| Turbulence | Large-scale \(\mathbf{B}\)-Field | Fluctuating \(\mathbf{B}\)-Field | Total \(\mathbf{B}\)-Field | ||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Simulation ID | \(\mathcal{M}\) | \(\frac{\ell_{\text{cor}, v}}{\ell_0}\) | \(\mathop{\mathrm{\mathcal{M}_{\text{A0}}}}\) | \(\frac{B_0}{c_s \rho_0^{1/2}}\) | \(\left\langle \frac{\delta B^2}{c_s^2 \rho_0} \right\rangle_{\mathop{\mathrm{\mathcal{V}}}}\) | \(\left\langle \left(\frac{\delta\mathbf{B}\cdot\mathop{\mathrm{\mathbf{B}_0}}}{c_s^2 \rho_0}\right)^2 \right\rangle^{1/2}_{\mathop{\mathrm{\mathcal{V}}}}\) | \(\mathop{\mathrm{\mathcal{M}_{\text{A,turb}}}}\) | \(\mathop{\mathrm{\mathcal{M}_{\text{A,total}}}}\) | |||||||
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | |||||||
M05MA001 |
\(0.567\) | \(_{-0.07}^{+0.02}\) | \(1.48\) | \(_{-0.07}^{+0.05}\) | \(0.0113\) | \(_{-0.001}^{+0.0003}\) | \(177.0\) | \(0.000191\) | \(_{-0.005}^{+0.004}\) | \(2.32\) | \(_{-0.5}^{+0.4}\) | \(392.0\) | \(_{-40.0}^{+20.0}\) | \(0.0113\) | \(_{-0.001}^{+0.0003}\) |
M05MA01 |
\(0.566\) | \(_{-0.07}^{+0.02}\) | \(1.47\) | \(_{-0.07}^{+0.05}\) | \(0.113\) | \(_{-0.01}^{+0.004}\) | \(17.7\) | \(0.0181\) | \(_{-0.04}^{+0.03}\) | \(2.23\) | \(_{-0.4}^{+0.3}\) | \(35.6\) | \(_{-2.0}^{+2.0}\) | \(0.113\) | \(_{-0.01}^{+0.004}\) |
M05MA05 |
\(0.534\) | \(_{-0.04}^{+0.004}\) | \(1.44\) | \(_{-0.07}^{+0.02}\) | \(0.534\) | \(_{-0.04}^{+0.004}\) | \(3.54\) | \(0.233\) | \(_{-0.08}^{+0.05}\) | \(1.16\) | \(_{-0.1}^{+0.05}\) | \(7.28\) | \(_{-0.2}^{+0.3}\) | \(0.544\) | \(_{-0.05}^{+0.005}\) |
M05MA1 |
\(0.469\) | \(_{-0.05}^{+0.01}\) | \(0.953\) | \(_{-0.005}^{+0.02}\) | \(0.938\) | \(_{-0.1}^{+0.03}\) | \(1.77\) | \(1.2\) | \(_{-0.3}^{+0.1}\) | \(1.0\) | \(_{-0.07}^{+0.08}\) | \(2.75\) | \(_{-0.2}^{+0.1}\) | \(0.974\) | \(_{-0.08}^{+0.07}\) |
M05MA2 |
\(0.462\) | \(_{-0.03}^{+0.03}\) | \(0.783\) | \(_{-0.03}^{+0.06}\) | \(1.85\) | \(_{-0.1}^{+0.1}\) | \(0.886\) | \(3.17\) | \(_{-0.3}^{+0.3}\) | \(0.871\) | \(_{-0.07}^{+0.03}\) | \(1.67\) | \(_{-0.08}^{+0.2}\) | \(1.59\) | \(_{-0.09}^{+0.2}\) |
M05MA4 |
