Table 13: Emission measure distributions for the Aschwanden & Schrijver (2002) models. $T_{\rm a}$ (keV) is the maximum temperature at the loop apex. $\Gamma $ is the loop cross section ratio between the loop apex and the photosphere. L is the loop half length (kpc), and $s_{\rm H}$ the heating scale height. M13 is the cluster mass in $10^{13}~M_{\hbox{$\odot$ }}$ within the radius R (kpc) where the loop is located. Y1-Y5 are the emission measures Yi (in m-3 of the temperature components 1-5. The corresponding temperatures are Ti = T1 / 2i-1. The density at the loop apex is $n_{\rm a}$(given in units of 104 m-3) and the average density over the loop volume is $\overline {n}$. The mass of an individual loop is Ml (in $10^{10}~M_{\hbox{$\odot$ }}$). Finally, N is the maximum number of loops per scale height, defined by $N\equiv 4\pi R^3/V$ with V the volume of an individual loop. All calculations are done for loops with a cross-sectional radius at the foot points (r0) of 10 kpc. For other values of r0, the following scaling applies: $Y_i\sim r_0^2$, $M_l\sim r_0^2$ and $N\sim r_0^{-2}$.
$T_{\rm a}$ $\Gamma $ L $s_{\rm H}/L$ M13 R Y2/Y1 Y3/Y1 Y4/Y1 Y5/Y1 Y1 $n_{\rm a}$ $\overline{n}/n_{\rm a}$ $T_1/T_{\rm a}$ Ml N
0.5 10 30 10 4 200 0.440 0.217 0.103 0.049 3.1E67 0.01 1.58 0.64 0.03 1720
1 10 30 10 4 200 0.146 0.054 0.022 0.009 1.6E69 0.07 1.29 0.88 0.19 1720
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E70 0.38 1.16 0.91 0.90 1720
4 10 30 10 4 200 0.069 0.015 0.004 0.001 5.3E71 1.63 1.10 0.93 3.64 1720
8 10 30 10 4 200 0.057 0.010 0.002 0.001 6.8E72 5.93 1.08 0.93 13.0 1720
2 1 30 10 4 200 0.319 0.113 0.040 0.014 5.3E69 0.40 1.35 0.74 0.18 10 700
2 3 30 10 4 200 0.163 0.054 0.019 0.007 1.4E70 0.39 1.23 0.87 0.36 4770
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E70 0.38 1.16 0.91 0.90 1720
2 30 30 10 4 200 0.055 0.011 0.004 0.001 8.4E70 0.38 1.13 0.93 2.36 630
2 100 30 10 4 200 0.029 0.004 0.001 0.000 2.6E71 0.38 1.11 0.94 7.38 200
2 10 3 10 4 200 0.074 0.019 0.006 0.002 5.1E71 5.06 1.10 0.92 1.13 17 200
2 10 10 10 4 200 0.080 0.021 0.007 0.002 1.3E71 1.41 1.12 0.92 1.06 5160
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E70 0.38 1.16 0.91 0.90 1720
2 10 100 10 4 200 0.153 0.051 0.018 0.006 4.0E69 0.06 1.29 0.88 0.56 516
2 10 300 10 4 200 0.528 0.216 0.077 0.027 1.6E68 0.01 1.44 0.65 0.24 172
2 10 30 0.1 4 200 0.006 0.000 0.000 0.000 1.8E71 0.95 1.08 1.00 2.07 1720
2 10 30 0.3 4 200 0.030 0.005 0.001 0.000 6.0E70 0.54 1.10 0.98 1.20 1720
2 10 30 1 4 200 0.060 0.013 0.004 0.001 4.0E70 0.43 1.13 0.95 0.99 1720
2 10 30 3 4 200 0.090 0.024 0.008 0.003 3.3E70 0.38 1.16 0.92 0.90 1720
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E70 0.38 1.16 0.91 0.90 1720
2 6 2 10 4 200 0.096 0.027 0.009 0.003 5.0E71 7.65 1.12 0.91 0.74 40 300
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E70 0.38 1.16 0.91 0.90 1720
2 30 102 10 4 200 0.096 0.026 0.009 0.003 8.7E69 0.06 1.23 0.91 1.38 185
2 10 30 10 4 200 0.096 0.027 0.009 0.003 3.2E69 0.38 1.16 0.91 0.90 1720
2 10 30 10 0 200 0.072 0.018 0.006 0.002 5.4E70 0.52 1.09 0.92 1.16 1720
2 10 30 10 0.8 100 0.089 0.024 0.008 0.003 3.7E70 0.41 1.14 0.91 0.96 215


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