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

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

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Prototype problem<br />

A simple non trivial 2 × 2 relaxation system is given by<br />

ut + vx = 0<br />

vt + ux = −µ(v − bu)<br />

In the stiff limit µ → ∞ <strong>for</strong> 0 < b < 1 the system relaxes to the equation<br />

ut + bux = 0<br />

We look <strong>for</strong> a Fourier solution u = û(t)e iξx , v = ˆv(t)e iξx . One obtains<br />

ût + iξˆv = 0<br />

ˆvt + iξû = −µ(ˆv − bû)<br />

The system can be written in vector <strong>for</strong>m as<br />

where<br />

U =<br />

� û<br />

ˆv<br />

�<br />

, C1 = −iξ<br />

dU<br />

dt = C1U + C2U<br />

� 0 1<br />

1 0<br />

�<br />

, C2 = −µ<br />

� 0 0<br />

−b 1<br />

The boundary of the region of absolute stability is given by the relation<br />

ρ(R(Z1, Z2)) = 1<br />

where ρ denotes the spectral radius, and Z1 = hC1, Z2 = hC2.<br />

�<br />

21

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