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Short communication: Increasing vertical attenuation length of cosmogenic nuclide production on steep slopes negates topographic shielding corrections for catchment erosion rates

机译:沟通短促:陡坡上宇宙成核物质产量的垂直衰减长度的增加抵消了流域侵蚀率的地形屏蔽校正

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Interpreting catchment-mean erosion rates from in situ produced cosmogenic sup10/supBe concentrations in stream sediments requires calculating the catchment-mean sup10/supBe surface production rate and effective mass attenuation length, both of which can vary locally due to topographic shielding and slope effects. The most common method for calculating topographic shielding accounts only for the reduction of nuclide production rates due to shielding at the surface, leading to catchment-mean corrections of up to 20?% in steep landscapes, and makes the simplifying assumption that the effective mass attenuation length for a given nuclide production mechanism is spatially uniform. Here I evaluate the validity of this assumption using a simplified catchment geometry with mean slopes ranging from 0 to 80 sup°/sup to calculate the spatial variation in surface skyline shielding, effective mass attenuation length, and the total effective shielding factor, defined as the ratio of the shielded surface nuclide concentration to that of an unshielded horizontal surface. For flat catchments (i.e., uniform elevation of bounding ridgelines), the effect of increasing vertical attenuation length as a function of hillslope angle and skyline shielding exactly offsets the effect of decreasing surface production rate, indicating that no topographic shielding correction is needed when calculating catchment-mean vertical erosion rates. For dipping catchments (as characterized by a plane fit to the bounding ridgelines), the catchment-mean surface nuclide concentrations are also equal to that of an unshielded horizontal surface, except for cases of extremely steep range-front catchments, where the surface nuclide concentrations are counterintuitively higher than the unshielded case due to added production from oblique cosmic ray paths at depth. These results indicate that in most cases topographic shielding corrections are inappropriate for calculating catchment-mean erosion rates, and are only needed for steep catchments with nonuniform distributions of quartz and/or erosion rate. By only accounting for shielding of surface production, existing shielding approaches introduce a slope-dependent systematic error that could lead to spurious interpretations of relationships between topography and erosion rate.
机译:从原位产生的宇宙成因 10 Be浓度解释流域平均侵蚀速率需要计算流域平均表面集水率 10 Be生产率和有效质量衰减长度,由于地形屏蔽和坡度影响,其局部变化。计算地形屏蔽的最常用方法仅考虑到由于在表面进行屏蔽而导致的核素生产率下降,从而导致陡峭地形中的集水率均值校正高达20%,并简化了假设,即有效质量衰减给定核素产生机制的长度在空间上是均匀的。在这里,我使用平均范围为0到80 °的平均斜率来计算该假设的有效性,以计算表面天际线屏蔽的空间变化,有效质量衰减长度以及总有效屏蔽系数定义为屏蔽表面核素浓度与未屏蔽水平表面的浓度之比。对于平坦的集水区(即均匀的山脊线高程),增加垂直衰减长度作为坡度和天际线遮挡的函数的影响正好抵消了降低表面生产率的影响,这表明在计算集水区时不需要地形屏蔽校正-平均垂直侵蚀率。对于浸入式集水区(特征在于与边界脊线的平面拟合),集水区平均表面核素浓度也等于非屏蔽水平面的浓度,但极陡峭的范围前集水区的情况除外,其中表面核素浓度由于在深处倾斜的宇宙射线路径增加了产量,因此比非屏蔽情况高出直觉。这些结果表明,在大多数情况下,地形屏蔽校正不适用于计算流域平均侵蚀率,仅在石英和/或侵蚀率分布不均匀的陡峭流域才需要。仅考虑表面生产的屏蔽,现有的屏蔽方法会引入与坡度有关的系统误差,这可能导致对地形和侵蚀速率之间关系的虚假解释。

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