Concentrated Solar Thermoelectric Conversion

Partner: external pageSolid State Chemistry, EMPA Dübendorf

Background: 

A thermoelectric converter (TEC) comprises p-type and n-type semiconductor legs sandwiched between two ceramic hot/cold plates and connected thermally in parallel and electrically in series as depicted in Fig. 1. The temperature gradient across the legs induces a voltage difference due to the Seebeck effect. The TEC performance is characterized by its figure-of-merit, ZT=S2T/(ρκ), where S is the Seebeck coefficient, ρ is the electrical resistivity and κ is the thermal conductivity. Due to the relatively low heat-to-electricity conversion efficiencies approaching 5% for ZT = 1, TECs have been mainly used in space applications. With the advent of novel functional ceramic materials, new high-temperature application areas are being considered, e.g. solar electricity generation. The new approach is to drive the TEC modules/arrays with concentrated solar radiation to obtain large temperature differences ΔT across the plates and, consequently, increases the energy conversion efficiency.

Principle of a TEC module
Fig. 1: Principle of a TEC module

A FV-based heat transfer model of a TEC module is developed for simulating its thermal performance and analyzing the effect of the geometrical parameters. Coupled radiation/conduction/convection heat transfer with electrical potential distribution is considered for a TEC module directly exposed to concentrated solar radiation. The model is experimentally validated with measurements of temperature and voltages/power using a set of simplified 4-leg TEC modules that were directly irradiated. Figure 2 depicts the experimental setup at ETH's High Flux Solar Simulator.

Schematic of the experimental setup at ETH's High Flux Solar Simulator. (a) the TEC module is placed at HFSS's focal plane; incident solar radiative fluxes measured by a thermogage (F). (b) position of type-K thermocouples (T) used to measure temperatures of the plates and of the hot end, middle, and cold end of the legs; terminals (V) provided at the cold ends for measuring the voltage/power output of the module. The cold plate was attached to a water-circuit cooler (denoted by screw fixation).
Fig. 2: Schematic of the experimental setup at ETH's High Flux Solar Simulator. (a) the TEC module is placed at HFSS's focal plane; incident solar radiative fluxes measured by a thermogage (F). (b) position of type-K thermocouples (T) used to measure temperatures of the plates and of the hot end, middle, and cold end of the legs; terminals (V) provided at the cold ends for measuring the voltage/power output of the module. The cold plate was attached to a water-circuit cooler (denoted by screw fixation).

Main research topics: 

  • Characterization of the radiation properties of the TEC components
  • Heat transfer analysis and geometrical optimization of a single TEC module
  • Design of a solar cavity-receiver packed with an array of TEC modules ("stack")
  • Optimization for maximum solar-to-electricity energy conversion efficiency
  • Conversion of waste heat, with focus on geothermal and solar waste heat

Project-related Publications

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