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NCN quantitative measurement in a laminar low pressure flame

机译:NCN在层层低压火焰中定量测量

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The present work has been performed to quantitatively determine the NCN radical concentration profile in a laminar low-pressure CH_4/O_2/N_2 (Φ = 1.25) flame. Laser induced fluorescence (LIF) technique has been implemented in order to record a NCN spectrum in the 326.7-330.1 nm range in flame conditions, and secondly to measure the spatially resolved NCN profile in the flame by exciting the main congested branch of NCN around 329.13 nm. The LIF profile has been calibrated into absorbance using cavity ring-down spectroscopy (CRDS). The calibration into absolute concentration has been done by using the PGOPHER spectral simulation program. The experimental and the simulated NCN spectra were found to be in very good agreement. It has allowed reconsidering the exact assignment of the transitions involved in the strong bandhead at flame temperature, which actually originate from the contribution of both the origin (000) band and the (010∑~+) component of the (010) band contrary to ambient temperature where only the (000) band contribution is significant around 329.13 nm. Thanks to the simulation and using electronic transition dipole moments extracted from available NCN fluorescence lifetimes, we provide a direct determination of the absorption cross-section: σ(λ = 329.13 nm) = (9.4 ± 1.8) × 10~(-17) cm~2/molecule at 1830 K. This cross-section was found constant within ±15% in the 1500-1900 K temperature range. Its determination is very important for research groups concerned with NCN chemistry at high temperature and prompt-NO formation. From that cross-section the peak mole fraction of the NCN radical has been determined to be equal to 170 ± 90 ppb in the low-pressure flame. The experimental uncertainty is mainly linked to the CRDS measurement conditions close to the detection limit and should be reduced in flame conditions yielding higher NCN concentration.
机译:已经进行了本作的工作以定量地确定层状低压CH_4 / O_2 / N_2(φ= 1.25)火焰中的NCN自由基浓度曲线。已经实现了激光诱导的荧光(LIF)技术,以便在火焰条件下记录326.7-330.1nm范围内的NCN光谱,其次是通过激发大约329.13的NCN的主要拥挤分支来测量火焰中的空间分辨的NCN轮廓纳米。使用腔响距光谱(CRD)校准LIF型材以吸光度校准。通过使用PGopher光谱仿真程序已经完成了绝对浓度的校准。发现实验和模拟的NCN光谱非常良好。它允许重新考虑火焰温度下涉及强频带中涉及的过渡的精确分配,其实际上源自(010)频带的原点(010)频带和(010σ〜+)组件的贡献相反环境温度只有(000)带贡献大约329.13 nm。由于仿真和使用从可用的NCN荧光寿命提取的电子转换偶极矩,我们提供了对吸收横截面的直接测定:σ(λ= 329.13nm)=(9.4±1.8)×10〜(-17)cm在1830K时〜2 /分子。发现该横截面恒定在1500-1900k温度范围内的±15%内。它的测定对于在高温下与NCN化学有关的研究组非常重要,并且不及时 - 不形成。从该横截面,NCN自由基的峰值摩尔分数已经确定在低压火焰中等于170±90ppb。实验性不确定性主要与接近检测极限的CRD测量条件相关,并且在火焰条件下应降低,产生更高的NCN浓度。

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