Table 3: Average energy per particle dissipated by jets of different power $L_{\rm j}$ in the three clusters characterized by $T_{\rm ew}$ = 0.5, 1, 2 kev. Reported are the average energy per particle dissipated inside the entire domain (first value) and inside the cluster core $R < r_{\rm s}$ (second value) at the end of the simulations.
$L_{\rm j}$ (erg s^-1) $T_{\rm ew}=$ 0.5 keV $T_{\rm ew}=$ 1 keV $T_{\rm ew}=$ 2 keV

10⁴⁶ 1-3.2 keV 0.5-2 keV 0.2-1 keV

$5\times10^{46}$ 4.1-9.7 keV 2.1-5.6 keV 0.9-3.1 keV

**Table 3:** Average energy per particle dissipated by jets of different power $L_{\rm j}$ in the three clusters characterized by $T_{\rm ew}$ = 0.5, 1, 2 kev. Reported are the average energy per particle dissipated inside the entire domain (first value) and inside the cluster core $R < r_{\rm s}$ (second value) at the end of the simulations.
$L_{\rm j}$ (erg s^-1)	$T_{\rm ew}=$ 0.5 keV	$T_{\rm ew}=$ 1 keV	$T_{\rm ew}=$ 2 keV
10⁴⁶	1-3.2 keV	0.5-2 keV	0.2-1 keV
$5\times10^{46}$	4.1-9.7 keV	2.1-5.6 keV	0.9-3.1 keV

Source LaTeX | All tables | In the text

	1 Introduction
	2 The baseline model
	3 The simulations
	4 The energy balance
	5 Entropy evolution
	6 Hydrostatic equilibrium
	7 Tests on numerical resolution and jet parameters
	8 Discussion and conclusions
	References