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首页> 外文期刊>Journal of Geophysical Research, D. Atmospheres: JGR >Seasonal cycles of Stratospheric Aerosol and GasExperiment H near-background aerosol in the lowerstratosphere
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Seasonal cycles of Stratospheric Aerosol and GasExperiment H near-background aerosol in the lowerstratosphere

机译:平流层下层平流层气溶胶和Gas的季节周期H背景气溶胶

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Extinction data from the Stratospheric Aerosol and Gas Experiment (SAGE) II in thelower stratosphere were analyzed for seasonal cycles in the near-background levels ofstratospheric aerosol. The data analyzed were the extinction coefficient at 0.525 tm ((30.525)and the extinction ratio at 0.525 um (E0.525) on the basis of climatological zonal monthlymean for the years 1998-2004. Distinct seasonal cycles were found for 00.525 at 35-15°Sabove 28 km (region A) and at 20°S-30°N from 16 to 20.5 km (region B). In the A region,the seasonal cycle of E0.525 was characterized by a maximum in local fall and can beexplained by the ascent of mean meridional circulation in local summer and descent in localwinter. In the B region, the seasonal cycles of E0.525 were characterized by a maximum inOctober-January, which can be interpreted by meridional transport and mixing. Theamplitude of the seasonal cycles for E0.525 exhibited asymmetry between the NorthernHemisphere (NH) and the Southern Hemisphere (SH); the amplitudes at latitudes of 20-30° were larger in the SH than in the NH above 29 km, whereas they were larger in the NHthan in the SH below 18 km. Comparison of the distribution of E0.525 with that of SAGE IIwater vapor suggested that the E0.525 distribution is controlled by the stratosphericcirculation and troposphere-originated gases. One difference between E0.525 and watervapor was found in the E0.525 maximum that appears over the winter subtropics. The E0.525maximum can be attributed to the dominance of temperature and microphysical effectscompared to transport effects, whereas the water vapor distribution can be attributed totransport effects. Another difference is that an upward propagation of the seasonalcycle of 4.525 at 5°S-30°N disappeared near 23 km. This difference is explained bythe fact that the chemical and microphysical processes of aerosol formation becomesignificant above 23 km.
机译:分析了平流层下部低层平流层气溶胶和气体实验(SAGE)II的消光数据,以了解平流层气溶胶在接近本底水平的季节周期。根据1998-2004年气候带区月平均数,所分析的数据为0.525 tm的消光系数((30.525)和0.525 um的消光比(E0.525)。在35-在28公里(A区)上方15°,在20°S-30°N(16至20.5 km(B区))。在A区,E0.525的季节周期特征是局部秋季最大,并且在B区,E0.525的季节周期以10月至1月的最大值为特征,这可以通过子午线的运输和混合来解释。 E0.525的季节性周期在北半球(NH)和南半球(SH)之间表现出不对称性; SH上纬度20-30°的振幅大于NH在29 km以上,而在北半球的振幅更大。 18 km以下南半球的NHthan E0分布的比较.525与SAGE II的水蒸气的关系表明,E0.525的分布受平流层循环和对流层起源的气体控制。 E0.525和水蒸气之间的差异是在整个冬季亚热带地区出现的E0.525最大值中发现的。最大E0.525可以归因于温度的优势和与运输效应相比的微观物理效应,而水蒸气分布可以归因于运输效应。另一个区别是,在5°S-30°N下4.525的季节性周期的向上传播在23 km附近消失了。这种差异可以通过以下事实解释:在23 km以上,气溶胶形成的化学和微物理过程变得非常重要。

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