999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

Reply to Discussion on “Analysis of Bingham fluid radial flow in smooth fractures”

2021-04-01 04:06:30LingchoZouUlfknssonVldimirCvetkovic

Lingcho Zou, Ulf H?knsson, Vldimir Cvetkovic

a Division of Resources,Energy and Infrastructure,Department of Sustainable Development,Environmental Science and Engineering,Royal Institute of Technology,Stockholm,10044, Sweden

b Division of Soil and Rock Mechanics, Department of Civil and Architectural Engineering, Royal Institute of Technology, Stockholm,10044, Sweden

c Skanska AB, Stockholm,11274, Sweden

Keywords:Rock grouting Radial flow Bingham fluid Approximation solution

ABSTRACT Recently, Hoang et al. (2021) discussed our paper Zou et al. (2020). In our paper, we made a statement that Dai and Bird(1981)’s solution for two-dimensional (2D) radial Bingham fluid flow between parallel plates violates mass balance.Hoang et al.pointed out that Dai and Bird(1981)’s solution does not violate the mass balance because Dai and Bird (1981)’s solution and our analysis are based on different assumptions, i.e. with consideration of the vertical velocity component in the continuity equation or not,which leads to two different approximation models. In this sense, the mass balance of Dai and Bird(1981)’s solution should not be checked using our solution as a reference. In this reply, we add remarks on the two approximation models and their implication for rock grouting analysis. The discussion by Hoang et al. and this reply are helpful to thoroughly eliminate the existing confusion regarding the two solutions in the rock grouting research community.

1. Introduction

We appreciate Hoang et al. (2021) for their interest and efforts made for the discussion on our paper ‘Analysis of Bingham fluid radial flow in smooth fractures’.The solution of Bingham fluid flow in smooth fractures is the basis for theoretical analysis of cement grouting in rock fractures.In our paper(Zou et al.,2020),we made a statement that Dai and Bird(1981)’s solution for two-dimensional(2D) radial Bingham fluid flow between parallel plates violates mass balance. Hoang et al. (2021) pointed out that Dai and Bird(1981)’s solution does not violate mass balance because Dai and Bird (1981)’s solution and our analysis are based on different assumptions, i.e. with consideration of the vertical velocity component in the continuity equation or not,which leads to two different approximation models.

In the literature, the confusion regarding Dai and Bird (1981)’s solution and its application to rock grouting has been raised because no explicit mathematical models, i.e. the governing equations, were presented either in Dai and Bird (1981) nor in the following rock grouting literature,e.g.Gustafson et al.(2013).In the discussion by Hoang et al. (2021), the two approximation models with associated solutions were clearly summarized in their Eqs.(5)-(7), which is helpful for clarification. If Dai and Bird (1981)’s solution is viewed as a different model from ours, its mass balance should not be checked using our solution as a reference; in this sense, our statement that Dai and Bird (1981)’s solution violates mass balance is indeed unnecessary as pointed out by Hoang et al.(2021).

The results of the two models were compared for different Bingham numbers (Bn) in Hoang et al. (2021), showing that the difference of results between the two types of models is not significant in general,which is consistent with our comparison results of the two types of rock grouting solutions shown in Figs.6 and 7 in Zou et al. (2020).

In this reply,we would like to add the following remarks on the two approximation models and their implication for rock grouting analysis.The discussion by Hoang et al.(2021)and this reply should be helpful to eliminate the existing confusion regarding the two solutions in the rock grouting research community.

2. Approximation for the complexity

We would like to emphasize that cement grouting in rock fractures is a complex process involving complex fluid flow in complex geometrical structures. Simplified models for radial flow of Bingham fluids in smooth fractures were used to develop theoretical models for rock grouting analysis.

The radial velocity is dependent on the radius in the radial flow configuration,and it reduces with the increasing radius.This means that the Reynolds number is not constant:it can be very high near the inlet (i.e. injection borehole) and very small near the outlet.Therefore, in principle, the kinematical effects should not be ignored to capture the realistic physical process. However, it is impossible to analytically solve the full continuity and momentum equations at present. The asymptotic expansion method has been used to obtain approximation solutions for radial flow of Bingham fluids in the configuration of squeeze flow (e.g. Muravleva, 2017).The model(Eqs.(5)-(7))presented in the discussion by Hoang et al.(2021) is the zero-order approximation of the continuity and momentum equations.The model presented in Zou et al.(2020)is also the zero-order approximation by further omitting the vertical velocity component in the continuity equation. Both models are approximations of realistic kinematical effects, as discussed by Muravleva (2017).

The shape of the plug flow region varies in the two different approximation models. For instance, the plug flow region in the model presented in Zou et al. (2020) is independent of the radius;in the model(Eqs.(5)-(7))presented in Hoang et al.(2021),the plug flow region increases with the radius. In higher orders of approximation models, the plug flow region can be more complex (e.g.Muravleva, 2017). The reason for the obtained different shapes of plug flow region in the two approximation models is indicated in the discussion by Hoang et al. (2021), which is due to the application of different boundary conditions for the shear stress. Specifically, we use the boundary condition on the surface of the plug flow region,while the other model sets shear stress equal to zero in the middle of the fracture aperture in the plug flow region. We think that the shear stress in the plug region is undefined according to the definition of the Bingham model,which only defines that the shear stress is below the yield stress in the plug flow region (it implies that the shear stress can be any value below the yield stress in the plug flow region)(see Eq. (3)in Zou et al. (2020)or Eqs. (1)and(2)in Hoang et al.(2021)).Moreover,the Bingham model is an idealized rheological model and its validity for any realistic fluids remains an open question(Barnes,1999).Therefore,the real shape of the plug flow region for realistic fluids/grouts or even the existence of a rigid plug flow region remains unknown at this point.

