含微气泡二相湍流边界层减阻理论计算

利用边界层中注入微气泡降低固体壁面摩擦阻力的方法是一项有实用价值且有待进一步研究的减阻技术.本文以含有微气泡的湍流边界层为研究对象,以气液二相流理论为基础,建立了二相湍流边界层控制方程,在对控制方程进行详细讨论的基础上,利用差分网格法进行了求解,计算结果表明微气泡具有明显的减阻效果.最后对影响减阻效果的因素进行了分析,并指出了今后的研究方向.     

基于大涡模拟的槽道微气泡减阻数值模拟

以大涡模拟和mixture两相流模型计算微气泡对湍流边界层的影响,以达到减小湍流边界层阻力的目的.数值模拟中,在同一水流速度和不同气泡喷射速度下,阻力随着气泡的喷射速度的增加而得到很大的减小,但当气泡量达到饱和时,减阻效果下降.数值模拟结果表明,在湍流边界层中注入微气泡是一种有效的减阻方式.     

二维船舶微气泡减阻数值模拟

为了研究来流雷诺数、微气泡浓度等因素对减少船舶摩擦阻力的影响,采用Lam-Bremhorst低雷诺拓展的K-ε模型,应用相间滑移算法,考虑了气-水两相的相间阻力、相间升力、相间压力和相间虚质量力以及气泡对湍流的作用,对二维平底型船舶,在船首底部喷射微气泡,进行了微气泡减阻的数值模拟.结果显示：提高边界层内气泡浓度是减阻的重要因素,而来流雷诺数过高对减阻不利.     

低速船舶微气泡减阻数值研究

为了研究船舶微气泡减阻规律,本文基于OpenFOAM中两相欧拉数值模型,对低速散货船进行微气泡减阻数值研究。对气液两相分别建立控制方程,考虑五种相间作用力及气泡聚合和破碎,采用考虑气泡影响的改进k-ε湍流模型,忽略自由面影响,采用叠模模型研究喷气量、气泡直径、航速及吃水等因素对船舶微气泡减阻的影响,分析气体体积分数、湍流粘度和气泡直径分布等。结果表明：微气泡可以同时减少船舶摩擦阻力、粘压阻力和总阻力;喷气量直接影响减阻率,喷气量越大,减阻率越高;较小气泡的平均气体体积分数较大且气体分布更均匀,同时湍流运动粘度较小,可以更有效减阻;气泡沿着流向会聚并,气泡越小聚并越剧烈;较高航速和小吃水更有利于减阻。     

微气泡层减阻的边界层模型计算

以流体中光滑平板为例,建立微气泡层覆盖平板的气液简单边界层模型,采用平板层流理论,对给定的气泡喷射参数和流体特性参数计算了微气泡层状态下平板的摩擦阻力,结果显示微气泡层对平板有明显减阻效果;最后给出了气体边界层的速度分布和剪切应力分布.     

控制气泡逸出技术的计算研究

采用欧拉方法的混合两相流模型及标准k-ε湍流模型,对采用控制气泡逸出技术的高速艇进行数值模拟,得到模型在喷气与不喷气状态下航行时的粘性流场,探讨不同控制气泡逸出方法对摩擦阻力减阻效果的影响,以寻求出使气泡在艇底保持及运动稳定性较好的最佳减阻措施。计算结果表明:在艇底加防溅条没有达到预期的减阻效果,优化后的新船型明显提高微气泡的减阻率。     

通过微气泡控制湍流边界层减阻的研究与进展

本文介绍了微气泡减阻的研究现状，阐述了湍流状态下微气泡减阻机理，对平板、轴对称体和船模等典型微气泡减阻试验做了简述后，总结了微气泡减阻理论研究的成果及相关的数学模型，最后介绍了微气泡减阻在实船上应用的现状和前景。     

