Interaction of two tandem deformable bodies in a viscous incompressible flow

被引:67
作者
Zhu, Luoding [1 ]
机构
[1] Indiana Univ Purdue Univ, Dept Math Sci, Indianapolis, IN 46202 USA
基金
美国国家科学基金会;
关键词
IMMERSED BOUNDARY METHOD; NAVIER-STOKES EQUATIONS; FLUID-STRUCTURE INTERACTION; SPECTRAL-PROJECTION METHOD; LEVEL-SET METHOD; CYLINDRICAL GEOMETRIES; INTERFACE METHOD; SOAP FILM; FILAMENTS; SIMULATION;
D O I
10.1017/S0022112009007903
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
Previous laboratory measurements oil drag of tandem rigid bodies moving in viscous incompressible fluids found that a following body experienced less drag than a leading one. Very recently a laboratory experiment (Ristroph & Zhang, Phys. Rev. Lett., vol. 101, 2008) with deformable bodies (rubble threads) revealed just the opposite the leading body had less drag than the following one. The Reynolds numbers in the experiment were around 10(4). To find out how this qualitatively different phenomenon may depend on the Reynolds number, a series of numerical simulations are designed and performed oil the interaction of a pair of tandem flexible flags separated by a dimensionless vertical distance (0 <= D <= 5.5) in a flowing viscous incompressible fluid at lower Reynolds numbers (40 <= Re <= 220) using the immersed boundary (IB) method. The dimensionless bending rigidity (K) over cap (b) and dimensionless flag mass density, 1.8 x 10(-5) <= (K) over cap (b) <= 1.8 x 10(-3), 0.8 <= (M) over cap <= 1.0. We used in our work are as follows: obtain all interesting result within these ranges of dimensionless parameters: when Re is large enough so that the flapping of the two flags is self-sustained, the leading flag has less drag than the following one; when Re is small enough so that the flags maintain two nearly static line segments aligned with the mainstream flow, the following flag has less drag than the leading one. The transitional range of Re separating the two differing phenomena depends on the value of ($) over cap (b). With Re ill this range, both the flapping and static states are observed depending on the separation distance D. When D is small enough, the flags are in the static state and the following flag has less drag; when D is large enough the flags are in the constant flapping state and the leading flag has less drag. The critical value of D depends oil (K) over cap (b).
引用
收藏
页码:455 / 475
页数:21
相关论文
共 67 条
[31]   Penalty immersed boundary method for an elastic boundary with mass [J].
Kim, Yongsam ;
Peskin, Charles S. .
PHYSICS OF FLUIDS, 2007, 19 (05)
[32]   REDUCTION OF WIND RESISTANCE AND POWER OUTPUT OF RACING CYCLISTS AND RUNNERS TRAVELING IN GROUPS [J].
KYLE, CR .
ERGONOMICS, 1979, 22 (04) :387-397
[33]   An immersed boundary method with formal second-order accuracy and reduced numerical viscosity [J].
Lai, MC ;
Peskin, CS .
JOURNAL OF COMPUTATIONAL PHYSICS, 2000, 160 (02) :705-719
[34]   Immersed interface methods for Stokes flow with elastic boundaries or surface tension [J].
Leveque, RJ ;
Li, ZL .
SIAM JOURNAL ON SCIENTIFIC COMPUTING, 1997, 18 (03) :709-735
[35]   THE IMMERSED INTERFACE METHOD FOR ELLIPTIC-EQUATIONS WITH DISCONTINUOUS COEFFICIENTS AND SINGULAR SOURCES [J].
LEVEQUE, RJ ;
LI, ZL .
SIAM JOURNAL ON NUMERICAL ANALYSIS, 1994, 31 (04) :1019-1044
[36]  
Li Z, 2006, FRONT APP M, V33
[37]   The immersed interface method for the Navier-Stokes equations with singular forces [J].
Li, ZL ;
Lai, MC .
JOURNAL OF COMPUTATIONAL PHYSICS, 2001, 171 (02) :822-842
[38]   The Karman gait: novel body kinematics of rainbow trout swimming in a vortex street [J].
Liao, JC ;
Beal, DN ;
Lauder, GV ;
Triantafyllou, MS .
JOURNAL OF EXPERIMENTAL BIOLOGY, 2003, 206 (06) :1059-1073
[39]   Mathematical foundations of the immersed finite element method [J].
Liu, Wing Kam ;
Kim, Do Wan ;
Tang, Shaoqiang .
COMPUTATIONAL MECHANICS, 2007, 39 (03) :211-222
[40]   An efficient spectral-projection method for the Navier-Stokes equations in cylindrical geometries - 1. Axisymmetric cases [J].
Lopez, JM ;
Shen, J .
JOURNAL OF COMPUTATIONAL PHYSICS, 1998, 139 (02) :308-326