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Do vibrationally excited OH molecules affect middle and upper atmospheric chemistry?

机译:振动激发哦分子影响中上部和上部大气化学吗?

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Except for a few reactions involving electronically excited molecular or atomic oxygen or nitrogen, atmospheric chemistry modelling usually assumes that the temperature dependence of reaction rates is characterized by Arrhenius' law involving kinetic temperatures. It is known, however, that in the upper atmosphere the vibrational temperatures may exceed the kinetic temperatures by several hundreds of Kelvins. This excess energy has an impact on the reaction rates. We have used upper atmospheric OH populations and reaction rate coefficients for OH(v=0...9)+O3 and OH(v=0...9)+O to estimate the effective (i.e. population weighted) reaction rates for various atmospheric conditions. We have found that the effective rate coefficient for OH(v=0...9)+O3 can be larger by a factor of up to 1470 than that involving OH in its vibrational ground state only. At altitudes where vibrationally excited states of OH are highly populated, the OH reaction is a minor sink of Ox and O3 compared to other reactions involving, e.g., atomic oxygen. Thus the impact of vibrationally excited OH on the ozone or Ox sink remains small. Among quiescent atmospheres under investigation, the largest while still small (less than 0.1%) effect was found for the polar winter upper stratosphere and mesosphere. The contribution of the reaction of vibrationally excited OH with ozone to the OH sink is largest in the upper polar winter stratosphere (up to 4%), while its effect on the HO2 source is larger in the lower thermosphere (up to 1.5% for polar winter and 2.5% for midlatitude night conditions). For OH(v=0...9)+O the effective rate coefficients are lower by up to 11% than those involving OH in its vibrational ground state. The effects on the odd oxygen sink are negative and can reach ?3% (midlatitudinal nighttime lowermost thermosphere), i.e. neglecting vibrational excitation overestimates the odd oxygen sink. The OH sink is overestimated by up to 10%. After a solar proton event, when upper atmospheric OH can be enhanced by an order of magnitude, the excess relative odd oxygen sink by consideration of vibrational excitation in the reaction of OH(v=0...9)+O3 is estimated at up to 0.2%, and the OH sink by OH(v=0...9)+O can be reduced by 12% in the thermosphere by vibrational excitation.
机译:除了涉及电子激发的分子或原子氧或氮气的少数反应,大气化学建模通常假设反应率的温度依赖性的特征在于Arhenius的涉及动力学温度的法律。然而,已知,在上层大气中,振动温度可能超过几百个开尔林的动力学温度。这种过量的能量对反应率产生影响。我们已经使用了OH(v = 0 ... 9)+ O3和OH(v = 0 ... 9)+ O的上大气oh群体和反应速率系数,以估计各种的有效(即群体加权)反应速率大气条件。我们已经发现OH(v = 0 ... 9)+ O3的有效速率系数可以大于1470的倍数,而不是涉及其振动接地状态。在高度填充的振动激发态的高度,OH反应是与其他涉及的其他反应相比,OH反应是OX和O3的次要水槽。因此,振动激发OH对臭氧或牛水槽的影响仍然很小。在调查的静态气氛中,对于极地冬季平流层和介质层,发现了最大的同时仍然很小(小于0.1%)。耐臭氧到OH水槽的振动激发反应的贡献在上极性冬季平流层中最大(高达4%),而其对HO2源的影响在较低的热层中(极性高达1.5%)冬季和2.5%的中间夜条件)。对于OH(v = 0 ... 9)+℃,有效速率系数低于11%,而不是涉及振动地面状态的速率。对奇数氧气水槽的影响是负的,可以达到?3%(中际夜间最低热圈),即忽略振动激发高估奇数氧气水槽。哦水槽高达10%。在太阳能质子事件之后,当上大气哦可以通过幅度提高时,通过考虑在OH(v = 0 ... 9)+ O3的反应中考虑振动激发的过量相对奇氧气沉积通过振动激励,通过振动激励,在热圈中可以减少12%的0.2%,oh水槽ob(v = 0 ... 9)+ O可以减少12%。

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