3. Implication for rock grouting analysis

With the understanding that Dai and Bird(1981)’s solution and our analysis are two separate approximation models, we should clarify that the two types of analytical solutions for rock grouting,presented in Gustafson et al. (2013) and Zou et al. (2020), respectively, are both approximation solutions, i.e. neither of them is an exact solution.However,as noted in the discussion by Hoang et al.(2021),the solution presented in Zou et al.(2020)is much simpler compared to that based on Dai and Bird (1981)’s solution. More importantly, the solution presented in Zou et al. (2020) is more relevant to the boundary condition commonly applied in rock grouting with controlled injection pressure,where the solution for the pressure is explicit with respect to the boundary pressures(see Eqs. (A3) and (A4) in Zou et al. (2020)). In contrast, Dai and Bird(1981)’s solution is more relevant to the boundary condition of known constant flowrate, where the solution for the pressure needs to be solved from the flowrate equation,i.e.Eq.(4)in Hoang et al. (2021). Considering that the difference between solutions of the two models is relatively small(see Fig.6 in Hoang et al.,2021)and that the predicted grout propagation lengths using the two models are very close (see Figs. 6 and 7 in Zou et al., 2020), it is recommended using the simpler solution presented in Zou et al.(2020)for rock grouting analysis in practice.

In summary, the two types of approximation models are both based on restrictive assumptions. They are at best applicable only for scoping calculations and some degree of uncertainty for analysis of rock grouting in engineering projects has to be expected. Validation of the two models using more rigorous direct numerical simulations (e.g. using an augmented Lagrangian approach or Uzawa/projection method) or physical experiments (e.g. Shamu et al., 2020) might be possible at small scales, but it remains unavailable at engineering application scales. Validation of the analytical models and development of more reliable numerical tools for design and operation of rock grouting applications are important topics for future studies.

Declaration of competing interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

主站蜘蛛池模板: 一级毛片高清| 色视频久久| 2021国产精品自产拍在线| 综合社区亚洲熟妇p| 日韩欧美国产成人| 亚洲青涩在线| 久草青青在线视频| 亚洲AV色香蕉一区二区| 国产福利在线免费观看| 欧美亚洲国产精品久久蜜芽| 欧美国产成人在线| a级毛片毛片免费观看久潮| 9啪在线视频| 国产成人精品在线1区| 福利国产在线| 亚洲成a人片| 日本成人福利视频| 亚洲高清无码久久久| 在线99视频| 一区二区三区精品视频在线观看| 国产精品女人呻吟在线观看| 亚洲精品中文字幕无乱码| 亚洲成a∧人片在线观看无码| 国产精品久久精品| 中文字幕第1页在线播| 丁香六月激情综合| 在线色国产| 欧美亚洲欧美区| 国产va在线观看免费| 久久国产精品娇妻素人| 亚洲精品无码成人片在线观看| 亚欧成人无码AV在线播放| 免费a级毛片18以上观看精品| 日本久久网站| 亚洲视频欧美不卡| 亚洲人成高清| 一级毛片免费不卡在线视频| 中文天堂在线视频| 国产小视频在线高清播放| 国产微拍一区二区三区四区| 波多野结衣无码AV在线| 成人免费一区二区三区| AⅤ色综合久久天堂AV色综合| 亚洲欧美成人在线视频| 日a本亚洲中文在线观看| 国产99视频精品免费观看9e| 日韩麻豆小视频| 91欧美在线| 欧美日韩专区| 欧美一级在线| 日本91在线| 久久天天躁狠狠躁夜夜躁| 婷婷亚洲天堂| 国产亚洲欧美日韩在线观看一区二区 | 毛片免费在线视频| 欧美性天天| yy6080理论大片一级久久| 国产精品无码翘臀在线看纯欲| 国产日韩欧美一区二区三区在线 | 精品无码一区二区三区电影| 伦精品一区二区三区视频| 青青操视频免费观看| 人禽伦免费交视频网页播放| 波多野结衣视频网站| 免费在线看黄网址| 国产男女免费视频| 久一在线视频| 91久久偷偷做嫩草影院电| 青草视频免费在线观看| 成人精品视频一区二区在线| 国禁国产you女视频网站| 欧美专区在线观看| 综合色在线| 无遮挡一级毛片呦女视频| 欧美国产中文| 国产尤物在线播放| 精品人妻一区二区三区蜜桃AⅤ| 国产女人喷水视频| 久久人人97超碰人人澡爱香蕉 | 色亚洲激情综合精品无码视频| 黄色福利在线| 国产成人一区免费观看|