\(0.473\) | \(_{-0.03}^{+0.06}\) | \(0.838\) | \(_{-0.03}^{+0.03}\) | \(3.79\) | \(_{-0.2}^{+0.5}\) | \(0.443\) | \(3.12\) | \(_{-0.2}^{+0.2}\) | \(0.415\) | \(_{-0.009}^{+0.02}\) | \(1.98\) | \(_{-0.2}^{+0.2}\) | \(2.1\) | \(_{-0.2}^{+0.4}\) |
M05MA6 |
\(0.483\) | \(_{-0.03}^{+0.06}\) | \(0.904\) | \(_{-0.03}^{+0.03}\) | \(5.8\) | \(_{-0.4}^{+0.8}\) | \(0.295\) | \(2.74\) | \(_{-0.1}^{+0.09}\) | \(0.256\) | \(_{-0.006}^{+0.01}\) | \(2.32\) | \(_{-0.1}^{+0.4}\) | \(2.51\) | \(_{-0.2}^{+0.5}\) |
M05MA8 |
\(0.502\) | \(_{-0.02}^{+0.06}\) | \(0.907\) | \(_{-0.02}^{+0.05}\) | \(8.03\) | \(_{-0.3}^{+1.0}\) | \(0.222\) | \(2.47\) | \(_{-0.2}^{+0.1}\) | \(0.192\) | \(_{-0.01}^{+0.009}\) | \(2.76\) | \(_{-0.1}^{+0.3}\) | \(2.99\) | \(_{-0.2}^{+0.3}\) |
M05MA10 |
\(0.514\) | \(_{-0.03}^{+0.06}\) | \(0.934\) | \(_{-0.03}^{+0.02}\) | \(10.3\) | \(_{-0.5}^{+1.0}\) | \(0.177\) | \(2.24\) | \(_{-0.07}^{+0.1}\) | \(0.145\) | \(_{-0.006}^{+0.01}\) | \(3.05\) | \(_{-0.2}^{+0.4}\) | \(3.18\) | \(_{-0.1}^{+0.4}\) |
M05MA100 |
\(0.637\) | \(_{-0.05}^{+0.09}\) | \(0.889\) | \(_{-0.03}^{+0.04}\) | \(127.0\) | \(_{-10.0}^{+20.0}\) | \(0.0177\) | \(0.721\) | \(_{-0.3}^{+0.1}\) | \(0.00852\) | \(_{-0.001}^{+0.0008}\) | \(7.9\) | \(_{-1.0}^{+3.0}\) | \(7.92\) | \(_{-1.0}^{+3.0}\) |
M05MA1000 |
\(0.672\) | \(_{-0.05}^{+0.07}\) | \(0.835\) | \(_{-0.04}^{+0.03}\) | \(1340.0\) | \(_{-100.0}^{+100.0}\) | \(0.00177\) | \(0.36\) | \(_{-0.3}^{+0.2}\) | \(0.000613\) | \(_{-0.0002}^{+0.0001}\) | \(11.8\) | \(_{-3.0}^{+8.0}\) | \(11.8\) | \(_{-3.0}^{+8.0}\) |
M2MA001 |
\(1.9\) | \(_{-0.06}^{+0.04}\) | \(1.34\) | \(_{-0.09}^{+0.02}\) | \(0.0095\) | \(_{-0.0003}^{+0.0002}\) | \(709.0\) | \(0.000879\) | \(_{-0.003}^{+0.02}\) | \(18.7\) | \(_{-2.0}^{+9.0}\) | \(498.0\) | \(_{-30.0}^{+20.0}\) | \(0.00943\) | \(_{-0.0003}^{+0.0002}\) |
M2MA01 |
\(1.85\) | \(_{-0.02}^{+0.06}\) | \(1.37\) | \(_{-0.1}^{+0.03}\) | \(0.0926\) | \(_{-0.001}^{+0.003}\) | \(70.9\) | \(0.0989\) | \(_{-0.03}^{+0.1}\) | \(18.4\) | \(_{-1.0}^{+4.0}\) | \(41.1\) | \(_{-3.0}^{+2.0}\) | \(0.0917\) | \(_{-0.001}^{+0.003}\) |
M2MA05 |
