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Identification of the 10-μm ammonia ice feature on Jupiter

机译:木星上10μm氨冰特征的识别

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We present the first detection of NH_3 ice in the thermal infrared in Jupiter's atmosphere using Cassini CIRS observations in the 10-μm region obtained on 31 December 2000 and 1 January 2001. We identify a brightness temperature difference α ≡ T_B (1040 cm~(-1)) -T_B(1060 cm~(-1)) as an indicator of spectrally identifiable NH_3 ice, where 1040 cm~(-1) is an adjacent continuum region and 1060 cm~(-1) is the NH_3 ice feature. Higher values of α imply a stronger NH_3 ice signature in the spectrum. Using midlatitude zonally averaged CIRS spectra, we demonstrate systematic spatial variations in α, with the highest values at the equator and near 23°N. In one CIRS spectral average (covering 22-25°N and 140-240°W), our radiative transfer models are consistent with an optical depth of 0.75 +- 0.25 for NH_3 ice particles modeled as randomly oriented 4:1 prolate spheroids (volume equivalent radius = 0.79 μm). Particles larger or smaller than 1 μm by about a factor of 2 would be unable to duplicate the observed NH_3 ice feature at 1060 cm~(-1): absorption due to larger particles is excessively broadened, and absorption due to smaller particles is hidden by NH_3 gas absorption at 1067 cm~(-1). We also modeled an average spectrum for a second region on Jupiter (14-17°N and 10-70°W), finding an upper limit of τ = 0.2 for the same NH_3 ice particle type. The choice of prolate spheroid particles is based on laboratory studies of NH_3 ice aerosols, although 1-m Mie-scattering spheres would also have detectable signatures at 1060 cm~(-1). We model the 1-μm NH_3 ice cloud with a particle-to-gas scale height ratio H_p/H_g = 1. For both CIRS spectra analyzed, the spectrum at frequencies greater than 1100 cm~(-1) also requires a second cloud with essentially grey absorption, which we modeled using 10-μm NH_3 ice spheres distributed with H_p/H_g = 1/8 and a cloud base at 790 mbar.
机译:我们利用2000年12月31日和2001年1月1日获得的10-μm区域的卡西尼CIRS观测值,首次检测了木星大气中热红外中的NH_3冰。我们确定了亮度温度差α≡T_B(1040 cm〜(- 1))-T_B(1060 cm〜(-1))作为可光谱识别的NH_3冰的指标,其中1040 cm〜(-1)是相邻的连续区域,而1060 cm〜(-1)是NH_3冰特征。 α值越高,表示光谱中的NH_3冰签名越强。使用中纬度纬向平均CIRS谱,我们证明了α的系统空间变化,在赤道和23°N附近具有最高值。在一个CIRS光谱平均值(覆盖22-25°N和140-240°W)中,我们的辐射传输模型与NH_3冰粒的光学深度0.75±0.25一致,NH_3冰粒建模为随机定向的4:1扁长球体(体积当量半径= 0.79μm)。大于或小于1μm约2倍的粒子将无法复制在1060 cm〜(-1)处观察到的NH_3冰特征:较大粒子引起的吸收过度展宽,较小粒子引起的吸收被隐藏在1067 cm〜(-1)处吸收NH_3气体。我们还对木星第二个区域(14-17°N和10-70°W)的平均光谱建模,发现相同NH_3冰粒类型的τ= 0.2的上限。扁长球体颗粒的选择基于NH_3冰气溶胶的实验室研究,尽管1-m Mie散射球在1060 cm〜(-1)处也具有可检测的特征。我们以粒子与气体尺度的高度比H_p / H_g = 1为模型,对1-μmNH_3冰云进行建模。对于所分析的两个CIRS光谱,频率大于1100 cm〜(-1)的光谱也需要第二个云,本质上是灰色吸收,我们使用分布为H_p / H_g = 1/8的10-μmNH_3冰球和790 mbar的云层进行建模。

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