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Constraining the N2O5 UV absorption cross section from spectroscopic trace gas measurements in the tropical mid-stratosphere

机译:在热带中层平流层中,通过光谱痕量气体测量来约束N2O5紫外吸收截面

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摘要

The absorption cross section of N2O5, σN2O5(λ, T), which is known from laboratory measurements with the uncertainty of a factor of 2 (Table 4-2 in (Jet Propulsion Laboratory) JPL-2011; the spread in laboratory data, however, points to an uncertainty in the range of 25 to 30%, Sander et al., 2011), was investigated by balloon-borne observations of the relevant trace gases in the tropical mid-stratosphere. The method relies on the observation of the diurnal variation of NO2 by limb scanning DOAS (differential optical absorption spectroscopy) measurements (Weidner et al., 2005; Kritten et al., 2010), supported by detailed photochemical modelling of NOy (NOx(= NO + NO2) + NO3 + 2N2O5 + ClONO2 + HO2NO2 + BrONO2 + HNO3) photochemistry and a non-linear least square fitting of the model result to the NO2 observations. Simulations are initialised with O3 measured by direct sun observations, the NOy partitioning from MIPAS-B (Michelson Interferometer for Passive Atmospheric Sounding – Balloon-borne version) observations in similar air masses at night-time, and all other relevant species from simulations of the SLIMCAT (Single Layer Isentropic Model of Chemistry And Transport) chemical transport model (CTM). Best agreement between the simulated and observed diurnal increase of NO2 is found if the σN2O5(λ, T) is scaled by a factor of 1.6 ± 0.8 in the UV-C (200–260 nm) and by a factor of 0.9 ± 0.26 in the UV-B/A (260–350 nm), compared to current recommendations. As a consequence, at 30 km altitude, the N2O5 lifetime against photolysis becomes a factor of 0.77 shorter at solar zenith angle (SZA) of 30° than using the recommended σN2O5(λ, T), and stays more or less constant at SZAs of 60°. Our scaled N2O5 photolysis frequency slightly reduces the lifetime (0.2–0.6%) of ozone in the tropical mid- and upper stratosphere, but not to an extent to be important for global ozone.
机译:N2O5的吸收截面,σN2O5(λ,T),这是从实验室测量得知的,不确定度为2(喷气推进实验室JPL-2011中的表4-2);但是实验室数据的分布通过对热带平流层中相关痕量气体进行气球观测,研究人员指出,不确定度范围在25%至30%之间(Sander等人,2011)。该方法依赖于通过肢体扫描DOAS(差分光学吸收光谱法)测量来观察NO2的昼夜变化(Weidner等人,2005; Kritten等人,2010),并由NOy(NOx(= NO + NO2)+ NO3 + 2N2O5 + ClONO2 + HO2NO2 + BrONO2 + HNO3)的光化学反应和模型的非线性最小二乘拟合对NO2的观测结果。初始模拟是通过直接阳光观测所测量的O3,来自MIPAS-B(用于大气被动探测的米歇尔森干涉仪–气球传播型)的NOy划分,夜间在类似空气质量中的观测以及所有其他相关物种的模拟而得出的。 SLIMCAT(化学和运输的单层等熵模型)化学运输模型(CTM)。如果σN2O5(λ,T)在UV-C(200-260 nm)中以1.6±0.8的比例缩放,而在UV-C(200–260 nm)中以0.9±0.26的比例缩放,则发现模拟的NO2和观察到的昼夜NO2的增加之间的最佳一致性。与目前的建议相比,UV-B / A(260-350 nm)。结果,在30 km的海拔高度下,抗光解作用的N2O5寿命在太阳天顶角(SZA)为30°时比使用推荐的σN2O5(λ,T)短0.77倍,并且在SZAs保持不变60°。我们按比例缩放的N2O5光解频率会稍微缩短热带中上层和高层平流层中臭氧的寿命(0.2–0.6%),但对全球臭氧的重要性不大。

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