\(2.24\) | \(_{-0.09}^{+0.07}\) | \(1.26\) | \(_{-0.06}^{+0.08}\) | \(0.561\) | \(_{-0.02}^{+0.02}\) | \(14.2\) | \(6.81\) | \(_{-0.3}^{+0.3}\) | \(20.6\) | \(_{-2.0}^{+3.0}\) | \(5.28\) | \(_{-0.3}^{+0.3}\) | \(0.575\) | \(_{-0.03}^{+0.01}\) |
M2MA1 |
\(1.98\) | \(_{-0.09}^{+0.1}\) | \(0.845\) | \(_{-0.02}^{+0.02}\) | \(0.989\) | \(_{-0.05}^{+0.05}\) | \(7.09\) | \(25.3\) | \(_{-1.0}^{+0.3}\) | \(16.3\) | \(_{-1.0}^{+0.7}\) | \(2.47\) | \(_{-0.2}^{+0.2}\) | \(1.01\) | \(_{-0.06}^{+0.05}\) |
M2MA2 |
\(1.95\) | \(_{-0.2}^{+0.2}\) | \(0.815\) | \(_{-0.04}^{+0.04}\) | \(1.95\) | \(_{-0.2}^{+0.2}\) | \(3.54\) | \(40.6\) | \(_{-0.9}^{+0.6}\) | \(12.3\) | \(_{-1.0}^{+0.7}\) | \(1.73\) | \(_{-0.07}^{+0.4}\) | \(1.54\) | \(_{-0.1}^{+0.1}\) |
M2MA4 |
\(2.07\) | \(_{-0.1}^{+0.2}\) | \(0.92\) | \(_{-0.04}^{+0.02}\) | \(4.13\) | \(_{-0.3}^{+0.5}\) | \(1.77\) | \(37.0\) | \(_{-0.3}^{+0.3}\) | \(5.88\) | \(_{-0.3}^{+0.4}\) | \(2.39\) | \(_{-0.4}^{+0.1}\) | \(2.39\) | \(_{-0.4}^{+0.3}\) |
M2MA6 |
\(2.09\) | \(_{-0.2}^{+0.2}\) | \(0.946\) | \(_{-0.05}^{+0.02}\) | \(6.26\) | \(_{-0.6}^{+0.6}\) | \(1.18\) | \(33.8\) | \(_{-0.4}^{+0.5}\) | \(3.83\) | \(_{-0.1}^{+0.1}\) | \(2.45\) | \(_{-0.3}^{+0.5}\) | \(2.68\) | \(_{-0.5}^{+0.6}\) |
M2MA8 |
\(2.05\) | \(_{-0.2}^{+0.09}\) | \(0.945\) | \(_{-0.02}^{+0.04}\) | \(8.21\) | \(_{-0.7}^{+0.4}\) | \(0.886\) | \(21.5\) | \(_{-0.3}^{+0.3}\) | \(2.39\) | \(_{-0.1}^{+0.1}\) | \(3.44\) | \(_{-0.3}^{+0.2}\) | \(3.91\) | \(_{-0.3}^{+0.2}\) |
M2MA10 |
\(2.11\) | \(_{-0.2}^{+0.1}\) | \(0.987\) | \(_{-0.03}^{+0.03}\) | \(10.5\) | \(_{-1.0}^{+0.7}\) | \(0.709\) | \(18.4\) | \(_{-0.1}^{+0.3}\) | \(1.74\) | \(_{-0.04}^{+0.1}\) | \(4.07\) | \(_{-0.6}^{+0.3}\) | \(4.65\) | \(_{-0.9}^{+0.4}\) |
M2MA100 |
\(2.36\) | \(_{-0.2}^{+0.1}\) | \(1.01\) | \(_{-0.02}^{+0.03}\) | \(118.0\) | \(_{-8.0}^{+6.0}\) | \(0.0709\) | \(3.3\) | \(_{-0.5}^{+0.08}\) | \(0.0729\) | \(_{-0.006}^{+0.003}\) | \(16.1\) | \(_{-2.0}^{+3.0}\) | \(17.0\) | \(_{-3.0}^{+4.0}\) |
M2MA1000 |
