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For the 3% O2 case, the model overpredicted the flame liftoff height.
As flow rate decreased from a lifted flame, liftoff height decreases nonlinearly and the flame reattached to a nozzle at a certain liftoff height.
The liftoff height also increases as the jet velocity is increased.
These interactions cause a liftoff height difference between the two flames.
Liftoff height and velocity measurements are presented for turbulent, lifted methane and ethylene flames.
In the case with tribrachial edge structure, the liftoff height increased nonlinearly with jet velocity.
Similar(13)
The liftoff heights were also correlated as a function of jet velocity times the square of ignition delay time.
The predictions are validated through a comparison of the flame reaction zone topologies, liftoff heights, lengths, and oscillation frequencies.
Measurements are reported for flame geometry (liftoff heights and flame heights), flame radiant fractions, and emission indices for oxides of nitrogen (EINOx).
The effect of thermal radiation is to slightly decrease the liftoff heights of both 1-g and μ-g flames under coflow conditions.
The liftoff heights obtained with co-flow gases diluted by CO2 were greater than those obtained when diluting with N2 due to both thermal and chemical dilution effects.
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