“…In essence, TE generation requires a sufficient temperature difference, ∆T, between hot and cold surfaces of TEGs to induce an electromotive force (EMF), and a high ∆T leads to a high EMF, which is attributed to EMF is the sum of the product of the relative Seebeck coefficient and the temperature difference for all p-type and n-type TE elements connected in serial [9], moreover, we had clarified that the homogeneous heat flux throughout a TEG is indispensable to enhance TE performance that is due to the geometry-dependent thermal diffusion becomes uniform [10,11]. Thus as a result, a pair of counter-flowing hot and cold fluids, as shown in Figure 1 (a), should give rise to a better TE conversion on module, where a high ∆T can be facilitated by the hot fluid, and a homogeneous heat flux can be obtained when the hot fluid is cooled and the cold fluid is heated at the same time by exchanging the heat through the conduction of solid TE module in the process of the thermal fluids flow in the opposite, as depicted in Figure 1 This study continued to model a three-dimension (3D) TE module whose surfaces are covered by the counter-flowing hot and cold fluids, and conducted a numerical simulation using finite-volume method in a commercial software environment, Fluent, to clarify the change of module performance with the flow rate of thermal fluids, where fluid dynamics and TE conversion are carried out synchronously, and then the effects of temperature difference and flow rate on TE performance are compared, which illuminates that the regulation of flow rate should be more effective in improving performance of TE module.…”