Abstract

The correct calculation of the vertical velocity of the Asian Summer Monsoon anticyclone (ASMA) region is helpful to know more accurately the ozone stratosphere-troposphere exchange, so as to explore the variation of ozone in the ASMA region. Therefore, the vertical velocity over the ASMA in June, July, August and September 2012 and 2016 is calculated by the thermodynamic method, which may avoid the deviations from the kinematics method using the mass continuity equation. In order to improve the accuracy, we used high-resolution heating rate datasets obtained via the Beijing Climate Center Radiation Transfer Model based on in situ observations and revised satellite data from MLS/AIRS. The vertical velocity calculated by the thermodynamic method (VT) is then compared with the data from ERA-Interim (VERA-I). In the daytime, values of VT were similar to VERA-I, and were dominated by ascending motion, although VT showed descending motion at the western edge of the ASMA below 100 hPa. The intensity of VT was slightly smaller than that of VERA-I at lower levels (200 hPa –100 hPa) over the ASMA region and significantly weaker above 100 hPa. In the night-time, situation was more complex. Both VT and VERA-I showed the convergence of vertical wind at 150 hPa, and the divergence at 80 hPa, but VT had a smaller standard deviation. Besides, VT showed descending in the western and northern ASMA, but VERA-I only descended in the west. The descending motion in the west, seen in both VT and VERA-I, is produced by the heating difference between Qinghai-Tibet Plateau and Iranian Plateau. The difference of the two vertical velocities in the northern ASMA may indicate the different understandings of the local Hadley Circulation and local Brewer-Dobson Circulation.

Highlights

  • About ∼99% of all weather phenomena occur in the troposphere, but the stratosphere, which accounts for ∼15% of the total mass of the Earth’s atmosphere, has an important role in atmospheric studies (Holton, 1990; Dessler and Sherwood, 2004; Aschmann et al, 2009; Bian, 2009; Randel and Jensen, 2013; Zhang et al, 2016)

  • Substituting three different heating rates into Eq 10, we calculated the average vertical velocity profiles for Ali station in JJAS (VAli), the daily vertical velocity data of the atmospheric infrared sounder (AIRS) (VAIRS), and the monthly average vertical velocity of the microwave limb sounder (MLS) (VMLS). We compared these results with the vertical velocity in the ERA-Interim (VERA−I) dataset, which had been interpolated at the same spatiotemporal resolution

  • We established a method based on the thermodynamic equation and introduced heating rate data obtained from in situ observations and revised satellite data from MLS/AIRS to determine the vertical velocity in JJAS 2012 and 2106

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Summary

Introduction

About ∼99% of all weather phenomena occur in the troposphere, but the stratosphere, which accounts for ∼15% of the total mass of the Earth’s atmosphere, has an important role in atmospheric studies (Holton, 1990; Dessler and Sherwood, 2004; Aschmann et al, 2009; Bian, 2009; Randel and Jensen, 2013; Zhang et al, 2016). Ozone is mainly present in the ozone layer, about 20 km above the Earth’s surface in the stratosphere (Lv et al, 2009; London and Park, 2011; Newman, 2014). Research on stratosphere–troposphere exchange is important in studying stratospheric ozone evolution (Liu et al, 2003; Tian et al, 2008; Bian et al, 2011a, 2020; Guo et al, 2012, 2015, 2017; Xie et al, 2012; Pavlov et al, 2013; Zhang H. et al, 2014; Gerber, 2015; Zhang J. et al, 2018). Previous studies have determined the structural distribution, vertical transport, and dynamics (Antokhin and Belan, 2013) of ozone in the stratosphere via LiDAR measurements (Kuang et al, 2012; Pavlov et al, 2013) the inversion of occultation data (Sofieva et al, 2017) and numerical simulations (Yang et al, 2004; Considine et al, 2008)

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