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Photochemical escape of atomic C and N on Mars: clues from a multi-instrument MAVEN dataset

机译:原子C和N在火星上的光化学逸出:来自多仪器MAVEN数据集的线索

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Context. Photochemical escape of hot atoms is crucial to the long-term evolution of the Martian climate. For atomic C and N, photochemical escape is primarily driven by photodissociation (PD) of CO and N_(2). Aims. Combining the Mars Atmosphere and Volatile Evolution (MAVEN) measurements of atmospheric neutral densities and solar EUV/X-ray irradiance, we perform a state-of-the-art analysis of atomic C and N escape on Mars. Methods. For each MAVEN orbit, we calculated the hot C and N production rates in the dayside Martian upper atmosphere via PD, from which the escape rates are estimated using a simplified technique to parameterize the respective escape probabilities taking into account multiple collisions with ambient neutrals. Results. The mean C and N escape rates are 1 × 10~(24)s~(?1)and 9 × 10~(24)s~(?1), appropriate for low to moderate solar activity conditions, and thermospheric PD makes a larger contribution to the total N escape than to the total C escape. The above differences highlight the importance of nascent energy, with more energetic nascent escaping atoms able to survive collisions with ambient neutrals more easily, thus extending down to deeper regions of the atmosphere. Solar cycle variation in C and N escape is revealed by our analysis, whereas solar zenith angle variation is absent for both species. These results could be explained by the fact that the production of nascent escaping atoms responds to varying solar illumination angle at low altitudes where the escape probability is negligible, but responds to varying level of solar EUV/X-ray irradiance at high altitudes where the atmosphere is essentially collisionless.
机译:上下文。热原子的光化学逸出对于火星气候的长期演变至关重要。对于原子C和N,光化学逸出主要由CO和N_(2)的光解离(PD)驱动。目的结合火星大气中性密度和太阳EUV / X射线辐照度的挥发分(MAVEN)测量,我们对火星上的原子C和N逸出进行了最新分析。方法。对于每个MAVEN轨道,我们都通过PD计算了火星在白天高空大气层中的高温C和N产生率,使用简化的技术从中估算出逃逸率,以考虑与环境中性粒子的多次碰撞来对各自的逃逸概率进行参数化。结果。 C和N的平均逸出率分别为1×10〜(24)s〜(?1)和9×10〜(24)s〜(?1),适用于中低度太阳活动条件,而热球PD使N总逸出量比C总逸出量更大。上述差异突出了新生能量的重要性,使更多高能的新生逃逸原子能够更轻松地与环境中性分子碰撞,从而向下延伸到更深的大气层。我们的分析揭示了C和N逸出的太阳周期变化,而这两个物种都没有太阳天顶角变化。这些结果可以通过以下事实来解释:新生逃逸原子的产生在逃逸概率可忽略的低空响应于变化的太阳照度,而在大气高空响应于变化的太阳EUV / X射线辐照水平本质上是无碰撞的。

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