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A viscoelastic strain energy principle expressed in fold-thrust belts and other compressional regimes

机译:褶皱-冲断带和其他压缩形式表达的粘弹性应变能原理

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A mathematical folding theory for stratified viscoelastic media in layer parallel compression is presented. The second order fluid, in slow flow, is used to model rock rheological behavior because it is the simplest nonlinear constitutive equation exhibiting viscoelastic effects. Scaling and non-dimensionalization of the model system reveals the presence of Weissenberg number (Wi), defined as a ratio of time scales ι~*/(H~*/V~*). V~*/H~* is the strain rate (s~(-1)) imposed by an assumed far field velocity V~* acting on a layer of thickness H~*, while ι~* (s) is related to the relaxation of normal stresses. Our most significant finding is a transitional behavior as Wi → 1/2, which is independent of the viscosity contrast. A change of variables shows that lengths associated with this transition are scaled by a parameter α = [(1-2Wi)/(1 + 2Wi)]~(1/2), which is inversely proportional to local strain energy. On this basis a scaling law representing a distribution of non-dimensional wavelengths (wavelength/layer thickness) is derived. Geologically this is consistent with a transition from folding to faulting, as observed in fold-thrust belts. Folding, a distributed deformation scaling as Wi~(-1), is found to be energetically favored at non-dimensional wavelengths ranging from about three to seven. Furthermore, the transition from folding to faulting, a localized deformation scaling as (α Wi)~(-1), is predicted at a non-dimensional wavelength of about seven. These findings are consistent with measurements of thrust sheets in the Sawtooth Mountains of western Montana, USA and other fold-thrust belts. A review of the literature reveals a similar distribution of non-dimensional wavelengths spanning a wide range of observational scales in compressional deformation. Specific examples include lithospheric scale folding in the central Indian Basin and microscopic scale failure of ice columns between splay microcracks in laboratory studies.
机译:提出了层状平行压缩中分层粘弹性介质的数学折叠理论。由于它是表现粘弹性效应的最简单的非线性本构方程,因此使用慢速流动的二阶流体来模拟岩石流变行为。模型系统的缩放和无量纲化揭示了魏森贝格数(Wi)的存在,其定义为时间标度η〜* /(H〜* / V〜*)的比率。 V〜* / H〜*是假设的远场速度V〜*作用在厚度为H〜*的层上而施加的应变率(s〜(-1)),而η〜*(s)与放松正常压力。我们最重要的发现是Wi→1/2的过渡行为,这与粘度对比无关。变量的变化表明,与该转变相关的长度由参数α= [(1-2Wi)/(1 + 2Wi)]〜(1/2)缩放,该参数与局部应变能成反比。在此基础上,得出了表示无量纲波长(波长/层厚度)分布的缩放定律。在地质学上,这与从褶皱冲断带中观察到的从褶皱到断层的过渡是一致的。发现在约3至7的无量纲波长上在能量上有利于折叠,即Wi-(-1)的分布式变形比例。此外,从折叠到断层的转变,局部变形定标为(αWi)〜(-1),是在约7的无量纲波长处预测的。这些发现与美国西部蒙大拿州的锯齿山及其他褶皱-冲断带的逆冲板测量结果一致。对文献的回顾揭示了在压缩形变中跨大范围观察尺度的无量纲波长的相似分布。具体的例子包括实验室研究中印度中部盆地的岩石圈尺度折叠和张开微裂纹之间冰柱的微观尺度破坏。

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