首页 | 本学科首页   官方微博 | 高级检索  
     检索      


Investigation of the Geometrical Dispersion Regime in a Single Fracture Using Positron Emission Projection Imaging
Authors:Loggia  D  Gouze  P  Greswell  R  Parker  D J
Institution:(1) Laboratoire Tectonophysique (UMR 5568), Université Montpellier 2, CC MSE, 34095 Montpellier Cedex 5, France;(2) School of Earth Sciences, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK;(3) School of Physics and Astronomy, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK
Abstract:The transport properties of a natural fracture crossing a limestone block of 36 cm × 26 cm × 60 cm is studied using positron emission projection imaging. This non-invasive technique allows to measure the spatial distribution of the activity of a radioactive solution (here irradiated-copper-EDTA solution) within the fracture. The fracture aperture is measured from the spatial distribution of the activity as the fracture is completely filled with the tracer. The experiment consists in injecting the tracer at a constant flow rate in the plane of the fracture filled with an identical non-radioactive solution. Every 10 min, a two-dimensional grey scale image of the concentration field is recorded. The heterogeneity of the tracer distribution increases with time in relation with the spatial heterogeneity of the aperture field, and favours only slightly the region of larger aperture. The correlation length of the aperture distribution is larger than the correlation length of the concentration distribution of the tracer within the sample. Consequently, the concentration distribution cannot be modelled using a classical advection–dispersion equation; the mixing process has not reached a stationary Fickian dispersion regime in the finite size domain of the experiment. Nevertheless, the transversally averaged concentration profiles 
$$\overline c \left( x \right)$$
evaluated along the flow direction x rescale adequately with an advective variable 
$${x \mathord{\left/ {\vphantom {x {\overline U t}}} \right. \kern-\nulldelimiterspace} {\overline U t}} $$
, where 
$${\overline U }$$
is the mean velocity and t the time. This result is explained in the context of the geometrical dispersion regime where the mixing dispersion zone grows proportionally with time. Different approaches are proposed to characterise this anomalous dispersion regime.
Keywords:dispersion  fracture  positron emission tomography  anomalous dispersion
本文献已被 SpringerLink 等数据库收录!
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号