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Upper-troposphere and lower-stratosphere water vapor retrievals from the 1400 and 1900 nm water vapor bands

机译:从1400和1900 nm水汽带对流层和平流层下层的水汽反演

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摘要

Measuring water vapor in the upper troposphere and lower stratosphere isdifficult due to the low mixing ratios found there, typically only a fewparts per million. Here we examine near-infrared spectra acquired with theSolar Spectral Flux Radiometer (SSFR) during the first science phase of theNASA Airborne Tropical TRopopause EXperiment (ATTREX). From the 1400 and1900 nm absorption bands we infer water vapor amounts in the tropicaltropopause layer and adjacent regions between altitudes of 14 and 18 km. Wecompare these measurements to solar transmittance spectra produced with theMODerate resolution atmospheric TRANsmission (MODTRAN) radiative transfermodel, using in situ water vapor, temperature, and pressure profiles acquiredconcurrently with the SSFR spectra. Measured and modeled transmittance valuesagree within 0.002, with some larger differences in the 1900 nm band (up to0.004). Integrated water vapor amounts along the absorption path lengths of 3to 6 km varied from 1.26 × 10 to4.59 × 10 g cm. A 0.002 difference in absorptance at1367 nm results in a 3.35 × 10 g cm change ofintegrated water vapor amounts; 0.004 absorptance change at 1870 nm resultsin 5.50 × 10 g cm of water vapor. These are 27%(1367 nm) and 44% (1870 nm) differences at the lowest measured valueof water vapor (1.26 × 10 g cm) and 7%(1367 nm) and 12% (1870 nm) differences at the highest measured valueof water vapor (4.59 × 10 g cm). A potential methodfor extending this type of measurement from aircraft flight altitude to thetop of the atmosphere is discussed.
机译:由于对流层和对流层下层的水汽混合比很低,因此很难进行测量,因为那里的混合比很低,通常只有百万分之几。在这里,我们研究了在美国国家航空航天局(NASA)机载热带菊苣试验(ATTREX)的第一个科学阶段用太阳能光谱通量辐射计(SSFR)获得的近红外光谱。从1400和1900 nm的吸收带中,我们推断出热带对流层顶层和高度在14和18 km之间的相邻区域中的水蒸气量。我们将这些测量结果与利用中等分辨率大气TRANsmission(MODTRAN)辐射传递模型产生的太阳透射光谱进行比较,并使用与SSFR光谱同时获取的原位水汽,温度和压力剖面。测得的和模拟的透射率值在0.002以内,在1900 nm波段有较大差异(最高0.004)。沿着3至6 km的吸收路径长度的积分水蒸气量为1.26×10至4.59×10 g cm。 1367 nm处的吸光度差异0.002导致积分的水蒸气量变化3.35×10 g cm。在1870 nm处0.004的吸收率变化导致5.50×10 g cm的水蒸气。在最低的水蒸气测量值(1.26×10 g cm)处分别有27%(1367 nm)和44%(1870 nm)的差异,在最高的测量值处分别有7%(1367 nm)和12%(1870 nm)的差异水蒸气(4.59×10 g厘米)。讨论了一种将这种类型的测量从飞机飞行高度扩展到大气层顶部的潜在方法。

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