首页 | 本学科首页   官方微博 | 高级检索  
     检索      


Measurements of fully developed turbulent flow in a trapezoidal duct
Authors:M M A Khalifa  A C Trupp
Institution:(1) Dept. of Mechanical Engineering, University of Manitoba, R3T 2N2 Winnipeg, Manitoba, Canada
Abstract:The turbulence characteristics of fully developed isothermal air flows through a symmetric trapezoidal duct were examined experimentally using Pitot tube and hot-wire anemometry over a Reynolds number range of 3.7–11.6×104. The measurements included local wall shear stress and the cross-sectional distributions of mean axial velocity, secondary velocities and Reynolds stresses. Four secondary flow cells were detected in a symmetric half of the duct. Although secondary velocity components were typically less than about 1% of the bulk axial velocity, their effect was especially pronounced on the distributions of turbulent kinetic energy and local wall shear stress.List of symbols a, b, c, d trapezoidal duct dimensions (Fig. 1) - A, B coefficients in log law (Table 1) - D h equivalent hydraulic diameter - f Darcy friction factor, (2D h /rhovU b 2 ) (dP/dx) - k turbulent kinetic energy per unit mass, 
$$\tfrac{1}{2}(\overline {u^2 }  + \overline {v^2 }  + \overline {w^2 } )$$
- k + dimensionless turbulent kinetic energy, k/(umacr *)2 - P static pressure - Re Reynolds number, rhovU b D h /mgr - s distance along inclined wall, measured from top corner (Fig. 1) - u, v, w fluctuating components of the velocities in the x, y, z directions - u +, v +, w + dimensionless turbulence intensities; radicu 2/umacr *, radicv 2/umacr *, radicw 2/umacr * - u * local friction velocity, (tau w /rhov)1/2 - umacr * average friction velocity, (¯gt/rhov)1/2 - Umacr axial mean velocity (time-average) - U b average mean axial velocity - U sec resultant of ¯V and ¯W, (¯V 2+¯ 2)1/2 - U + dimensionless velocity, Umacr/u * - ¯V, ¯W mean velocities in the y, z directions (secondary velocities) - x axial direction - y, 2 horizontal and vertical directions (Fig. 1) - z + dimensionless distance from (and normal to) a wall, zu */v - 
$$\hat z$$
distance from wall (at y=0) to location of maximum axial velocity - mgr laminar dynamic viscosity - v kinematic viscosity - rhov air density - tau w local wall shear stress - ¯tau w average of local wall shear stresses over all walls - ¯tau average wall shear stress, (dP/dx) (D h /4) - phgr corner angle of trapezoidal duct (Fig. 1) A version of this paper was presented at the 10th Symposium on Turbulence, University of Missouri-Rolla, Sept. 22–24, 1986
Keywords:
本文献已被 SpringerLink 等数据库收录!
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号