首页> 外文期刊>Journal of Geophysical Research. Biogeosciences >AN ATMOSPHERIC TAPE RECORDER - THE IMPRINT OF TROPICAL TROPOPAUSE TEMPERATURES ON STRATOSPHERIC WATER VAPOR
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AN ATMOSPHERIC TAPE RECORDER - THE IMPRINT OF TROPICAL TROPOPAUSE TEMPERATURES ON STRATOSPHERIC WATER VAPOR

机译:大气带记录器-热带对流层温度对平流层水蒸气的影响

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We describe observations of tropical stratospheric water vapor q that show clear evidence of large-scale upward advection of the signal from annual fluctuations in the effective ''entry mixing ratio'' q(E) of air entering the tropical stratosphere, In other words, air is ''marked,'' on emergence above the highest cloud tops, like a signal recorded on an upward moving magnetic tape, We define q(E) as the mean water vapor mixing ratio, at the tropical tropopause, of air that will subsequently rise and enter the stratospheric ''overworld'' at about 400 K. The observations show a systematic phase lag, increasing with altitude, between the annual cycle in q(E) and the annual cycle in q at higher altitudes, The observed phase lag agrees with the phase lag calculated assuming advection by the transformed Eulerian-mean vertical velocity of a q(E) crudely estimated from 100-hPa temperatures, which we use as a convenient proxy for tropopause temperatures, The phase agreement confirms the overall robustness of the calculation and strongly supports the tape recorder hypothesis, Establishing a quantitative link between q(E) and observed tropopause temperatures, however, proves difficult because the process of marking the tape depends subtly on both small- and large-scale processes, The tape speed, or large-scale upward advection speed, has a substantial annual variation and a smaller variation due to the quasi-biennial oscillation, which delays or accelerates the arrival of the signal by a month or two in the middle stratosphere. As the tape moves upward, the signal is attenuated with an e-folding time of about 7 to 9 months between 100 and 50 hPa and about 15 to 18 months between 50 and 20 hPa, constraining possible orders of magnitude both of vertical diffusion K-z and of rates of mixing in from the extratropics. For instance, if there were no mixing in, then K-z would be in the range 0.03-0.09 m(2) s(-1); this is an upper bound on K-z. [References: 62]
机译:我们描述了对热带平流层水蒸气q的观测,这些观测表明来自进入热带平流层的空气的有效“入口混合比” q(E)的年度波动的信号大规模向上平流的证据,换句话说,空气在最高云层上方出现时被“标记”,就像记录在向上移动的磁带上的信号一样,我们将q(E)定义为热带对流层顶上空气的平均水蒸气混合比随后在约400 K处上升并进入平流层“ overworld”。观测结果表明,在较高高度处,q(E)的年周期与q的年周期之间存在系统的相位滞后,随高度增加而增加。滞后时间与相位滞后时间一致,该滞后时间与假设的对流时间一致,该滞后时间是根据从100-hPa温度粗略估算的aq(E)转换后的欧拉平均垂直速度对流计算得出的,我们将其用作对流层顶温度的便捷代表,该相位滞后确认了总体计算的鲁棒性并有力地支持了磁带录音机的假设,但是,在q(E)与对流层顶温度之间建立定量联系非常困难,因为标记磁带的过程取决于小规模和大规模过程,磁带速度或大型向上对流速度由于准两年一次的振荡而具有较大的年度变化和较小的变化,这会使信号在平流层中部延迟或加速达一两个月。当磁带向上移动时,信号在100到50 hPa之间以大约7到9个月的电子折叠时间衰减,在50到20 hPa之间以大约15到18个月的电子折叠时间衰减,从而限制了垂直扩散Kz和来自热带的混合速率。例如,如果没有混合,则K-z将在0.03-0.09 m(2)s(-1)范围内;这是K-z的上限。 [参考:62]

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