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海王星上的云层、阴霾和平流层甲烷丰度。

Clouds, hazes, and the stratospheric methane abundance in Neptune.

作者信息

Baines K H, Hammel H B

机构信息

Jet Propulsion Laboratory, California Institute of Technology, Pasadena 91109, USA.

出版信息

Icarus. 1994 May;109(1):20-39. doi: 10.1006/icar.1994.1075.

DOI:10.1006/icar.1994.1075
PMID:11539136
Abstract

Analysis of high-spatial-resolution (approximately 0.8 arcsec) methane band and continuum imagery of Neptune's relatively homogeneous Equatorial Region yields significant constraints on (1) the stratospheric gaseous methane mixing ratio (fCH4,s), (2) the column abundances and optical properties of stratospheric and tropospheric hydrocarbon hazes, and (3) the wavelength-dependent single-scattering albedo of the 3-bar opaque cloud. From the center-to-limb behavior of the 7270-angstroms and 8900-angstrom sCH4 bands, the stratospheric methane mixing ratio is limited to fCH4,s < 1.7 x 10(-3), with a nominal value of fCH4,s = 3.5 x 10(-4), one to two orders of magnitude less than pre-Voyager estimates, but in agreement with a number of recent ultraviolet and thermal infrared measurements, and largely in agreement with the tropopause mixing ratio implied by Voyager temperature measurements. Upper limits to the stratospheric haze mass column abundance and 6190-angstroms and 8900-angstroms haze opacities are 0.61 microgram cm-2 and 0.075 and 0.042, respectively, with nominal values of 0.20 microgram cm-2 and 0.025 and 0.014 for the 0.2-micrometer radius particles preferred by the recent Voyager PPS analysis of Pryor et al. (1992, Icarus 99, 302-316). The tropospheric CH4 haze opacities are comparable to that found in the stratosphere, upper limits of 0.104 and 0.065 at 6190 angstroms and 8900 angstroms, respectively, with nominal values of 0.085 and 0.058. This indicates a column abundance less than 11.0 micrograms cm-2, corresponding to the methane gas content within a well-mixed 3% methane tropospheric layer only 0.1 cm thick near the 1.5-bar CH4 condensation level. Constraints on the single-scattering albedos of these hazes include (1) for the stratospheric component, 6190-angstroms and 8900-angstroms imaginary indices of refraction less than 0.047 and 0.099, respectively, with 0.000 (conservative scattering) being the nominal value at both wavelengths, and (2) CH4 haze single-scattering albedos greater than 0.85 and 0.50 at these two wavelengths, with conservative scattering again begin the preferred value. However, conservative scattering is ruled out for the opaque cloud near 3 bars marking the bottom of the visible atmosphere. Specifically, we find cloud single-scattering albedos of 0.915 +/- 0.006 at 6340 angstroms, 0.775 +/- 0.012 at 7490 angstroms, and 0.803 +/- 0.010 at 8260 angstrom. Global models utilizing a complete global spectrum confirm the red-absorbing character of the 3-bar cloud. The global-mean model has approximately 7.7 times greater stratospheric aerosol content then the Equatorial Region. An analysis of stratospheric haze precipitation rates indicates a steady-state haze production rate of 0.185-1.5 x 10(-14) g cm-2 sec-1, in agreement with recent theoretical photochemical estimates. Finally, reanalysis of the Voyager PPS 7500-angstroms phase angle data utilizing the fCH4,s value derived here confirms the Pryor et al. result of a tropospheric CH4 haze opacity of a few tenths in the 22-30 degrees S latitude region, several times that of the Equatorial Region or of the globe. The factor-of-10 reduction in fCH4,s below that assumed by Pryor et al. implies decreased gas absorption and consequently a decrease in the forward-scattering component of tropospheric aerosols.

摘要

对海王星相对均匀的赤道区域的高空间分辨率(约0.8角秒)甲烷谱带和连续体图像进行分析,得出了以下重要限制:(1)平流层气态甲烷混合比(fCH4,s);(2)平流层和对流层碳氢化合物霾的柱丰度和光学性质;(3)3巴不透明云的波长依赖单散射反照率。根据7270埃和8900埃sCH4谱带从中心到边缘的变化情况,平流层甲烷混合比限制为fCH4,s < 1.7×10−3,标称值为fCH4,s = 3.5×10−4,比航海者号之前的估计值小一到两个数量级,但与最近的一些紫外和热红外测量结果一致,并且在很大程度上与航海者号温度测量所暗示的对流层顶混合比一致。平流层霾质量柱丰度以及6190埃和8900埃霾的光学厚度的上限分别为0.61微克/平方厘米、0.075和0.042,而普赖尔等人(1992年,《伊卡洛斯》99卷,302 - 316页)最近对航海者号偏振光分光计(PPS)的分析所青睐的半径为0.2微米的粒子的标称值分别为0.20微克/平方厘米、0.025和0.014。对流层CH4霾的光学厚度与平流层中的相当,6190埃和8900埃处的上限分别为0.104和0.065,标称值分别为0.085和0.058。这表明柱丰度小于11.0微克/平方厘米,对应于在1.5巴CH4凝结水平附近仅0.1厘米厚的充分混合的3%甲烷对流层内的甲烷气体含量。对这些霾的单散射反照率的限制包括:(1)对于平流层成分,6190埃和8900埃处的虚折射率分别小于0.047和0.099,两个波长处的标称值均为0.000(保守散射);(2)在这两个波长处,CH4霾的单散射反照率大于0.85和0.50,保守散射再次为首选值。然而,对于标志着可见大气底部的3巴附近的不透明云,保守散射被排除。具体而言,我们发现在6340埃处云的单散射反照率为0.915±0.006,在7490埃处为0.775±0.012,在8260埃处为0.803±0.010。利用完整的全球光谱的全球模型证实了3巴云的红吸收特性。全球平均模型的平流层气溶胶含量比赤道区域大约高7.7倍。对平流层霾沉降率的分析表明,稳态霾产生率为0.185 - 1.5×10−14克/平方厘米·秒,与最近的理论光化学估计值一致。最后,利用此处得出的fCH4,s值对航海者号PPS 7500埃相角数据进行重新分析,证实了普赖尔等人的结果,即在南纬22 - 30度区域对流层CH4霾的光学厚度为十分之几,是赤道区域或全球的几倍。fCH4,s比普赖尔等人假设的值降低了一个数量级,这意味着气体吸收减少,从而对流层气溶胶的前向散射分量减少。

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