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the experimental work are given in Section 7.1 and conclusions for the computational work are presented in Section 7.2. Section 7.3 describes the conclusions gained from the cost analysis of the microwave system, and lastly, suggestions for future work to proceed further in this research area will be offered in Section 7.4. 7.1 Experimental Conclusions 7.1.1 Development of Atmospheric Pressure Microwave Plasma Source The experimental system was designed to meet the requirements of efficient CO2 dissociation: a non-thermal discharge with Te > Tv > Tg. The system was also designed with large-scale operation in mind to perform at atmospheric pressure, eliminating the operational and maintenance costs of a vacuum pump. Based on a review of the available literature, the microwave-excited surface wave plasma system was chosen for its ability to produce non-thermal and high electron density plasmas while operating at atmospheric pressure. Actual operation of the 2-kW microwave plasma requires external ignition when operating at atmospheric pressure because the applied electric field at 2 kW of input power is not capable of exceeding the necessary breakdown voltage for plasma ignition to occur. Typically, the external ignition source is in the form of a high voltage spark across the discharge tube generated by a Tesla coil. Additionally, the discharge tube requires a cooling mechanism to protect against melting due to high gas temperatures in the plasma. Mass spectrometry and optical emission spectroscopy are the main diagnostic tools implemented in the experimental setup, providing information on species and plasma temperature characterization, respectively. 153PDF Image | CO2 Conversion in a Microwave Plasma Catalyst System
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