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Modeling crater populations on Venus and Titan

机译:在金星和土卫六上模拟环形山人口

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We describe a model for crater populations on planets and satellites with dense atmospheres, like those of Venus and Titan. The model takes into account ablation (or mass shedding), pancaking, and fragmentation. Fragmentation is assumed to occur due to the hydrodynamic instabilities promoted by the impactors' deceleration in the atmosphere. Fragments that survive to hit the ground make craters or groups thereof. Crater sizes are estimated using standard laws in the gravity regime, modified to take into account impactor disruption. We use Monte Carlo methods to pick parameters from appropriate distributions of impactor mass, zenith angle, and velocity. Good fits to the Venus crater populations (including multiple crater fields) can be found with reasonable values of model parameters. An important aspect of the model is that it reproduces the dearth of small craters on Venus: this is due to a cutoff on crater formation we impose, when the expected crater would be smaller than the (dispersed) object that would make it. Hydrodynamic effects alone (ablation, pancaking, fragmentation) due to the passage of impactors through the atmosphere are insufficient to explain the lack of small craters. In our favored model, the observed number of craters (940) is produced by ~5500 impactors with masses > 10~(15) gm, yielding an age of 730 ± 110Myr (1-σ uncertainty) for the venusian surface. This figure does not take into account any uncertainties in crater scaling and impactor population characteristics, which probably increase the uncertainty to a factor of two in age. We apply the model with the same parameter values to Titan to predict crater populations under differing assumptions of impactor populations that reflect present conditions. We assume that the impactors (comets) are made of 50% porous ice. Predicted crater production rates are ≈ 190 craters (10~9 yr)~(-1). The smallest craters on Titan are predicted to be ≈ 2 km in diameter, and ≈ 5 crater fields (10~9 yr)~(-1) are expected. If the impactors are composed of solid ice (density 0.92 gmcm~(-3)), crater production rates increase by ≈ 70% and the smallest crater is predicted to be ≈ 1.6km in diameter. We give cratering rates for denser comets and atmospheres 0.1 and 10 times as thick as Titan's current atmosphere. We also explicitly address leading-trailing hemisphere asymmetries that might be seen if Titan's rotation rate were strictly synchronous over astronomical timescales: if that is the case, the ratio of crater production on the leading hemisphere to that on the trailing hemisphere is ≈ 4 : 1.
机译:我们描述了一个在大气层密集的行星和卫星上(如金星和泰坦)的陨石坑人口的模型。该模型考虑了消融(或大量脱落),结块和碎裂。假定碎裂是由于冲击器在大气中的减速所引起的水动力不稳定性而发生的。幸存下来撞击地面的碎片会形成陨石坑或陨石坑。火山口的大小是根据重力情况下的标准定律估算的,修改后考虑了撞击器的破坏。我们使用蒙特卡洛方法从冲击器质量,天顶角和速度的适当分布中选取参数。可以找到具有合理模型参数值的金星火山口种群(包括多个火山口区域)的良好拟合。该模型的一个重要方面是,它再现了金星上小的陨石坑的缺乏:这是由于我们施加的陨石坑形成的临界值所致,此时预期的陨石坑将小于形成它的(分散的)物体。仅由于冲击器通过大气而产生的流体动力效应(消融,裂化,破碎)不足以解释缺少小火山口的原因。在我们偏爱的模型中,观测到的火山口数量(940)是由5500个质量大于10〜(15)g的撞击器产生的,金星表面的年龄为730±110Myr(1-σ不确定性)。该数字未考虑火山口规模和撞击者种群特征的任何不确定性,这些不确定性可能会将不确定性增加到年龄的两倍。我们将具有相同参数值的模型应用于Titan,以根据反映当前状况的不同影响人口假设来预测火山口人口。我们假设撞击器(彗星)由50%的多孔冰制成。预测的火山口生产率约为190火山口(10〜9年)〜(-1)。土卫六上最小的陨石坑的直径预计约为≈2 km,预计会有≈5个陨石坑场(10〜9年)〜(-1)。如果撞击器由固态冰组成(密度为0.92 gmcm〜(-3)),则陨石坑的生产率将增加≈70%,并且最小的陨石坑的直径预计约为≈1.6 km。对于较密集的彗星和大气,我们给出的陨石坑率是土卫六当前大气的0.1和10倍。如果土卫六的旋转速率在天文时间尺度上严格同步,则可能会看到前半球的不对称性:如果是这种情况,则前半球与后半球的弹坑产量之比为≈4:1 。

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