Similar to Fig. 10 (same legend) for magnetically related quantities. On the left: Lorentz number corrected for the fraction of Ohmic dissipation as a function of a combination of nondimensional buoyancy power and magnetic Prandtl number. The scaling relations are $Lo{f}_{ohm}^{-1/2}=A{P}^{\frac{1}{3}}P{m}^{\frac{1}{10}}$, where A is 0.9 or 0.7 for dipolar and multipolar dynamos, respectively. Yadav et al. (2013) found that the value $f_{dip,l<12}^{axi,surf}>0.3$ divides the data into dipolar and multipolar, and these two types of runs are best fit separately. On the right: characteristic timescale of the magnetic energy dissipation as a function of Rossby number. The scaling relations are τ_mag,dip = 1.51 Ro^−0.63 and τ_mag,mulip = 0.67 Ro^−0.69.