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Nitric oxide density measurements in air and air/fuel nanosecond pulse discharges by laser induced fluorescence
173
Citations
62
References
2009
Year
EngineeringAtomic Emission SpectroscopyAtmospheric PhotochemistryGlow DischargeDensity MeasurementsAbsorption SpectroscopyDecay RateChemistryChemical EngineeringOptical DiagnosticsAir Plasma KineticsPhysicsElectronic States N2Laser PhotochemistryNatural SciencesSpectroscopyLaser-induced BreakdownApplied PhysicsGas Discharge PlasmaAtomic Fluorescence Spectroscopy
Laser induced fluorescence is used to measure absolute nitric oxide concentrations in air, methane–air and ethylene–air non-equilibrium plasmas, as a function of time after initiation of a single pulse, 20 kV peak voltage, 25 ns pulse duration discharge. A mixture of NO and nitrogen with known composition (4.18 ppm NO) is used for calibration. Peak NO density in air at 60 Torr, after a single pulse, is ~8 × 1012 cm−3 (~4.14 ppm) occurring at ~250 µs after the pulse, with decay time of ~16.5 ms. Peak NO atom mole fraction in a methane–air mixture with equivalence ratio of = 0.5 is found to be approximately equal to that in air, with approximately the same rise and decay rate. In an ethylene–air mixture (also with equivalence ratio of = 0.5), the rise and decay times are comparable to air and methane–air, but the peak NO concentration is reduced by a factor of approximately 2.5. Spontaneous emission measurements show that excited electronic states N2(C 3Π) and NO(A 2Σ) in air at P = 60 Torr decay within ~20 ns and ~1 µs, respectively. Kinetic modelling calculations incorporating air plasma kinetics complemented with the GRI Mech 3.0 hydrocarbon oxidation mechanism are compared with the experimental data using three different NO production mechanisms. It is found that NO concentration rise after the discharge pulse is much faster than predicted by Zel'dovich mechanism reactions, by two orders of magnitude, but much slower compared with reactions of electronically excited nitrogen atoms and molecules, also by two orders of magnitude. It is concluded that processes involving long lifetime (~100 µs) metastable states, such as N2(X 1Σ,v) and O2(b 1Σ), formed by quenching of the metastable N2(A 3Σ) state by ground electronic state O2, may play a dominant role in NO formation. NO decay, in all cases, is found to be dominated by the reverse Zel'dovich reaction, NO + O → N + O2, as well as by conversion into NO2 in a reaction of NO with ozone.
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