\(2.37\) | \(_{-0.1}^{+0.08}\) | \(0.999\) | \(_{-0.05}^{+0.01}\) | \(1180.0\) | \(_{-70.0}^{+40.0}\) | \(0.00709\) | \(0.276\) | \(_{-0.3}^{+0.3}\) | \(0.00214\) | \(_{-0.0007}^{+0.0005}\) | \(61.9\) | \(_{-20.0}^{+40.0}\) | \(62.8\) | \(_{-20.0}^{+40.0}\) |
M4MA01 |
\(4.03\) | \(_{-0.5}^{+0.06}\) | \(1.39\) | \(_{-0.09}^{+0.05}\) | \(0.101\) | \(_{-0.01}^{+0.002}\) | \(142.0\) | \(0.838\) | \(_{-0.4}^{+0.2}\) | \(106.0\) | \(_{-20.0}^{+9.0}\) | \(36.5\) | \(_{-3.0}^{+3.0}\) | \(0.1\) | \(_{-0.01}^{+0.002}\) |
M4MA05 |
\(4.08\) | \(_{-0.1}^{+0.04}\) | \(1.27\) | \(_{-0.1}^{+0.04}\) | \(0.51\) | \(_{-0.01}^{+0.005}\) | \(28.4\) | \(24.4\) | \(_{-0.6}^{+0.4}\) | \(74.1\) | \(_{-7.0}^{+7.0}\) | \(4.94\) | \(_{-0.4}^{+0.3}\) | \(0.513\) | \(_{-0.01}^{+0.007}\) |
M4MA1 |
\(4.12\) | \(_{-0.4}^{+0.5}\) | \(0.832\) | \(_{-0.04}^{+0.04}\) | \(1.03\) | \(_{-0.09}^{+0.1}\) | \(14.2\) | \(84.3\) | \(_{-2.0}^{+2.0}\) | \(61.9\) | \(_{-10.0}^{+7.0}\) | \(2.49\) | \(_{-0.1}^{+0.3}\) | \(1.02\) | \(_{-0.1}^{+0.05}\) |
M4MA2 |
\(4.02\) | \(_{-0.3}^{+0.2}\) | \(0.846\) | \(_{-0.02}^{+0.04}\) | \(2.01\) | \(_{-0.1}^{+0.08}\) | \(7.09\) | \(125.0\) | \(_{-1.0}^{+1.0}\) | \(43.4\) | \(_{-6.0}^{+2.0}\) | \(1.93\) | \(_{-0.1}^{+0.2}\) | \(1.49\) | \(_{-0.1}^{+0.2}\) |
M4MA4 |
\(4.03\) | \(_{-0.4}^{+0.2}\) | \(0.916\) | \(_{-0.03}^{+0.02}\) | \(4.03\) | \(_{-0.4}^{+0.2}\) | \(3.54\) | \(109.0\) | \(_{-0.5}^{+0.2}\) | \(20.3\) | \(_{-0.5}^{+2.0}\) | \(2.38\) | \(_{-0.3}^{+0.1}\) | \(2.41\) | \(_{-0.3}^{+0.1}\) |
M4MA6 |
\(3.97\) | \(_{-0.4}^{+0.2}\) | \(0.959\) | \(_{-0.02}^{+0.02}\) | \(5.96\) | \(_{-0.6}^{+0.3}\) | \(2.36\) | \(76.3\) | \(_{-0.6}^{+0.3}\) | \(11.7\) | \(_{-0.4}^{+0.7}\) | \(2.94\) | \(_{-0.3}^{+0.4}\) | \(3.29\) | \(_{-0.2}^{+0.4}\) |
M4MA8 |
\(4.05\) | \(_{-0.5}^{+0.08}\) | \(0.979\) | \(_{-0.03}^{+0.02}\) | \(8.1\) | \(_{-1.0}^{+0.2}\) | \(1.77\) | \(68.5\) | \(_{-0.4}^{+0.6}\) | \(8.38\) | \(_{-0.3}^{+0.3}\) | \(3.41\) | \(_{-0.6}^{+0.3}\) | \(4.15\) | \(_{-1.0}^{+0.4}\) |
M4MA10 |
\(3.91\) | \(_{-0.2}^{+0.2}\) | \(0.994\) | \(_{-0.01}^{+0.03}\) | \(9.78\) | \(_{-0.6}^{+0.5}\) | \(1.42\) | \(59.7\) | \(_{-0.2}^{+0.2}\) | \(6.27\) | \(_{-0.3}^{+0.2}\) | \(3.69\) | \(_{-0.1}^{+0.3}\) | \(4.23\) | \(_{-0.3}^{+0.9}\) |