平板微气泡减阻预报及影响因素研究

假定气-液两相流均匀混合,且微气泡在水流中存在滑移,运用流体计算软件Fluent中的混合多相流模型对平板微气泡减阻过程进行数值模拟,研究了微气泡流的减阻机理及喷气速度与主流速度之比、微气泡大小、空隙率分布等对水中运动平板减阻效果的影响规律,并指出微气泡减阻率为喷气速度与主流速度之比的非线性对数函数,且存在相对饱和喷气速度,同时建立了一个平板微气泡减阻率大小的预报模型,并从理论上对减阻效果进行了预报。     

基于OpenFOAM的平板微气泡减阻数值分析

本文基于OpenFOAM两相欧拉求解器(twoPhaseEulerFoam)对二维平板进行微气泡减阻数值模拟。模型直接求解两相N-S方程,同时采用标准k-ε湍流模型,并考虑两相间作用力的影响,通过求解界面输运方程来模拟气泡的聚并和破碎。将数值结果和Madavan[1]试验结果进行对比,验证了模型的可行性。分析了不同流速下气泡直径、通气速度、浮力对减阻率的影响,并且研究了气泡对边界处流体速度分布、气体体积分数的影响。从数值结果可以看出通气速度较大且气泡直径较小时,减阻效率高,并且浮力对减阻有一定影响。     

利用微气泡层减少平板阻力的边界层模型计算

以流体中光滑平板为例，建立微气泡层覆盖平板的气液简单边界层模型，采用平板层流理论，对给定的一系列气泡喷射速度参数和流体特性参数计算了微气泡状态下平板的摩擦阻力，结果显示微气泡对平板有明显减阻效果；最后给出了气体边界层的速度分布和剪切应力分布。     

Effect of microbubbles on the structure of turbulence in a turbulent boundary layer

The time-averaged velocity and turbulence intensity distributions were measured by a laser Doppler velocimeter in a turbulent boundary layer filled with microbubbles. The void fraction distribution was also measured using a fiber-optic probe. The velocity decreased in the region below 100 wall units with an increase in bubble density. This led to a decrease in the velocity gradient at the wall, which was consistent with a decrease in shearing stress on the wall. The turbulence intensity in the buffer layer increased at a low microbubble density, and then began to decrease with an increasing microbubble density. Based on the present measurements, the mechanism of turbulence reduction by microbubbles is discussed and a model is proposed. Received for publication on Dec. 3, 1999; accepted on April 18, 2000     

Reduction of skin friction by microbubbles and its relation with near-wall bubble concentration in a channel

Determination of the flow structure near the wall is essential for a clear insight into the phenomenon of skin friction reduction by microbubbles in a turbulent boundary layer. An important parameter, is the bubble concentration or void fraction in the wall region in drag-reducing conditions. The purpose of this paper is to show drag-reducing effects due to microbubbles in a water channel and, more importantly, to show the dependence of the drag-reduction values on the near-wall void fraction. A two-dimensional channel with an aspect ratio of 10 was specially built for this purpose with provisions for air injection through porous plates. Skin friction was directly measured by a miniature floating element transducer with a 5-mm circular sensing disk mounted flush on the top wall 67 channel-heights downstream of the injector. The wall friction in the presence of air bubbles was found to be reduced under the same bulk velocity when compared with the value without air. Detailed void fraction profiles across the channel were obtained by a sampling probe and a fiber-optic probe. Better collapse of the drag reduction data, independent of different profile shapes, was found when plotted against the near-wall void fraction than against a cross-sectional mean void fraction. While this dependence reconfirms that the phenomena are essentially inner-region dependent, the lack of influence of the bubble distribution patterns away from the wall implies lack of outer region influence.     

