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Shock-induced vaporization of anhydrite and global cooling from the K/T impact

机译:冲击诱导的硬石膏汽化和K / T冲击引起的整体冷却

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Discovery of abundant anhydrite (CaSO_4) and gypsum (CaSO_4·2H_2O) in the otherwise carbonate sediment comprising the upper 3 km thick layer of the target rock at the K/T impact site has prompted research on these minerals. Evaluation of the severity of the proposed extinction mechanism involving injection of impact-generated SO_2 and SO_3 into the stratosphere entails determination of criteria for shock-induced vaporization of these minerals. In the present work we present new data on the vaporization criteria of anhydrite. These are based on the reanalysis of the shock wave experiments of Yang and Ahrens [Earth Planet. Sci. Lett. 156 (1998) 125-140], conducted on material with 30% porosity, in which the shock- (fully or partially) vaporized sample interacts with an overlying LiF window. The velocity histories, monitored using a velocity interferometer, are compared with numerical simulations employing an improved equation of state for porous anhydrite and its vaporization products. We also employ the 'entropy criterion' for vaporization of material under shock compression. The values of the entropies of incipient and complete vaporization for anhydrite are determined to be 1.65 ± 0.12 and 3.17 ± 0.12 kJ (kg K)~(-1), respectively, and the corresponding pressures for incipient and the complete vaporization along the Hugoniot for the solid material are 32.5 ± 2.5 and 122 ± 13 GPa, respectively as compared with 81 ± 7 and 155 ± 13 GPa previously reported by Yang and Ahrens. Along with these criteria, the use of the recent estimate of diameter (100 km) for the Chicxulub transient crater [O'Keefe and Ahrens, J. Geophys. Res. 104 (E11) (1999) 27091-27104; Morgan et al., Nature 390 (1997) 472-476] that is smaller than previously assumed, along with Ivanov et al.'s [Geol. Soc. Am. Spec. Pap. 307 (1996) 125-142] 2-D hydrodynamic simulation to determine the shock attenuation and Pope et al.'s [J. Geophys. Res., 102 (E9) (1997) 21645-21664] radiative transfer model, yields the maximum decrease in the average global surface temperature of 12-19 K for 9.0-9.5 years at the K/T boundary. Thus, the global cooling is inferred to have been less severe than that indicated by the upper limit of the range of 5-31 K decrease lasting for ~ 12 years calculated by Pope et al. Because ambient global surface temperatures at K/T time were ~ 18-20 ℃ warmer than present values, this cooling even produced cold, but not freezing conditions at the Earth's surface.
机译:在K / T撞击点的目标岩石上部3 km厚的碳酸盐沉积物中发现了丰富的硬石膏(CaSO_4)和石膏(CaSO_4·2H_2O),这促使人们对这些矿物进行了研究。对拟议的灭绝机制的严重性进行评估,包括将撞击产生的SO_2和SO_3注入到平流层中,就需要确定冲击诱发的这些矿物汽化的标准。在目前的工作中,我们提出了有关硬石膏汽化标准的新数据。这些是基于对Yang和Ahrens [地球行星的冲击波实验的重新分析。科学来吧156(1998)125-140],该方法在孔隙率为30%的材料上进行,其中被冲击(完全或部分)汽化的样品与上方的LiF窗口相互作用。将使用速度干涉仪监测的速度历史与采用改进状态方程的多孔硬石膏及其汽化产物的数值模拟进行比较。我们还采用“熵准则”对材料在冲击压缩条件下的气化进行汽化。硬石膏的初始和完全汽化的熵值分别确定为1.65±0.12和3.17±0.12 kJ(kg K)〜(-1),相应的沿Hugoniot的初始压力和完全汽化的压力为固态材料分别为32.5±2.5和122±13 GPa,而Yang和Ahrens先前报道的为81±7和155±13 GPa。连同这些标准一起,使用了Chicxulub瞬变坑的最近直径估计值(100 km)[O'Keefe and Ahrens,J. Geophys。 Res。 104(E11)(1999)27091-27104; Morgan等人,以及Ivanov等人的[Geol。Chem。,(1989)472-476]比以前假定的要小。 Soc。上午。规格爸爸307(1996)125-142] 2D流体动力学模拟,以确定冲击衰减和Pope等人的研究[J.地理学。 [Res。,102(E9)(1997)21645-21664]的辐射传递模型在K / T边界处产生了9.0-9.5年的12-19 K的平均全球平均表面温度的最大下降。因此,推断总体降温程度不如Pope等人计算的,持续时间约为12年的5-31 K降幅范围的上限所表明的那样严重。由于在K / T时间的全球地表温度要比现在的温度高约18-20℃,所以这种冷却甚至在地球表面产生了寒冷,但没有结冰。

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