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Implicit-Explicit Runge-Kutta schemes for hyperbolic systems ... - utenti

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Hyperbolic <strong>systems</strong> with relaxation<br />

Introduction<br />

Many physical models are described by <strong>hyperbolic</strong> <strong>systems</strong> with relaxation of the <strong>for</strong>m<br />

∂tU + ∂xF (U) = 1<br />

R(U), x ∈ R,<br />

ε<br />

where U = U(x, t) ∈ R N , F : R N → R N , F ′ (U) has real eigenvalues and admits a basis of<br />

eigenvectors ∀ U ∈ R N and ε > 0 is called relaxation parameter.<br />

Examples<br />

Gas dynamics<br />

Shallow water<br />

Discrete kinetic models<br />

Extended Thermodynamics<br />

Hydrodynamical models <strong>for</strong> semiconductors<br />

Traffic models<br />

Granular gases<br />

...................<br />

Related problems: convection-diffusion-reaction, low Mach number/diffusive limits<br />

⊲ Purpose of the talk is to give an overview of <strong>Runge</strong>-<strong>Kutta</strong> time discretization methods<br />

<strong>for</strong> such <strong>systems</strong>, with particular emphasis on the treatment of stiff regimes.<br />

2

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