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3. PROPERTIES OF MICRO-DISCHARGES 3.3. RESULTS 700 sccm 600 sccm 500 sccm 100 80 60 40 20 0 Figure 3.10: Distribution of filaments: Y -axis shows how counts of half cycles with 1, 2 and 3 filaments. Pressure 600 mbar Uappl=15.5 kVpk−pk, Pavg=0.15 W 3.3.4 Charge statistics For a complete understanding of electrical properties of filaments and their effect on CO2 dissociation, charge transported by each filament were done using the method described in section 3.2.2. Also, combined with imaging measurements, charge measurement will explain the origin of difficulty in creating in new filaments – the power law relation observed between filaments and power injected. The average charge transferred by the first filament alone (∆Qf1), second filament alone (∆Qf2) and all the filaments together (∆Qf) in a half cycle are plotted in the figure 3.11. ∆Qf1 remains constant at 0.5 nC irrespective of pressure. ∆Qf2 appears increasing with increase in power and seems to saturate at some higher Pavg while ∆Qf linearly increases with power as shown in figure 3.11. According to Eliasson et al [66] ∆Qf perfilamentshouldbeconstantatallpressures.However,inthisworkonly∆Qf1 remains constant; because of the electrode geometry used, the filament can extend in length and not all filaments are equivalent in this respect. The extension in length will be discussed in section 3.3.5. The error in the charge transferred is not shown in the plots for the sake of clarity. The average standard deviation in charge transferred by same type of filament (∆Qf1 or ∆Qf2) varies from 30% to 50 % which increases with increasing in power just like Navg. Further analysis of error is discussed in appendix 3.B. 56 123 Number of filaments per half cycle CountsPDF Image | Understanding CO2 containing non-equilibrium plasmas
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