M4MA100 |
\(4.21\) | \(_{-0.08}^{+0.2}\) | \(1.02\) | \(_{-0.02}^{+0.03}\) | \(105.0\) | \(_{-2.0}^{+5.0}\) | \(0.142\) | \(6.29\) | \(_{-0.4}^{+0.4}\) | \(0.203\) | \(_{-0.01}^{+0.01}\) | \(21.0\) | \(_{-2.0}^{+3.0}\) | \(24.2\) | \(_{-2.0}^{+5.0}\) |
M4MA1000 |
\(4.31\) | \(_{-0.2}^{+0.1}\) | \(1.05\) | \(_{-0.01}^{+0.02}\) | \(1080.0\) | \(_{-50.0}^{+30.0}\) | \(0.0142\) | \(0.391\) | \(_{-0.3}^{+0.4}\) | \(0.00519\) | \(_{-0.001}^{+0.001}\) | \(115.0\) | \(_{-40.0}^{+20.0}\) | \(128.0\) | \(_{-50.0}^{+30.0}\) |
M6MA01 |
\(6.96\) | \(_{-0.8}^{+0.5}\) | \(1.35\) | \(_{-0.04}^{+0.05}\) | \(0.116\) | \(_{-0.01}^{+0.008}\) | \(213.0\) | \(3.86\) | \(_{-0.7}^{+0.3}\) | \(325.0\) | \(_{-60.0}^{+20.0}\) | \(29.0\) | \(_{-3.0}^{+4.0}\) | \(0.115\) | \(_{-0.01}^{+0.008}\) |
M6MA05 |
\(6.44\) | \(_{-0.1}^{+0.2}\) | \(1.21\) | \(_{-0.04}^{+0.02}\) | \(0.536\) | \(_{-0.01}^{+0.02}\) | \(42.5\) | \(58.0\) | \(_{-0.7}^{+1.0}\) | \(169.0\) | \(_{-10.0}^{+10.0}\) | \(5.02\) | \(_{-0.3}^{+0.3}\) | \(0.535\) | \(_{-0.01}^{+0.01}\) |
M6MA1 |
\(6.01\) | \(_{-0.8}^{+0.8}\) | \(0.844\) | \(_{-0.02}^{+0.04}\) | \(1.0\) | \(_{-0.1}^{+0.1}\) | \(21.3\) | \(157.0\) | \(_{-4.0}^{+1.0}\) | \(121.0\) | \(_{-20.0}^{+10.0}\) | \(2.73\) | \(_{-0.2}^{+0.2}\) | \(0.937\) | \(_{-0.2}^{+0.1}\) |
M6MA2 |
\(5.81\) | \(_{-0.3}^{+0.3}\) | \(0.844\) | \(_{-0.03}^{+0.03}\) | \(1.94\) | \(_{-0.09}^{+0.1}\) | \(10.6\) | \(217.0\) | \(_{-0.5}^{+2.0}\) | \(83.7\) | \(_{-5.0}^{+9.0}\) | \(2.1\) | \(_{-0.1}^{+0.2}\) | \(1.58\) | \(_{-0.09}^{+0.09}\) |
M6MA4 |
\(6.23\) | \(_{-0.4}^{+0.1}\) | \(0.94\) | \(_{-0.01}^{+0.02}\) | \(4.15\) | \(_{-0.3}^{+0.08}\) | \(5.32\) | \(202.0\) | \(_{-2.0}^{+0.8}\) | \(42.8\) | \(_{-5.0}^{+2.0}\) | \(2.55\) | \(_{-0.2}^{+0.2}\) | \(2.53\) | \(_{-0.2}^{+0.3}\) |
M6MA6 |
\(5.96\) | \(_{-0.6}^{+0.4}\) | \(0.946\) | \(_{-0.01}^{+0.02}\) | \(5.96\) | \(_{-0.6}^{+0.4}\) | \(3.54\) | \(168.0\) | \(_{-1.0}^{+1.0}\) | \(25.8\) | \(_{-2.0}^{+3.0}\) | \(2.82\) | \(_{-0.2}^{+0.3}\) | \(3.04\) | \(_{-0.2}^{+0.3}\) |
M6MA8 |
