所谓“仙女圈”中地下H2浓度的时空分布:来自概念二维输运模型的见解

Andrey Myagkiy, I. Moretti, F. Brunet
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引用次数: 14

摘要

现在已经在世界上许多地方测量了地面自然排放的氢气。这些排放物可以局限在断层上,也可以更分散地分布在一些沉积盆地中,通常是元古代的盆地。在这种情况下,从航空图像或高分辨率地形图上通常可以看到辐射区,因为它们对应于圆形到椭圆形的轻微凹陷。此外,圆形的洼地覆盖着灌木植被,与周围的植被形成鲜明对比。虽然发射结构呈现出非常规则的形状,但这种结构中首米土壤中H2浓度的分布确实呈现出清晰的规律。例如,在结构的中心几乎没有测量到最大浓度,并且很少有时间分辨的数据表明土壤H2浓度随时间变化。本文采用H2在多孔介质中输运的二维平流扩散模型模拟了H2浓度的时空演化。测试了氢气点源(脉冲)的深度和周期性、细菌氢气消耗和土壤渗透性非均质性等参数。结构的半径与氢气在土壤中停留的时间有关,这取决于土壤的渗透性、气体泄漏点的深度和气泡的压力。为了解释现场观测,对结构中心的泥质、渗透性较差的非均质进行了模拟。其结果是沿结构边缘的浓度增加,而结构中心的信号接近于零。如果深信号是周期性的,且频率小于几小时,则土壤中H2浓度几乎是恒定的;在其他情况下,近地表浓度波反映了具有延迟的源的浓度周期性(在30米土壤的12小时范围内),因此近地表H2浓度值将高度依赖于进行测量的时间。因此,通过传感器网络进行H2监测是表征仙女圈土壤中H2动态的必要条件。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Space and time distribution of subsurface H2 concentration in so-called “fairy circles”: Insight from a conceptual 2-D transport model
Natural H2 emissions from the ground have now been measured in many places worldwide. These emissions can be localized on faults or be more diffuse in some sedimentary basins, usually of Proterozoic age. In such a case, emanation zones are often visible from aerial images or on high-resolution topographic maps since they correspond to slight depressions of circular to elliptic shape. Furthermore, the rounded depressions are covered with a scrubby vegetation which often contrasts with the surrounding vegetation. Although the emission structure displays a very regular shape, the distribution of H2 concentration in the first meter of soil in such a structure does show a clear pattern. For example, the maximum concentration is almost never measured in the center of the structure and the few time-resolved data show that the soil H2 concentration is variable with time. Here, the time and space evolution of H2 concentration is simulated using a 2-D advective-diffusive model of H2 transport in porous media. Several parameters have been tested as the depth and periodicity of the H2 point source (pulsed), bacterial H2 consumption and permeability heterogeneities of the soil. The radius of the structure is linked to the time spent by the H2 in the soil that depends on the soil permeability, the depth of the gas leakage point and the pressure of the bubble. To account for field observations, the case of a shaly, less permeable, heterogeneity in the center of the structures has been modeled. It resulted in an increase of the concentration toward the rim of the structure and a close to zero signal in its center. If the deep signal is periodic with a frequency smaller than a few hours, H2 concentration within the soil is almost constant; in other cases, the near surface concentration wave reflects the concentration periodicity of the source with a delay (in the range of 12 h for 30 m of soil) and so the near surface H2 concentration values will be highly dependent on the time at which the measurement is performed. H2 monitoring through a sensor network is thus mandatory to characterize the H2 dynamics in the soil of fairy circles.
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