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Post-bubble close-off fractionation of gases in polar firn and ice cores: effects of accumulation rate on permeation through overloading pressure

机译:极地冰芯和冰芯中气体的气泡后关闭分馏:通过超载压力,积累速率对渗透的影响

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Gases in ice cores are invaluable archives of past environmental changes (e.g., the past atmosphere). However, gas fractionation processes after bubble closure in the firn are poorly understood, although increasing evidence indicates preferential leakages of smaller molecules (e.g., neon, oxygen, and argon) from the closed bubbles through the ice matrix. These fractionation processes are believed to be responsible for the observed millennial delta O-2/N-2 variations in ice cores, linking ice core chronologies with orbital parameters. In this study, we investigated high-resolution delta Ar/N-2 of the GISP2 (Greenland Ice Sheet Project 2), NGRIP (North Greenland Ice Core Project), and Dome Fuji ice cores for the past few thousand years. We find that delta Ar/N-2 at multidecadal resolution on the "gas-age scale" in the GISP2 ice core has a significant negative correlation with accumulation rate and a positive correlation with air contents over the past 6000 years, indicating that changes in overloading pressure induced delta Ar/N-2 fractionation in the firn. Furthermore, the GISP2 temperature and accumulation rate for the last 4000 years have nearly equal effects on delta Ar/N-2 with sensitivities of 0.72 +/- 0.1 parts per thousand degrees C-1 and -0.58 +/- 0.09 parts per thousand(0.01mice year(-1))(-1), respectively. To understand the fractionation processes, we applied a permeation model for two different processes of bubble pressure build-up in the firn, "pressure sensitive process" (e.g., microbubbles: 0.3-3% of air contents) with a greater sensitivity to overloading pressures and "normal bubble process". The model indicates that delta Ar/N-2 in the bubbles under the pressure sensitive process are negatively correlated with the accumulation rate due to changes in overloading pressure. On the other hand, the normal bubbles experience only limited depletion (< 0.5 parts per thousand) in the firn. Colder temperatures in the firn induce more depletion in delta Ar/N-2 through thicker firn. The pressure sensitive bubbles are so depleted in delta Ar/N-2 at the bubble close-off depth that they dominate the total delta Ar/N-2 changes in spite of their smaller air contents. The model also indicates that delta Ar/N-2 of ice cores should have experienced several per mil of depletion during the storage 14-18 years after coring. Further understanding of the delta Ar/N-2 fractionation processes in the firn, combined with nitrogen and argon isotope data, may lead to a new proxy for the past temperature and accumulation rate.
机译:冰芯中的气体是过去环境变化(例如过去大气)的宝贵档案。然而,尽管越来越多的证据表明较小的分子(例如,氖,氧和氩)从闭合的气泡通过冰基质优先泄漏,但人们对熔炉中气泡闭合后的气体分馏过程了解甚少。据信,这些分馏过程是造成冰芯中观测到的千年三角洲O-2 / N-2变化的原因,并将冰芯年代与轨道参数联系起来。在这项研究中,我们调查了过去几千年来GISP2(格陵兰冰原项目2),NGRIP(北格陵兰冰芯项目)和圆顶富士冰芯的高分辨率δAr / N-2。我们发现,在过去的6000年中,GISP2冰芯中“气-年龄尺度”上的数十年代分辨率上的Ar / N-2增量与累积速率呈显着负相关,与空气含量呈正相关。压力过大会导致炉内δAr / N-2分馏。此外,最近4000年的GISP2温度和累积速率对Delta Ar / N-2具有几乎相同的影响,其灵敏度分别为0.72 +/- 0.1份/千摄氏度C-1和-0.58 +/- 0.09份/千( 0.01小鼠年(-1))(-1)。为了理解分馏过程,我们对渗透过程中气泡压力建立的两个不同过程应用了渗透模型,即“压力敏感过程”(例如,微气泡:空气含量的0.3-3%),对过载压力具有更高的敏感性。和“正常气泡过程”。该模型表明,由于超载压力的变化,压敏过程中气泡中的δAr / N-2与累积速率呈负相关。另一方面,正常气泡在焙烧过程中仅经历有限的消耗(<0.5千分之几)。炉膛温度较低,通过较厚的炉膛会导致δAr / N-2耗尽。压敏气泡在气泡关闭深度处以ΔAr/ N-2耗尽,以至于尽管它们的空气含量较小,但它们仍控制着总ΔAr/ N-2变化。该模型还表明,取芯后14到18年的存储期间,冰芯的δAr / N-2损耗应达到每密耳数百万。进一步了解炉膛中的δAr / N-2分馏过程,再结合氮和氩同位素数据,可能会为过去的温度和累积速率提供新的替代指标。

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