论文标题
超临界水流的新型两相法
Novel two-phase method for supercritical water flow
论文作者
论文摘要
临界点以外的相图研究中的当前复兴已经质疑超临界流体作为具有不同特性的单个相的常规信念。在同一条线上,已经提出了一种新型的两相方法来研究以传热恶化(HTD)现象的超临界流量。流体(VOF)多相模型的体积已被用于分析流量,模拟结果合理地预测了壁温峰。此外,不同轴向位置的速度和湍流动能谱解释了HTD的出现,并且与现有的数值方法相当。此外,论文中提出的定量分析阐述了定性理解。热物理特性的参数研究表明,密度变化是超临界流中HTD的主要原因。因此,根据这一结论,提出的研究重点是由于密度变化而产生的力。该技术使我们对超临界流的整体图片进行了整体图像。它导致了这样的推断,即对于不存在HTD效应,浮力和惯性力在整个流中必须具有相当的幅度。此外,伪阶段变化模型通过向我们提供量分数数据来超越现有研究。该变量的映射表明,在HTD位点附近的墙壁附近,较轻的相位的厚度突然跳跃,这也反映为无量距性的两相厚度(P)图中的最大值。然而,这种观察仅限于浮力引起的HTD。最后,为计算两相厚度(H)值的理论表达已被概念化,该值可以用作超临界流中的基本长度尺度,因为它标志着壁附近的最高属性梯度的区域。
The current resurgence in the phase diagram study beyond the critical point has questioned the conventional belief of supercritical fluid as a single phase with varying properties. On the same line, a novel two-phase approach has been proposed to study the supercritical flow with heat transfer deterioration (HTD) phenomena. The Volume of Fluid (VOF) multiphase model has been used to analyze the flow, and the simulation result reasonably predicts the wall temperature peaks. Moreover, the velocity and turbulent kinetic energy profiles for different axial locations explain the occurrence of HTD, and it is on par with the pre-existing numerical method. Besides, the quantitative analysis presented in the paper expounds on qualitative understanding. The parametric study of the thermophysical properties revealed that the density variation is the primary cause of HTD in supercritical flows. So banking on this conclusion, the propounded study focuses on the forces generated due to the density variation. This technique equips us with a holistic picture of the supercritical flows. It leads to the inference that for no HTD effects to be present, buoyancy and inertia forces have to be of comparable magnitude throughout the flow. In addition, the pseudo phase change model outclasses the existing research by rendering us the volume fraction data. Mapping of this variable reveals a sudden jump in the lighter phase's thickness near the wall at the site of HTD, which is also reflected as a maximum in the nondimensional two-phase thickness (P) plot. Nevertheless, this observation is only restricted to HTD caused by buoyancy. In the end, a theoretical expression has been conceptualized for computing the two-phase thickness (h) value, which can serve as a fundamental length scale in supercritical flows as it marks the region of highest property gradient near the wall.