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MODEL ANALYSIS OF STRATOSPHERE-TROPOSPHERE EXCHANGE OF OZONE AND ITS ROLE IN THE TROPOSPHERIC OZONE BUDGET

机译:臭氧层层 - 对流层交换的模型分析及其在对流层臭氧预算中的作用

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We have addressed several aspects of STE of ozone and the impact on tropospheric ozone levels. Using ozone observations in the upper troposphere and lower stratosphere from MOZAIC, we have examined the relation between ozone and PV in the lower stratosphere. A distinct seasonality in the ratio between ozone and PV is evident, with a maximum in spring and minimum in fall associated with the seasonality of downward transport in the meridional circulation and of the ozone concentrations in the lower stratosphere. The ozone-PV ratio is applied in our tropospheric chemistry-climate model to improve the boundary conditions for ozone above the tropopause, to improve the representativity of simulated ozone distributions near synoptic disturbances and realistically simulate cross-tropopause ozone transports. It is expected that the results will further improve when the model is applied in a finer horizontal and vertical resolution. In the literature a wide range of estimates regarding the influx of ozone from the stratosphere into the troposphere is presented, derived by many different methods. Some studies report an annual flux between 200-870 Tg O_3 yr~(-1) globally, whereas other studies report a flux between 500 and 1000 Tg O_3 yr~(-1) for the NH only. With our model we estimate for the NH a net downward flux from the stratosphere of 580 Tg O_3 yr~(-1), which is partly balanced by an upward flux of ozone from photochemical production in the troposphere of 210 Tg O_3 yr~(-1), yielding a net downward cross-tropopause ozone transport of 370 Tg O_3 yr~(-1). Globally, these values are 950, 370 and 580 Tg O_3 yr~(-1), respectively. (Note that the troposphere-to-stratosphere ozone flux in the extratropics has only a limited extent since this air does not penetrate the stratosphere above about 100 hPa, the "overworld"). It is evident that different definitions and assumptions may explain part of the range. For example, when upward transport of ozone across the tropopause is not, or only partly, accounted for, the estimated ozone STE flux represents mainly the downward flux and is likely to be in the high end of the range. This may be the case, for example, when global fluxes are extrapolated from the analysis of transports in a single mesoscale event. Also, it should be explicitly stated whether a study separates an upward flux of photochemically produced tropospheric ozone from the downward flux of stratospheric ozone. The results of this study indicate that chemical destruction in the troposphere, however important as a sink for O_3s, does not significantly influence the tropospheric budget of stratospheric ozone. Chemical destruction is only very efficient in a relatively small region well removed from the source region. Therefore, transport in the troposphere is an important factor, so that the representation of the large scale circulation, of synoptic scale events and the mixing of tropospheric and stratospheric air likely add to the range between estimates. Finally we examined the contribution of ozone from the stratosphere on surface ozone levels for pre-industrial, present-day and future atmospheres. Due to relatively low efficiency of photochemical ozone formation in the pre-industrial atmosphere, the seasonality of surface ozone was strongly linked to that of STE except in (sub-)tropical areas, with a clear maximum in winter. In the present-day atmosphere a build-up of anthropogenically emitted ozone precursors takes place at mid-high northern latitudes during winter, so that the winter maximum of ozone of stratospheric origin is followed by a peak in photochemical production in late spring, causing the ozone spring peak observed in NH remote locations. At present, ozone of stratospheric origin appears to contribute about 50% of total surface ozone in winter at mid-high latitudes, and only little during summer. Furthermore, our model simulations suggest that in the next few decades ozone concentrations will increase significantly
机译:我们已经解决了臭氧STE的几个方面,以及对对流层臭氧水平的影响。在莫扎克中,在上层对流层和较低的平流层中使用臭氧观察,我们研究了臭氧与PV在较低平流层之间的关系。臭氧和光伏之间的比例的不同季节性是明显的,春季和最小值最多与子宫内循环中的下行运输季节性相关,并且臭氧浓度在较低平流层中的臭氧浓度相关。臭氧-PV比在我们的对流层化学 - 气候模型中应用,以改善臭氧的边界条件,以提高模拟臭氧分布附近的模拟臭氧紊乱,并现实地模拟交叉对象臭氧输送。预计当模型应用于更精细的水平和垂直分辨率时,结果将进一步改善。在文献中,通过许多不同的方法,提出了关于从平流层进入对流层的臭氧涌入的各种估计值。一些研究报告了200-870 TG O_3 YR〜(-1)之间的年度通量,而其他研究仅报告了NH的500%至1000 TG O_3 YR〜(-1)之间的通量。通过我们的模型,我们估计了来自580 TG O_3 YR〜(-1)的平流层的NH净向下通量,这是由210 TG O_3 YR的对流层的光化学生产中臭氧的向上通量部分平衡〜( - 1),产生净向下交叉对象臭氧输送370 Tg O_3 YR〜(-1)。在全球范围内,这些值分别为950,370和580 TG O_3 YR〜(-1)。 (请注意,卓越层上的对流层 - 平流层臭氧通量只有有限的程度,因为这种空气不会穿透大约100hpa的平流层,“Overworld”)。很明显,不同的定义和假设可以解释该范围的一部分。例如,当对流罗门狗的臭氧向上传输不是部分,估计的臭氧STE助焊剂主要是向下通量表示,并且可能处于该范围的高端。例如,当全局助熔剂从单个Messcale事件中的传输分析推断时,这可能是这种情况。此外,应该明确说明一项研究是否将光学产生的上散液的向上通量从平坦散臭的下流分离。本研究的结果表明,对流层中的化学破坏,然而,作为O_3S的水槽很重要,不会显着影响地流层臭氧的对流层预算。化学破坏在从源区移除的相对较小的区域中仅高效。因此,对流层中的运输是一个重要因素,使得大规模循环的表示,天气尺度事件和对流层和流程层的混合可能增加到估计之间的范围。最后,我们研究了臭氧从平流层对地表臭氧水平的贡献,用于预工业,当天和未来的大气。由于预工业气氛中的光化学臭氧形成的效率相对较低,表面臭氧的季节性与斯特的季节性密切相关,除了(亚)热带地区,冬季最大的最大值。在当前的气氛中,在冬季北部北部纬化地区的人为发射的臭氧前体的积累,使冬季臭氧的冬季最大的臭氧在晚春天的光化学生产中,导致在NH远程位置观察到臭氧弹簧峰。目前,平流层原产地的臭氧似乎在中高纬度的冬季占总表面臭氧的50%,夏季只有很少。此外,我们的模型模拟表明,在接下来的几十年中,臭氧浓度将显着增加

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