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P. I. Plotnikov

Publications and source records attributed to P. I. Plotnikov.

3 recordsLinked to original sources

A Proof of Hélein's Conjecture on Boundedness of Conformal Factors when n=3

For smooth mappings of the unit disc into the oriented Grassmannian manifold $\mathbb G_{n,2}$, Hélein (2002) conjectured the global existence of Coulomb frames with bounded conformal factor provided the integral of $|\boldsymbol A|^2$, the squared-length of the second fundamental form, is less than $γ_n=8π$. It has since been shown that the optimal bounds on the integral of $|\boldsymbol A|^2$ that guarantee this result are: $γ_3 = 8π$ and $γ_n = 4π$ for $n \geq 4$. For isothermal immersions, this hypothesis is equivalent to saying the integral of the sum of the squares of the principal curvatures is less than $γ_n$. The goal here is to prove that when $n=3$ the same conclusion holds under weaker hypotheses. In particular, it holds for isothermal immersions when $|\boldsymbol A|$ is square-integrable and the integral of $|K|$, $K$ the Gauss curvature, is less than $4π$. Since $2|K| \leq |\boldsymbol A|^2$ this implies the known result for isothermal immersions, but $|K|$ may be small when $|\boldsymbol A|^2$ is large. That the result under the weaker hypothesis is sharp is shown by Enneper's surface and stereographic projections. The method, which is purely analytic, is then extended to investigate the case when the length of the second fundamental form is square-integrable.

math.AP

Isothermal Navier-Stokes Equations and Radon Transform

In the paper we prove the existence results for initial-value boundary value problems for compressible isothermal Navier-Stokes equations. We restrict ourselves to 2D case of a problem with no-slip condition for nonstationary motion of viscous compressible isothermal fluid. However, the technique of modeling and analysis presented here is general and can be used for 3D problems.

math.AP

Steady 3D viscous compressible flows with adiabatic exponent $γ\in (1,\infty)$

The Navier-Stokes equations for compressible barotropic flow in the stationary three dimensional case are considered. It is assumed that a fluid occupies a bounded domain and satisfies the no-slip boundary condition. The existence of a weak solution under the assumption that the adiabatic exponent satisfies $γ>1$ is proved. These results cover the cases of monoatomic, diatomic, and polyatomic gases.

math.AP