\(5.96\) | \(_{-0.5}^{+0.2}\) | \(0.979\) | \(_{-0.01}^{+0.01}\) | \(7.95\) | \(_{-0.6}^{+0.2}\) | \(2.66\) | \(139.0\) | \(_{-0.9}^{+0.3}\) | \(17.4\) | \(_{-0.6}^{+1.0}\) | \(3.39\) | \(_{-0.4}^{+0.2}\) | \(3.73\) | \(_{-0.4}^{+0.2}\) |
M6MA10 |
\(5.99\) | \(_{-0.5}^{+0.2}\) | \(0.99\) | \(_{-0.02}^{+0.02}\) | \(9.99\) | \(_{-0.8}^{+0.4}\) | \(2.13\) | \(124.0\) | \(_{-1.0}^{+0.5}\) | \(12.6\) | \(_{-0.4}^{+1.0}\) | \(3.82\) | \(_{-0.6}^{+0.8}\) | \(4.11\) | \(_{-0.7}^{+1.0}\) |
M8MA01 |
\(8.7\) | \(_{-0.9}^{+0.09}\) | \(1.49\) | \(_{-0.1}^{+0.02}\) | \(0.109\) | \(_{-0.01}^{+0.001}\) | \(284.0\) | \(4.53\) | \(_{-0.7}^{+0.4}\) | \(488.0\) | \(_{-90.0}^{+40.0}\) | \(32.0\) | \(_{-4.0}^{+4.0}\) | \(0.108\) | \(_{-0.01}^{+0.001}\) |
M8MA05 |
\(8.35\) | \(_{-0.3}^{+0.2}\) | \(1.14\) | \(_{-0.02}^{+0.02}\) | \(0.522\) | \(_{-0.02}^{+0.01}\) | \(56.7\) | \(90.2\) | \(_{-0.6}^{+1.0}\) | \(278.0\) | \(_{-30.0}^{+20.0}\) | \(5.01\) | \(_{-0.4}^{+0.3}\) | \(0.505\) | \(_{-0.03}^{+0.01}\) |
M8MA1 |
\(8.16\) | \(_{-1.0}^{+0.6}\) | \(0.837\) | \(_{-0.03}^{+0.04}\) | \(1.02\) | \(_{-0.1}^{+0.08}\) | \(28.4\) | \(257.0\) | \(_{-4.0}^{+2.0}\) | \(205.0\) | \(_{-20.0}^{+10.0}\) | \(2.74\) | \(_{-0.3}^{+0.3}\) | \(0.92\) | \(_{-0.1}^{+0.07}\) |
M8MA2 |
\(8.15\) | \(_{-0.5}^{+0.4}\) | \(0.863\) | \(_{-0.03}^{+0.03}\) | \(2.04\) | \(_{-0.1}^{+0.1}\) | \(14.2\) | \(395.0\) | \(_{-1.0}^{+1.0}\) | \(148.0\) | \(_{-8.0}^{+7.0}\) | \(2.25\) | \(_{-0.2}^{+0.2}\) | \(1.59\) | \(_{-0.2}^{+0.1}\) |
M8MA4 |
\(7.99\) | \(_{-0.4}^{+0.3}\) | \(0.933\) | \(_{-0.03}^{+0.01}\) | \(4.0\) | \(_{-0.2}^{+0.1}\) | \(7.09\) | \(344.0\) | \(_{-2.0}^{+0.8}\) | \(72.7\) | \(_{-8.0}^{+4.0}\) | \(2.41\) | \(_{-0.1}^{+0.2}\) | \(2.3\) | \(_{-0.2}^{+0.2}\) |
M8MA6 |
\(7.97\) | \(_{-0.9}^{+0.4}\) | \(0.938\) | \(_{-0.02}^{+0.02}\) | \(5.98\) | \(_{-0.7}^{+0.3}\) | \(4.73\) | \(278.0\) | \(_{-1.0}^{+2.0}\) | \(42.4\) | \(_{-1.0}^{+7.0}\) | \(2.84\) | \(_{-0.5}^{+0.2}\) | \(2.93\) | \(_{-0.6}^{+0.3}\) |
M8MA8 |
\(7.82\) | \(_{-0.4}^{+0.4}\) | \(0.994\) | \(_{-0.02}^{+0.01}\) | \(7.82\) | \(_{-0.4}^{+0.4}\) | \(3.54\) | \(247.0\) | \(_{-1.0}^{+0.8}\) | \(31.5\) | \(_{-2.0}^{+2.0}\) | \(3.2\) | \(_{-0.3}^{+0.2}\) | \(3.46\) | \(_{-0.3}^{+0.5}\) |