Influence of microbubble diameter and distribution on frictional resistance reduction

Investigations into frictional resistance reduction by microbubbles were carried out using a two-dimensional channel. The flow velocity and the amount of air injected were varied, and the frictional resistance reduction was measured. The frictional resistance reduction increased with increasing mean void ratio. When the bubble diameter was changed, the influence on frictional resistance reduction was negligible. The influence of bubble distribution near a wall was also investigated. Although it is thought that the influence of microbubbles near a wall is large, further investigations are required. Received: February 6, 2002 / Accepted: April 30, 2002 Acknowledgments. This research was supported by a special research program of Toyo University, SR239 Research Committee of the Shipbuilding Research Association of Japan, and the Research Project on Smart Control of Turbulence. The authors express their sincere gratitude for these supports. Address correspondence to: H. Kato (kato@eng.toyo.ac.jp)     

采用微气泡缩减高速船拖曳阻力(英文)

Ship hull form of the underwater area strongly influences the resistance of the ship.The major factor in ship resistance is skin friction resistance.Bulbous bows,polymer paint,water repellent paint(highly water-repellent wall),air injection,and specific roughness have been used by researchers as an attempt to obtain the resistance reduction and operation efficiency of ships.Micro-bubble injection is a promising technique for lowering frictional resistance.The injected air bubbles are supposed to somehow modify the energy inside the turbulent boundary layer and thereby lower the skin friction.The purpose of this study was to identify the effect of injected micro bubbles on a navy fast patrol boat(FPB) 57 m type model with the following main dimensions:L=2 450 mm,B=400 mm,and T=190 mm.The influence of the location of micro bubble injection and bubble velocity was also investigated.The ship model was pulled by an electric motor whose speed could be varied and adjusted.The ship model resistance was precisely measured by a load cell transducer.Comparison of ship resistance with and without micro-bubble injection was shown on a graph as a function of the drag coefficient and Froude number.It was shown that micro bubble injection behind the mid-ship is the best location to achieve the most effective drag reduction,and the drag reduction caused by the micro-bubbles can reach 6%-9%.     

Comparison of Microbubble and Air Layer Injection with Porous Media for Drag Reduction on a Self-propelled Barge Ship Model

Ship resistance issues are related to fuel economy, speed, and cost efficiency. Air lubrication is a promising technique for lowering hull frictional resistance as it is supposed to modify the energy in the turbulent boundary layer and thereby reduce hull friction. In this paper, the objective is to identify the optimum type of air lubrication using microbubble drag reduction (MBDR) and air layer drag reduction (ALDR) techniques to reduce the resistance of a 56-m Indonesian self-propelled barge (SPB). A model with the following dimensions was constructed: length L?=?2000 mm, breadth B?=?521.60 mm, and draft T?=?52.50 mm. The ship model was towed using standard towing tank experimental parameters. The speed was varied over the Froude number range 0.11–0.31. The air layer flow rate was varied at 80, 85, and 90 standard liters per minute (SLPM) and the microbubble injection coefficient over the range 0.20–0.60. The results show that the ship model using the air layer had the highest drag reduction up to a maximum of 90%. Based on the characteristics of the SPB, which operates at low speed, the optimum air lubrication type to reduce resistance in this instance is ALDR.     

基于积分法的粗糙壁面湍流边界层发展预测

壁面粗糙度对湍流的影响研究是流体动力学的热点问题。利用边界层积分法对零压力梯度下棱锥形粗糙壁面湍流边界层的发展进行预测分析。首先,以2个几何统计参数对棱锥形的粗糙形态进行描述,通过对试验数据的拟合分析,确定粗糙度函数的具体形式;然后,利用动量积分方程和壁面律求解出粗糙壁面湍流边界层厚度和局部摩擦系数沿流向的变化情况。计算结果与试验数据吻合较好,表明采用积分法预测粗糙壁面湍流边界层的发展精度较高,适于工程应用。     

非均衡湍流边界层脉动压力测试研究

通过建立非均衡湍流边界层脉动压力测试技术及可提供较高测试信噪比的低噪声风洞试验装置,采用表面贴装式硅微传声器线列阵,测量获得了不同压力梯度模型的湍流边界层脉动压力特性,压力梯度模型表面湍流边界层脉动压力低频平台区幅值增加3-5 dB;回归得到了非均衡湍流边界层流脉动压力频谱与Strauhal数及Re数和压力梯度相关的拟合模型,具有一定的适用性;压力梯度对湍流边界层脉动压力频率—波数谱的影响主要集中在300 Hz以下的低频段,传输波数附近峰脊区谱级增加3-5 dB。