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Figure 6a_Space resolved black body emission amplitude 60 slm, 4% CH4, 900 W
Resources
- Figure 2_Uncalibrated overview spectrum
- Figure 3_Radially resolved amplitudes and temperatures
- Figure 4a_Space resolved gas temperature 60 slm, 4% CH4, 900 W
- Figure 4b_Space resolved gas temperature 60 slm, 4% CH4, 1800 W
- Figure 4c_Space resolved gas temperature 60 slm, 8% CH4, 1800 W
- Figure 4d_Space resolved gas temperature 80 slm, 4% CH4, 1200 W
- Figure 5a_Space resolved dicarbon Swan Bands emission amplitude 60 slm, 4% CH4, 900 W
- Figure 5b_Space resolved dicarbon Swan Bands emission amplitude 60 slm, 4% CH4, 1800 W
- Figure 5c_Space resolved dicarbon Swan Bands emission amplitude 60 slm, 8% CH4, 1800 W
- Figure 5d_Space resolved dicarbon Swan Bands emission amplitude 80 slm, 4% CH4, 1200 W
- Figure 6a_Space resolved black body emission amplitude 60 slm, 4% CH4, 900 W
- Figure 6b_Space resolved black body emission amplitude 60 slm, 4% CH4, 1800 W
- Figure 6c_Space resolved black body emission amplitude 60 slm, 8% CH4, 1800 W
- Figure 6d_Space resolved black body emission amplitude 80 slm, 4% CH4, 1200 W
- Figure 7_Thermal equilibrium mole fractions
- Figure 8a_Methane Pyrolysis Kinetics at 1400 K
- Figure 8b_Methane Pyrolysis Kinetics at 2100 K
- Figure 8c_Methane Pyrolysis Kinetics at 3600 K
- Figure C1a_Simulated dicarbon Swan bands Delta v=2
- Figure C1b_Simulated dicarbon Swan bands Delta v=1
- Figure C1c_Simulated dicarbon Swan bands Delta v=0
- Figure C1d_Simulated dicarbon Swan bands Delta v=-1
- Figure C1e_Simulated dicarbon Swan bands Delta v=-2
- Figure C2_NMSSE between two simulated spectra as a function of the rotational temperature
- Figure C3a_NMSSE between two simulated spectra as a function of the rotational temperature and the full width at half maximum Delta v=2
- Figure C3b_NMSSE between two simulated spectra as a function of the rotational temperature and the full width at half maximum Delta v=1
- Figure C3c_NMSSE between two simulated spectra as a function of the rotational temperature and the full width at half maximum Delta v=0
- Figure C3d_NMSSE between two simulated spectra as a function of the rotational temperature and the full width at half maximum Delta v=-1
- Figure C3e_NMSSE between two simulated spectra as a function of the rotational temperature and the full width at half maximum Delta v=-2
- Figure C4a_NMSSE between two simulated spectra as a function of the rotational and vibrational temperatures Delta v=2
- Figure C4b_NMSSE between two simulated spectra as a function of the rotational and vibrational temperatures Delta v=1
- Figure C4b_NMSSE between two simulated spectra as a function of the rotational and vibrational temperatures Delta v=0
- Figure C4d_NMSSE between two simulated spectra as a function of the rotational and vibrational temperatures Delta v=-1
- Figure C4d_NMSSE between two simulated spectra as a function of the rotational and vibrational temperatures Delta v=-2
- Figure C5_Boltzmann plot
Additional Information
Field | Value |
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mimetype | text/plain |
filesize | 5.65 KB |
resource type | file upload |
timestamp | Jun 10, 2025 |