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Figure 6.17: Plasma/monolith temperature results from SPECAIR simulations. Re- sults presented for CO2 flow rates 1-8 slm, Ar flow rate 10 slm, and power from 1-2 kW. monolith is inserted into the discharge tube for every operating condition with a change in CO2 flow rate. Again it is assumed that Ar flow rate has no effect on CO2 conversion. 6.2.2.1 Plasma/Catalyst Efficiencies The results for energy efficiency in the plasma/catalyst system are shown in Figure 6.18. The same trend of η ∝ 1/Ev is evident in the results. However the energy efficiency experiences an even larger drop with the addition of Rh catalyst. Here ηmax = 6%, half the energy efficiency for the same operating condition in the pure plasma system, and lower still than the plasma/monolith system. Likewise, the lowest value of η reaches about 2-2.5%, unlike the pure plasma system with η = 5%. Figure 6.19 displays results for conversion efficiency. As expected based on the energy efficiency results, the conversion efficiency is lower than the pure plasma system. Maximum conversion reaches 20% while the pure plasma system reached about 45% for the same operating condition. For the lowest value of specific energy tested at 8 slm CO2, the conversion rate drops to 8%, which is about half the value achieved in 128PDF Image | CO2 Conversion in a Microwave Plasma Catalyst System
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