TY - GEN
T1 - Three-dimensional numerical simulation of hydrodynamic forces on an oblique cylinder in oscillatory flow
AU - Zhao, M.
AU - Cheng, L.
PY - 2010
Y1 - 2010
N2 - Sinusoidal oscillating flow around a circular cylinder at an oblique angle is investigated by direct numerical simulation. Simulations are carried out for oblique angles of α = 0°, 15°, 30°, 45° and 60°, Reynolds number Re = 2000 and KC number ranging from 6.75 to 30. The oblique angle is defined as the angle between the flow direction and the transverse plane of the cylinder (see Fig. 1). The predicted vortex shedding regimes agree well with those found from physical experiments. When the KC number is close to the boundary value of KC number between two vortex shedding regimes (KC = 6.75, 15, 20 and 30) the correlation of sectional force in cylinder's spanwise direction is very weak and the time series of the transverse force contains two or three predominant frequencies, implying the flow switches from one mode to another continuously. The span-wise correlation factor obtained according to the sectional transverse force is always close to 1 for single-mode flows. Comparison between the numerical results of α=0° and those of α≠0° shows that the independent principle is applicable for the calculated KC number range and the oblique angle ( α≤60°). The oblique angle has little effect on mode-averaged transverse force and the in-line force coefficients.
AB - Sinusoidal oscillating flow around a circular cylinder at an oblique angle is investigated by direct numerical simulation. Simulations are carried out for oblique angles of α = 0°, 15°, 30°, 45° and 60°, Reynolds number Re = 2000 and KC number ranging from 6.75 to 30. The oblique angle is defined as the angle between the flow direction and the transverse plane of the cylinder (see Fig. 1). The predicted vortex shedding regimes agree well with those found from physical experiments. When the KC number is close to the boundary value of KC number between two vortex shedding regimes (KC = 6.75, 15, 20 and 30) the correlation of sectional force in cylinder's spanwise direction is very weak and the time series of the transverse force contains two or three predominant frequencies, implying the flow switches from one mode to another continuously. The span-wise correlation factor obtained according to the sectional transverse force is always close to 1 for single-mode flows. Comparison between the numerical results of α=0° and those of α≠0° shows that the independent principle is applicable for the calculated KC number range and the oblique angle ( α≤60°). The oblique angle has little effect on mode-averaged transverse force and the in-line force coefficients.
UR - http://www.scopus.com/inward/record.url?scp=84857005369&partnerID=8YFLogxK
M3 - Conference Paper
AN - SCOPUS:84857005369
SN - 9781617829130
T3 - 17th Australasian Fluid Mechanics Conference 2010
SP - 47
EP - 50
BT - 17th Australasian Fluid Mechanics Conference 2010
T2 - 17th Australasian Fluid Mechanics Conference 2010, 17AFMC
Y2 - 5 December 2010 through 9 December 2010
ER -