M8MA10 |
\(8.06\) | \(_{-1.0}^{+0.2}\) | \(1.01\) | \(_{-0.03}^{+0.02}\) | \(10.1\) | \(_{-1.0}^{+0.3}\) | \(2.84\) | \(197.0\) | \(_{-0.5}^{+1.0}\) | \(22.3\) | \(_{-0.5}^{+1.0}\) | \(3.72\) | \(_{-0.4}^{+0.6}\) | \(3.89\) | \(_{-0.5}^{+0.6}\) |
M10MA01 |
\(11.3\) | \(_{-1.0}^{+0.3}\) | \(1.45\) | \(_{-0.09}^{+0.07}\) | \(0.113\) | \(_{-0.01}^{+0.003}\) | \(354.0\) | \(6.76\) | \(_{-1.0}^{+1.0}\) | \(720.0\) | \(_{-200.0}^{+100.0}\) | \(33.7\) | \(_{-7.0}^{+8.0}\) | \(0.112\) | \(_{-0.01}^{+0.003}\) |
M10MA05 |
\(10.2\) | \(_{-0.3}^{+0.3}\) | \(1.13\) | \(_{-0.02}^{+0.02}\) | \(0.509\) | \(_{-0.02}^{+0.01}\) | \(70.9\) | \(143.0\) | \(_{-2.0}^{+2.0}\) | \(420.0\) | \(_{-40.0}^{+20.0}\) | \(4.88\) | \(_{-0.5}^{+0.6}\) | \(0.496\) | \(_{-0.02}^{+0.02}\) |
M10MA1 |
\(9.72\) | \(_{-0.9}^{+0.9}\) | \(0.868\) | \(_{-0.03}^{+0.03}\) | \(0.972\) | \(_{-0.09}^{+0.09}\) | \(35.4\) | \(338.0\) | \(_{-4.0}^{+3.0}\) | \(309.0\) | \(_{-40.0}^{+20.0}\) | \(2.79\) | \(_{-0.1}^{+0.4}\) | \(0.888\) | \(_{-0.1}^{+0.06}\) |
M10MA2 |
\(10.5\) | \(_{-0.8}^{+0.3}\) | \(0.888\) | \(_{-0.02}^{+0.02}\) | \(2.1\) | \(_{-0.2}^{+0.07}\) | \(17.7\) | \(549.0\) | \(_{-1.0}^{+0.9}\) | \(215.0\) | \(_{-10.0}^{+9.0}\) | \(2.39\) | \(_{-0.3}^{+0.1}\) | \(1.56\) | \(_{-0.1}^{+0.2}\) |
M10MA4 |
\(10.3\) | \(_{-0.4}^{+0.4}\) | \(0.931\) | \(_{-0.03}^{+0.03}\) | \(4.12\) | \(_{-0.2}^{+0.2}\) | \(8.86\) | \(529.0\) | \(_{-2.0}^{+2.0}\) | \(112.0\) | \(_{-6.0}^{+8.0}\) | \(2.42\) | \(_{-0.2}^{+0.4}\) | \(2.32\) | \(_{-0.2}^{+0.4}\) |
M10MA6 |
\(9.78\) | \(_{-1.0}^{+0.3}\) | \(0.952\) | \(_{-0.03}^{+0.02}\) | \(5.87\) | \(_{-0.7}^{+0.2}\) | \(5.91\) | \(398.0\) | \(_{-0.7}^{+2.0}\) | \(65.2\) | \(_{-3.0}^{+7.0}\) | \(2.7\) | \(_{-0.4}^{+0.3}\) | \(2.77\) | \(_{-0.4}^{+0.3}\) |
M10MA8 |
\(10.0\) | \(_{-0.9}^{+0.4}\) | \(0.997\) | \(_{-0.02}^{+0.02}\) | \(8.03\) | \(_{-0.7}^{+0.3}\) | \(4.43\) | \(346.0\) | \(_{-1.0}^{+1.0}\) | \(46.7\) | \(_{-1.0}^{+4.0}\) | \(3.27\) | \(_{-0.4}^{+0.4}\) | \(3.41\) | \(_{-0.6}^{+0.4}\) |
