We present a geometric formalism for the non-equilibrium thermodynamics of a small system coupled to external isothermal reservoirs as an application of Thouless pumping, where the electrochemical potentials of the reservoirs and parameters in the system’s Hamiltonian are adiabatically controlled. By analyzing the quantum master equation for the Anderson model of a quantum dot under the wide-band approximation, we obtain the work and effective efficiency of the thermodynamic engine as functions of the phase difference between the externally controlled electrochemical potentials after the system reaches a geometric cyclic state. Since the entropy production is negligible in adiabatic operations, the process we consider is reversible, analogous to the Carnot cycle.

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