On the sources of aerodynamic forces: Steady flow around a cylinder or a sphere

被引:15
作者
Chang, CC
Lei, SY
机构
[1] Institute of Applied Mechanics, College of Engineering, National Taiwan University
来源
PROCEEDINGS OF THE ROYAL SOCIETY A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES | 1996年 / 452卷 / 1954期
关键词
D O I
10.1098/rspa.1996.0128
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
In the present study, we analyse various force contributions for viscous compressible how around a finite body. Aerodynamic forces are found to be directly related to fluid elements of non-zero vorticity and density gradient. Since the aerodynamic range is large, relative importance of various sources should, however, be assessed under different flow conditions. The effect of compressibility is our major concern. Let rho denote the density, u velocity, and omega vorticity. It is demonstrated that for largely separated hows about bluff bodies, there are two major source elements: R(e)(x) = -1/2u(2) del rho .del phi and V-e(x) = -rho u x omega .del phi, where phi is an acyclic potential, generated by the solid body moving with unit velocity in the negative direction of the force considered. All the physical quantities are nondimensionalized. In particular, we consider steady flows around a circular cylinder or a sphere in a transonic-to-supersonic regime. Numerical results indicate that these two elements contribute to 95% or more of the total drag for all the cases under consideration. For flows around either a cylinder or a sphere, it is found that the source elements are concentrated on four regions; they are the front shock region, the boundary layer in front of the body, the shear layer separating from the shoulder of the body, and a region of expansion/compression upstream of the separated shear layer. The separated shear layer is found to be an important source fdr both elements R(e)(x) and V-e(x). The region of expansion and the front shock contribute largely and positively to the drag through R(e)(x), while the front boundary layer contributes largely and negatively to the drag through V-e(x). Other how structures such as the trailing shock wave and the regions of eddying motion, including the wake and a region of dead air behind the body are shown to play relatively much less significant roles in contributing to the drag.
引用
收藏
页码:2369 / 2395
页数:27
相关论文
共 23 条
[1]  
Batchelor GK, 2000, An Introduction to Fluid Dynamics
[2]   POTENTIAL FLOW AND FORCES FOR INCOMPRESSIBLE VISCOUS-FLOW [J].
CHANG, CC .
PROCEEDINGS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1992, 437 (1901) :517-525
[3]   An analysis of aerodynamic forces on a delta wing [J].
Chang, CC ;
Lei, SY .
JOURNAL OF FLUID MECHANICS, 1996, 316 :173-196
[4]   THE AERODYNAMIC PERFORMANCE OF SMALL SPHERES FROM SUBSONIC TO HIGH SUPERSONIC VELOCITIES [J].
CHARTERS, AC ;
THOMAS, RN .
JOURNAL OF THE AERONAUTICAL SCIENCES, 1945, 12 (04) :468-476
[5]  
Dyke M. V., 1982, ALBUM FLUID MOTION
[7]   LOWER-UPPER IMPLICIT SCHEMES WITH MULTIPLE GRIDS FOR THE EULER EQUATIONS [J].
JAMESON, A ;
YOON, S .
AIAA JOURNAL, 1987, 25 (07) :929-935
[8]  
Landau L. D., 1987, FLUID MECH-SOV RES
[9]  
Launder B. E., 1974, Computer Methods in Applied Mechanics and Engineering, V3, P269, DOI 10.1016/0045-7825(74)90029-2
[10]   TURBULENCE MODELING FOR COMPUTATIONAL AERODYNAMICS [J].
MARVIN, JG .
AIAA JOURNAL, 1983, 21 (07) :941-955