陈湘, 杨铸涛, 王党朝. 非旋转条件下圆柱形底部中心开孔容器中液体的非定常流动特性[J]. 内江师范学院学报, 2023, 38(10): 65-73,92. DOI: 10.13603/j.cnki.51-1621/z.2023.10.011
    引用本文: 陈湘, 杨铸涛, 王党朝. 非旋转条件下圆柱形底部中心开孔容器中液体的非定常流动特性[J]. 内江师范学院学报, 2023, 38(10): 65-73,92. DOI: 10.13603/j.cnki.51-1621/z.2023.10.011
    CHEN Xiang, YANG Zhutao, WANG Dangchao. Study on unsteady flow characteristics of liquid in a cylindrical container with a central opening at the bottom under non rotating conditions[J]. Journal of Neijiang Normal University, 2023, 38(10): 65-73,92. DOI: 10.13603/j.cnki.51-1621/z.2023.10.011
    Citation: CHEN Xiang, YANG Zhutao, WANG Dangchao. Study on unsteady flow characteristics of liquid in a cylindrical container with a central opening at the bottom under non rotating conditions[J]. Journal of Neijiang Normal University, 2023, 38(10): 65-73,92. DOI: 10.13603/j.cnki.51-1621/z.2023.10.011

    非旋转条件下圆柱形底部中心开孔容器中液体的非定常流动特性

    Study on unsteady flow characteristics of liquid in a cylindrical container with a central opening at the bottom under non rotating conditions

    • 摘要: 在不考虑旋转情况下,建立了流体沿静止的圆柱形容器底部中心开孔处下漏问题的非定常微分方程,并分别采用准定常近似、非定常逐级逼近和精确解等方法,得到了液面距底部高度与液面初始高度、液面降速、圆孔处液体的流速、流量等随时间变化的关系,深入研究了液体的非定常流动特性.结果表明,逐级逼近法求出的非定常流动解中,液面折合高度对应的理论时刻与准定常流动解之间存在一个比例系数βn,该系数中β与圆柱体容器直径和小孔直径之比ε相关.以水、饱和盐水、酒精为介质的实验结果,很好地验证了液面的折合高度Z'与时间t呈现良好的线性关系t=k'Z'.且由于非定常效应,实际比例系数k'大于准定常计算值k;在本文的直径比范围内,k'/k均在1.5左右,与液体种类呈弱相关.相同ε下,三种液体的k'和非定常近似级数n分别具有一致性;但随ε变化,二者分别与ε2和ε4成正比关系.WTBZ并基于实验数据得到了液面折合高度与对应实际时刻的数值解析式.

       

      Abstract: Without considering the rotation, the differential equation of fluid leakage along the center opening at the bottom of a stationary cylindrical container is established, and the relationship between the height of the liquid surface from the bottom and the initial height and time of the liquid surface, as well as the relationship between the liquid surface deceleration, the liquid velocity and flow rate at the circular hole with time are obtained by using quasi steady approximation, unsteady step-by-step approximation, and unsteady accurate analytical solution. The results show that there is a proportional coefficient βn between the theoretical time corresponding to the reduced height of the liquid surface and the quasi steady flow solution in the unsteady flow solution obtained by the step-by-step approximation method, and the coefficient β is related to the ratio ε of the diameter of the cylindrical container to the diameter of the small hole. The experimental results using water, saturated brine and alcohol as media are well verified the good linear relationship t=k'Z' of liquid surface height Z' with time t. Because of the unsteady effect, the actual ratio coefficient k' is greater than the quasi steady calculated value k, and within the diameter ratio range of this paper, k'/k is about 1.5, which is weakly related to the type of liquid. Under the same ε, the k' and n are also consistent, but with ε changes, they are proportional to ε2 and ε4 respectively. Based on the experimental data, the numerical analytical expressions of, and, and the actual time corresponding to the reduced height of the liquid surface are obtained.

       

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