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Home All issues Volume 498 / No 1 (April IV 2009) A&A, 498 1 (2009) 241-271 Full HTML
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Table B.4:

Continuation of Table B.3. For the MBI model with $b_0^z = 10 ~ {\rm G}$, we do not provide values for the Maxwell stress, because the magnetic field behaves similar to a purely passive field.
Field Grid size Resolution Rot $\partial _{\varpi } S$ bz0 BC $\sigma $ $M_{\varpi \phi }^{{\rm term}}$ $M_{\varpi \phi }^{{\rm max}}$ $\left\langle M_{\varpi \phi} \right\rangle$
  [km3]     $\left[{\rm km}^{-1}\right]$ $\left[10^{12}~{\rm G}\right]$   $\left[ {\rm ms^{-1}} \right]$ $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$ $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$ $\left[10^{28}~{\rm G}^2 ~ {\rm cm}^{-3}\right]$

V3

 $1 \times 1 \times 1$ $50 \times 50 \times 50$ d 0 10 d 0.66 0.13 0.24 0.16
  $1 \times 1 \times 1$ $50 \times 50 \times 50$ d 0 20 d 0.96 0.53 0.53 0.21
  $1 \times 1 \times 1$ $50 \times 50 \times 50$ d 0 40 d 1.03 1.5 1.5 0.27
  $1 \times 4 \times 1$ $50 \times 200 \times 50$ d 0 10 d 0.66 0.13 0.52 0.24
  $1 \times 4 \times 1$ $50 \times 200 \times 50$ d 0 20 d 0.90 0.36 0.80 0.43
  $1 \times 4 \times 1$ $100 \times 400 \times 100$ d 0 20 d 1.08 1.1 1.1 0.20
  $1 \times 4 \times 1$ $100 \times 400 \times 100$ d 0 20 p 1.08 1.5 1.5 0.21
U3 $1 \times 2 \times 1$ $ 26 \times 50 \times 26 $ d -0.038 20 d 1.5 1.9 5.3 0.83
  $1 \times 2 \times 1$ $ 26 \times 50 \times 26 $ d -0.038 40 d 1.7 4.1 7.2 1.1
  $1 \times 2 \times 1$ $50 \times 100 \times 50$ d -0.038 20 d 1.7 3.1 3.1 0.16
  $1 \times 2 \times 1$ $50 \times 100 \times 50$ d -0.038 40 d 1.9 4.4 4.4 0.23
  $1 \times 2 \times 1$ $50 \times 100 \times 50$ r1900 -0.10 10-11 d 2.6      
  $1 \times 2 \times 1$ $50 \times 100 \times 50$ r1900 -0.10 0.01 d 2.6 $2.3 \times 10^{-8}$ 0.11 0.040
  $1 \times 2 \times 1$ $50 \times 100 \times 50$ r1900 -0.10 20 d 2.6 0.060 0.87 0.30
V3 $1 \times 2 \times 1$ $50 \times 100 \times 50$ d -0.038 20 d 1.6 0.54 0.54 0.011

Source LaTeX | All tables | In the text

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