solutions should …
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2 votes

Vorticity equation for generalized Naiver Stokes equations

Taking the curl of the original equation in $\mathbb R^3$ gives$$\partial_t\omega+\nu(-\Delta)^\alpha\omega+(u\cdot\nabla)\omega-(\omega\cdot\nabla) u=\nabla\times f$$ $$\nabla\times u=\omega$$ $$\nab …
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1 vote
Accepted

Morrey condition (integral condition) and (local) Holder condition

No. Take $n=2$, $x=0$ (and $\alpha=1$, wlog). Define $f$ in polar coordinates as $f(r,\theta)=r^\beta g_r(\theta)$ where $\int_0^{2\pi} g_r(\theta)\ d\theta=1$ and $\lim_{r\to 0}g_r(0)=\infty$, which …
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2 votes

Are Pointwise conditions studied?, do they make sense?, do they have any applications?

Such interpolatory conditions are better treated by solving your PDE $Af=\sum_ic_i\delta_{p_i}$ as distributions in the whole domain, with the $c_i$s to be determined so that $f(p_i)=d_i$. For ellipti …
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5 votes

Gaussian distribution, maximum entropy and the heat equation

Besides the central limit theorem, there is the connection between diffusion and Wasserstein distance $W_2(p,q)$ (the minimum integral of squared distance from $x$ to $T(x)$ when $T$ maps $p$ to $q$) …
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8 votes
1 answer
328 views

Continuous right inverse to the Laplacian operator on $C^\infty$

For each $f\in C^\infty(\mathbb R^n)$, there exists $u\in C^\infty(\mathbb R^n)$ such that $\Delta u=f$. This, I guess, has been known well before the more general Malgrange-Ehrenpreis theorem that sa …
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2 votes

An acting condition for a superposition operator from $H^1(\Omega)$ to $H^1(\Omega)$

The obvious sufficient condition for $v\mapsto f(v)$ to map $H^1(\Omega)$ to itself ($\Omega$ bounded) is $f$ globally Lipschitz, i.e. $f'\in L^\infty(\mathbb R)$. Add $f(0)=0$ for general $\Omega$. …
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2 votes

Reformulation of the classical Navier-Stokes equation as a semilinear evolution equation and...

You are right, $(4)$ has to be understood in the special sense that the semigroup $S(t)$ (and the (Leray?) $L^2$-projection operator to $H$, as well) extend to a wider space, that of "distributional d …
Jean Duchon's user avatar
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2 votes

A $W^{1,2}_{loc}$ function with uniformly bounded integrals on compact subsets $W^{1,2}$?

Yes. There is an increasing sequence of compacts $K_n\subset\Omega$ whose union is $\Omega$, then $\int_{\Omega}(|f|^2+|\nabla f|^2)=\lim_{n\to\infty}\int_{K_n}(|f|^2+|\nabla f|^2)\le C$.
Jean Duchon's user avatar
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2 votes
1 answer
110 views

Smoluchowski-Poisson dynamics with atomic measures

"Smoluchowski-Poisson dynamics" is just a tentative provisional name I give to the following transport equation:$$\partial_t m+\nabla_x\cdot(um)=0$$where $u(x,t)\in\mathbb R^n$ ($x\in\mathbb R^n$, $t\ …
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