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Assessment of open thermodynamic system concepts for fluviokarst temperature calculations – an example, the Cent-Fonts resurgence (Hérault, France)

机译:评估用于潮热岩溶温度计算的开放式热力学系统概念–例如,Cent-Fonts回潮(法国,埃罗)

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摘要

We propose to assess the error done when temperature is considered as a conservative tracer in fluviokarst studies. As a matter of fact, heat exchanges occur between karstic Conduit System (CS) and Porous Fractured Matrix (PFM) that prevents from using this approximation without caution. The conservative tracer approximation boils down to consider the cooling of CS water by PFM flow in an open thermodynamic system where the CS is bounded by an Adiabatic Wall (AW). The resulting CS water temperature contrasts with the one obtained from more complete models (CW), which also take into account heat conduction within the CS, within the PFM, and from the CS to PFM through CS a Conductive Wall. In order to assess first orders of this error, the dimensionless equations, characteristic of CS cooling by PFM, have been solved thanks to Alternate Finite Difference Implicit methods both in AW and CW configurations. Four groups of dimensionless numbers appear in the various terms of energy and mass equations among which the Peclet and Reynolds numbers depict the large morphologic and hydrologic variability of natural karstic systems. A parametric exploration of the differences between AW and CW models has then been conducted vs. Peclet numbers (Pe numbers varying from 106 to 109, at constant CS Reynolds number) and vs. Reynolds numbers (Red varying from 103 to 107, at constant Peclet number). The error curves bound finite volumes in the Peclet–Reynolds space that converge uniformly to zero for the extreme values of these parameters. However, for Peclet and Reynolds numbers characteristic of realistic fluviokarst configurations, the errors reach finite values, that give first order information assessing the error done by considering temperatures as conservative tracers. Maximum relative errors around 10−2 (in fact 0.0092) have been found varying Pe; while it remained slightly lower than 0.7 × 10−2 varying Red. An illustrative example of the temperature conservative tracer AW approximation is presented with the data obtained from the main morphologic and hydrologic properties of the Cent–Font resurgence (Hérault, France). According to the results, the error reached at the output of the fluviokarst is 0.00613 (for Pe = 1.4993 × 108 and Red = 4.2969 × 104). When rescaled to the physical domain, this error leads to a temperature difference of 1.77 K between the CW and AW configurations.
机译:我们建议评估在潮汐岩溶研究中将温度视为保守示踪剂时所做的误差。事实上,在岩溶导管系统(CS)和多孔裂缝性基质(PFM)之间发生热交换,从而在没有谨慎的情况下阻止使用这种近似。保守的示踪剂近似可以归结为考虑在开放热力学系统中CS受到绝热壁(AW)限制的情况下,PFM流对CS水的冷却。产生的CS水温与从更完整的模型(CW)获得的水温形成对比,后者也考虑了CS内部,PFM内以及通过CS到CS到PFM的热传导。为了评估该误差的一阶,通过在AW和CW配置中使用交替有限差分隐式方法,已解决了无因次方程,即通过PFM进行CS冷却的特性。在能量和质量方程的各个术语中出现了四组无量纲数,其中Peclet和Reynolds数描述了自然岩溶系统的大形态和水文变异性。然后,对AW和CW模型之间的差异进行了参数化探索,即与Peclet数(在恒定的CS雷诺数下,Pe数在106到109之间变化)和与Reynolds数(在恒定的Peclet时,红在103到107之间变化)数)。误差曲线限制了Peclet-Reynolds空间中的有限体积,对于这些参数的极值,该体积均匀收敛于零。但是,对于实际的潮汐岩溶构造的Peclet和Reynolds数特征,误差达到有限值,从而通过将温度视为保守示踪剂,从而给出了一阶信息来评估误差。已经发现,随着Pe的变化,最大相对误差约为10−2(实际上是0.0092)。而它仍然略低于0.7×10-2的红色。通过从Cent-Font回潮的主要形态和水文特性(法国埃罗特)获得的数据,给出了温度守恒示踪剂AW近似的一个说明性示例。根据结果​​,在液流岩溶输出处达到的误差为0.00613(对于Pe = 1.4993×108和Red = 4.2969×104)。当重新缩放到物理域时,此错误导致CW和AW配置之间的温度差为1.77K。

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