This project reproduces a 2D magnetized Kelvin–Helmholtz (K–H) instability test using FLASH ver 4.8.
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Velocity:
$\vec{v} = \left[ \frac{M}{2} \tanh\left(\frac{y}{y_0}\right),\ 0,\ 0 \right]$ -
Magnetic field:
$\vec{B} = c_a \sqrt{\rho} \left[\cos\theta,\ 0,\ \sin\theta \right]$ -
Perturbation in the y-velocity:
$v_y = v_{y0} \sin(2\pi x) \exp\left(-\frac{y^2}{\sigma^2}\right)$
- Mach number:
$M=1$ - Shear scale height:
$y_0 = 1/20$ - Perturbation amplitude:
$v_{y0} = 10^{-2}$ - Perturbation width:
$\sigma = 0.1$ - Alfven speed:
$c_a = 0.1$ - Domain:
$[0, 1] \times [-1, 1]$ - Angle in xz plane:
$\theta = \pi/3$
Mignone, A., Tzeferacos, P., & Bodo, G. (2010). High-order conservative finite difference GLM–MHD schemes for cell-centered MHD. Journal of Computational Physics, arXiv:1001.2832