“…T hw = x and T cw = ȳ are known as internal working temperatures, and they define heat fluxes Qh = J h (from the internal heat deposit at temperature x to the system) and Qc = J c (from the system to the internal heat deposit at temperature ȳ). Hence, we use x, ȳ, Jh and Jc to specify temperatures and heat fluxes in a steady state [16,17,18,19,20,29,30]. As the endoreversibility hypothesis implies the internal entropy production is null [5,6,7,8,9,10], then:…”