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A new model for shallow viscoelastic free-surface flows forced by gravity on rough inclined bottom

机译:重力作用在粗糙斜底上的浅层粘弹性自由表面流新模型

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A thin-layer model for shallow viscoelastic free-surface gravity flows on slippery topographies around a flat plane has been derived recently in [Bouchut-Boyaval, M3AS (23) 2013]. We show here how the model can be modified for flows on rugous topographies varying around an inclined plane. The new reduced model extends the scope of one derived in [Bouchut-Boyaval, M3AS (23) 2013]. It is one particular thin-layer model for free-surface gravity flows among many ones that can be formally derived with a generic unifying procedure. Many rheologies and various shallow flow regimes have already been treated within a single unified framework in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013]. The initial full model used here as a starting point is however a little different to one used in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], although the new thin-layer model is very similar to the one derived therein. Precisely, here, the bulk dissipation (due to e.g. viscosity) is neglected from the beginning, like in [Bouchut-Boyaval, M3AS (23) 2013]. Moreover, unlike in [Bouchut-Boyaval, HAL-ENPC (00833468) 2013], we perform here numerical simulations. The interest of the extension is illustrated in a physically interesting situation where new stationary solutions exist. To that aim, the Finite-Volume method proposed in [Bouchut-Boyaval, M3AS (23) 2013] needs to be modified, with an adequate discretization of the new source terms. Interestingly, we can also numerically exhibit an apparently new kind of “roll-wave” solution.
机译:最近在[Bouchut-Boyaval,M3AS(23)2013]中推导了在光滑的地形上围绕平坦平面的浅层粘弹性自由表面重力流的薄层模型。我们在这里展示如何针对在倾斜平面周围变化的崎top地形上的流动修改模型。新的简化模型扩展了[Bouchut-Boyaval,M3AS(23)2013]中衍生的模型的范围。它是一种用于自由表面重力流的特殊的薄层模型,可以通过通用的统一程序正式导出。在[Bouchut-Boyaval,HAL-ENPC(00833468)2013]中,已经在一个统一的框架内处理了许多流变学和各种浅流形式。尽管新的薄层模型与其中衍生的模型非常相似,但此处用作起点的初始完整模型与[Bouchut-Boyaval,HAL-ENPC(00833468)2013]中使用的模型有所不同。确切地说,在这里,就像[Bouchut-Boyaval,M3AS(23)2013]一样,从一开始就忽略了整体散逸(由于粘度)。此外,与[Bouchut-Boyaval,HAL-ENPC(00833468)2013]不同,我们在此处执行数值模拟。在存在新的固定解的物理情况下,说明了扩展的兴趣。为此,需要修改[Bouchut-Boyaval,M3AS(23)2013]中提出的有限体积方法,并充分离散化新的源术语。有趣的是,我们还可以从数字上展示一种看似新型的“滚波”解决方案。

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