Figure 1

The currents of heat Q̇ and work Ẇ as well as their local and nonlocal components, i.e., \(\dot{W}^{\mathrm{loc}}\), \(\dot{W}^{\mathrm{non}-\mathrm{loc}}\), \(\dot{Q}^{\mathrm{loc}}\) and \(\dot{Q}^{\mathrm{non}-\mathrm{loc}}\), as a function of \(J_{s}^{x}/J_{s}^{y}\) for \(\omega _{S_{1}}=\omega _{S_{2}}=\omega _{R}=3\), \(J_{1}=0.4\), \(J_{2}=1.2\) and \(T_{R}=1\)