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A Hamiltonian regularization of the Burgers equation
PDE Seminar| Speaker: | Razvan Fetecau, Stanford University |
| Location: | 3106 MSB |
| Start time: | Thu, May 18 2006, 3:10PM |
Description
We consider the following scalar equation:
u_t + uu_x − α^2 u_{txx} − α^2 uu_{xxx} = 0, (1)
with α > 0. We may rewrite (1) as
v_t + uv_x = 0, (2)
where
v = u − α^2 u_{xx} , (3)
One can think of the equation (2) as the inviscid Burgers equation,
v_t + v v_x = 0,
where the convective velocity in the nonlinear term is replaced by a smoother velocity field
u. This idea goes back to Leray (1934) who employed it in the context of the incompressible
Navier-Stokes equation. Leray’s program consisted in proving existence of solutions for his
modified equations and then showing that these solutions converge, as α ↓ 0, to solutions of
Navier-Stokes.
We apply Leray’s ideas in the context of Burgers equation. We show strong analytical and
numerical indication that (2)-(3) (or equivalently, (1)) represent a valid regularization of the
Burgers equation. That is, we claim that solutions uα (x, t) of (1) converge strongly, as α → 0,
to unique entropy solutions of the inviscid Burgers equation. Interestingly, for all α > 0, the
regularized equation possesses a Hamiltonian structure.
We also study the stability of the traveling waves for equation (1). These traveling waves
consist of ”fronts,” which are monotonic profiles that connect a left state to a right state. The
front stability results show that the regularized equation (1) mirrors the physics of rarefaction
and shock waves in the Burgers equation.
