study on evacuated tube solar collector using supercritical CO2

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study on evacuated tube solar collector using supercritical CO2 ( study-evacuated-tube-solar-collector-using-supercritical-co2 )

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1228 X.R. Zhang, H. Yamaguchi / Applied Thermal Engineering 28 (2008) 1225–1233 1.0 0.8 0.6 0.4 0.2 0.0 5:00 7:00 9:00 11:00 Time 15:00 35 30 25 20 15 10 5 0 17:00 19:00 Solar radiation Air temperature Fig. 3. Variations in the solar radiation and atmosphere temperature measured with time. 13:00 and flow rate of 0.03 kg/s, respectively. A Coriolis effect mass flow meter (CT9401-KIMM30) is used to monitor and record the mass flow of liquid CO2, which also has a maximum permissible operating pressure of 12 MPa. The flow meter is installed in the downstream side of the CO2 feed pump, as shown in Fig. 1. It provides a measurement range of 0.09–2.0 kg/min with an accuracy of ±0.1%. Five T-type thermocouples and five pressure transmit- ters are mounted at different positions in the CO2 flow to measure its temperatures and pressures, with an accuracy of ±0.1 °C for temperature measurements and ±0.2% for pressure measurements. The measuring points of these sen- sors are also shown in Fig. 1. The heat exchanging compo- nents are intended to dissipate heat from the CO2 loop, and cool CO2 to temperature low enough becoming liquid state to be pumped back into the collector. There are simulta- neous high-temperature heat exchanger (heat exchanger 1) and low-temperature heat exchanger (heat exchanger 2) installed in the CO2 loop in order to achieve CO2 liquid state at the inlet of the CO2 feed pump. In the present study, higher-temperature water (hot water) and lower- temperature water (cold water) are, respectively supplied to the heat exchangers 1 and 2 (CO2/water heat exchanger) to dissipate heat from the CO2 loop in the experimental set- up, as shown in Fig. 1. A mechanical-draft water cooling tower (CTA-5 NE) is used as a heat sink, dissipating heat collected from the CO2 cycle to the ambient. In order to achieve a good heat exchange between CO2 and water, shell 200 150 100 50 0.0 0.2 200 150 100 50 0 9:00 11:00 0.4 0.6 I (kW/m2) 0.8 1.0 Measured data Polynomial fit curve (T =51.6+282.3I-151.5I2) 1 Solar collector inlet Solar collector outlet 13:00 15:00 Time 17:00 Fig. 4. Variations in the CO2 temperature measured with the solar radiation (a) and with the time (b). 10 9 8 7 6 5 0.0 10 8 6 4 2 0 9:00 0.2 0.4 0.6 I (kW/m2) 0.8 1.0 Measured data Polynomial fit curve 2 (P =4.3+10.4I-5.6I ) 1 11:00 13:00 Time 15:00 17:00 Fig. 5. Variations in the CO2 pressure measured with the solar radiation (a) and with the time (b). Temperature (°C) T1 (°C) Pressure (MPa) P (MPa) 1 Solar radiation (kW m2) Air temperature (°C)

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