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Interannual variation patterns of total ozone and lower stratospheric temperature in observations and model simulations

机译:观测和模型模拟中总臭氧和平流层较低温度的年际变化规律

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We report results from a multiple linear regression analysis oflong-term total ozone observations (1979 to 2000, by TOMS/SBUV), of temperaturereanalyses (1958 to 2000, NCEP), and of two chemistry-climate model simulations(1960 to 1999, by ECHAM4.L39(DLR)/CHEM (=E39/C), and MAECHAM4-CHEM). The model runs are transientexperiments, where observed sea surface temperatures, increasing source gasconcentrations (CO2, CFCs, CH4, N2O, NOx), 11-year solar cycle,volcanic aerosols and the quasi-biennial oscillation (QBO) are all accountedfor. MAECHAM4-CHEM covers the atmosphere from the surface up to 0.01 hPa (≈80 km).For a proper representation of middle atmosphere (MA) dynamics, itincludes a parametrization for momentum deposition by dissipating gravity wavespectra. E39/C, on the other hand, has its top layer centered at 10 hPa(≈30 km). It is targeted on processes near the tropopause, and has morelevels in this region. Despite some problems, both models generally reproduce the observed amplitudes and much ofthe observed low-latitude patterns of the various modes of interannual variability intotal ozone and lower stratospherictemperature. In most aspects MAECHAM4-CHEM performs slightly better than E39/C.MAECHAM4-CHEM overestimates the long-term decline of total ozone, whereas underestimates the decline over Antarctica and at northern mid-latitudes. Thetrue long-term decline in winter and spring above the Arctic may be underestimatedby a lack of TOMS/SBUV observations in winter, particularly in the cold 1990s.Main contributions to the observed interannualvariations of total ozone and lower stratospheric temperature at 50 hPa comefrom a linear trend (up to -10 DU/decade at high northern latitudes, up to -40 DU/decadeat high southern latitudes, and around -0.7 K/decade over much of the globe),from the intensity of the polar vortices (more than 40 DU, or 8 K peak to peak),the QBO (up to 20 DU, or 2 K peak to peak), and from tropospheric weather (upto 20 DU, or 2 K peak to peak). Smaller variations are related to the 11-yearsolar cycle (generally less than 15 DU, or 1 K), or to ENSO (up to 10 DU, or1 K). These observed variations are replicated well in the simulations.Volcanic eruptions have resulted in sporadic changes (up to -30 DU, or+3 K). At low latitudes, patterns are zonally symmetric.At higher latitudes, however, strong, zonally non-symmetric signals are foundclose to the Aleutian Islands or south of Australia. Such asymmetric featuresappear in the model runs as well, but often at different longitudes than in theobservations. The results point to a key role of the zonally asymmetric Aleutian(or Australian) stratospheric anti-cyclones for interannual variations athigh-latitudes, and for coupling between polar vortex strength, QBO, 11-year solarcycle and ENSO.
机译:我们报告了对长期总臭氧观测值(1979年至2000年,通过TOMS / SBUV),温度再分析(1958年至2000年,NCEP)以及两个化学-气候模型模拟(1960年至1999年)的多元线性回归分析结果, ECHAM4.L39(DLR)/ CHEM(= E39 / C)和MAECHAM4-CHEM)。该模型运行是瞬态实验,其中观察到的海面温度,源气浓度增加(CO 2 , CFC s,CH 4 ,N 2 O,NO x ),11年太阳周期,火山气溶胶和准两年一次振荡(QBO)均被考虑在内。 MAECHAM4-CHEM覆盖从地面到0.01 hPa(≈80km)的大气。为了正确表示中间大气(MA)动力学,它包括通过耗散重力波谱进行动量沉积的参数化。另一方面,E39 / C的顶层位于10 hPa(≈30km)的中心。它以对流层顶附近的过程为目标,并且在该区域具有更高的水平。尽管存在一些问题,但这两个模型通常会重现观测到的振幅和许多观测到的低纬度模式,这些模式是臭氧和平流层温度较低的年际变化的各种模式。在大多数方面,MAECHAM4-CHEM的性能略优于E39 /C。MAECHAM4-CHEM高估了总臭氧的长期下降,而低估了南极和北中纬度地区的臭氧下降。由于缺乏冬季的TOMS / SBUV观测值,特别是在1990年代寒冷的冬季,北极和北部冬季和春季的真正长期下降可能被低估了。在50 hPa时观测到的总臭氧和平流层较低温度的年际变化的主要贡献来自线性趋势(极地涡流的强度)(超过40个)在北高纬度地区达-10 DU / decade,在南高纬度地区达-40 DU / decade,在全球大部分地区约为-0.7 K / decade。 DU(或8 K峰至峰),QBO(最高20 DU,或2 K峰至峰),以及对流层天气(最高20 DU,或2 K峰至峰)。较小的变化与11年的太阳周期(通常小于15 DU或1 K)或ENSO(最大10 DU或1 K)有关。这些观测到的变化在模拟中得到了很好的再现。火山喷发导致了零星的变化(高达-30 DU或+3 K)。在低纬度地区,模式呈区域对称性;在高纬度地区,靠近阿留申群岛或澳大利亚南部发现强的,区域性非对称信号。这种不对称特征也出现在模型中,但通常与观察中的经度不同。结果表明,纬向不对称的阿留申(或澳大利亚)平流层反气旋对于高纬度的年际变化以及极涡强度,QBO,11年太阳周期和ENSO之间的耦合起着关键作用。

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