OH radical kinetics in hydrogen-air mixtures at the conditions of strong vibrational nonequilibrium. (27th November 2017)

• Record Type: Journal Article
• Authors: Winters, Caroline; Hung, Yi-Chen; Jans, Elijah; Eckert, Zak; Frederickson, Kraig; Adamovich, Igor V; Popov, Nikolay
• Is Part Of: Journal of physics. Volume 50:Number 50(2017)
• Publication Date: 2017-11-27
• Subjects: ns pulse discharge -- plasma assisted combustion -- radical kinetics -- vibrational nonequilibrium; Physics -- Periodicals; 530
• DOI: 10.1088/1361-6463/aa97b4
• Languages: English
• ISSNs: 0022-3727

Abstract

Abstract: This work presents results of time-resolved, absolute measurements of OH number density, nitrogen vibrational temperature, and translational-rotational temperature in air and lean hydrogen-air mixtures excited by a diffuse filament nanosecond pulse discharge, at a pressure of 100 Torr and high specific energy loading. The main objective of these measurements is to study kinetics of OH radicals at the conditions of strong vibrational excitation of nitrogen, below autoignition temperature. N2 vibrational temperature and gas temperature in the discharge and the afterglow are measured by ns broadband coherent anti-Stokes Raman scattering. Hydroxyl radical number density is measured by laser induced fluorescence, calibrated by Rayleigh scattering. The results show that the discharge generates strong vibrational nonequilibrium in air and H2 -air mixtures for delay times after the discharge pulse of up to ~1 ms, with a peak vibrational temperature of T v ≈ 1900 K at T ≈ 500 K. Nitrogen vibrational temperature peaks at 100–200 µ s after the discharge pulse, before decreasing due to vibrational-translational relaxation by O atoms (on the time scale of several hundred µ s) and diffusion (on ms time scale). OH number density increases gradually after the discharge pulse, peaking at t ~ 100–300 µ s and decaying on a longer time scale, until t ~ 1 ms. Both OH rise time and decay time decrease as H2 fraction in the mixture is increased from 1% to 5%. Comparison of the experimental data with kinetic modeling predictions shows that OH kinetics is controlled primarily by reactions of H2 and O2 with O and H atoms generated during the discharge. At the present conditions, OH number density is not affected by N2 vibrational excitation directly, i.e. via vibrational energy transfer to HO2 . The effect of a reaction between vibrationally excited H2 and O atoms on OH kinetics is also shown to be insignificant. As the discharge pulse coupled energy is increased, the model predicts transient OH number density overshoot due to the temperature rise caused by N2 vibrational relaxation by O atoms, which may well be a dominant effect in discharges with specific energy loading.