M10MA10 |
\(9.42\) | \(_{-0.5}^{+0.2}\) | \(0.99\) | \(_{-0.01}^{+0.01}\) | \(9.42\) | \(_{-0.5}^{+0.2}\) | \(3.54\) | \(288.0\) | \(_{-3.0}^{+2.0}\) | \(34.3\) | \(_{-4.0}^{+3.0}\) | \(3.37\) | \(_{-0.2}^{+0.3}\) | \(3.5\) | \(_{-0.3}^{+0.5}\) |
Notes: All simulations listed are run with grid resolutions of \(16^3\), \(36^3\), \(72^3\), \(144^3\) and \(288^3\). All statistics are spatially averaged over the entire domain, \(\mathop{\mathrm{\mathcal{V}}}= \mathop{\mathrm{\mathcal{V}}}_{L}\), and are computed for 51 time realisations, across 5 correlation times of the Ornstein-Uhlenbeck forcing function. From the distributions in time, we report the values for the \(16^{\rm th}\), \(50^{\rm th}\), and \(84^{\rm th}\) percentiles. This process minimises the possibility of using statistics that are undergoing temporally intermittent turbulent events. Column (1): the simulation ID, used throughout this study. Column (2): the turbulent Mach number, \(\mathcal{M}\equiv \left\langle (\delta v / c_s)^2 \right\rangle^{1/2}_{\mathop{\mathrm{\mathcal{V}}}_{L}}\). Column (3): the correlation scale of the turbulence, \(\ell_{\text{cor},v}\), in units of the driving scale, \(\ell_0\), defined directly from the power spectra. Column (4): the Alfvén Mach number of the mean magnetic field, \(\mathop{\mathrm{\mathcal{M}_{\text{A0}}}}\equiv \left\langle (\delta v \sqrt{4\pi\rho_0} ) / B_0 \right\rangle\), with fluctuations coming from \(\delta v\), since \(\partial_{x_i}\mathbf{B}_0 = \partial_{t} \mathbf{B}_0 = 0\). Column (5): the mean magnetic field strength in units of \(c_s \rho_0^{1/2}\). Column (6): the volume-averaged square of the turbulent magnetic field, proportional to the turbulent magnetic energy, in units of thermal energy. Column (7): the volume-averaged root-mean-squared of the magnetic coupling term \(\mathop{\mathrm{\delta\mathbf{B}\cdot\mathop{\mathrm{\mathbf{B}_0}}}}\), in units of thermal energy. Column (8): the Alfvén Mach number of the turbulent magnetic field. Column (9): the Alfvén Mach number of the total magnetic field.