THE PHYSICAL MECHANISM OF TRANSITION IN BLUFF BODY WAKES

By M. Thompson, T. Leweke, Charles H. K. Williamson. 2001

157 citations recorded by the source corpus.

Subfields: Aerospace Engineering, Computational Mechanics, Environmental Engineering

View Paper: https://www.semanticscholar.org/paper/35a444717e1c2fb269e1e2478322a605c3d7c949

How researchers see this paper

The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.

In Aerospace Engineering

1. L. E. Jones
2. Richard D. Sandberg
3. Neil D. Sandham
4. Julio Romano Meneghini
5. Gregory J. Sheard
6. Kerry Hourigan
7. M. Fitzgerald
8. Spencer J. Sherwin

In Computational Mechanics

1. L. E. Jones
2. Richard D. Sandberg
3. Lars Davidson
4. Julio Romano Meneghini
5. B. Carmo
6. Fujun Wang
7. Lixia Qu
8. Shia-Hui Peng

In Environmental Engineering

1. Lars Davidson
2. Fujun Wang
3. Lixia Qu
4. Shia-Hui Peng
5. Gregory J. Sheard
6. B. Carmo
7. Julio Romano Meneghini
8. Spencer J. Sherwin

Citations in the corpus

• Cylinders with square cross-section: wake instabilities with incidence angle variation (2009, background): “For instance, Karniadakis & Triantafyllou (1992); Barkley & Henderson (1996); Thompson et al. (1996); Williamson (1996); Leweke & Williamson (1998); Thompson, Leweke & Williamson (2001b) investigated a circular cylinder, Sheard (2007) investigated an elliptical cylinder, Ryan, Thompson & Hourigan ”
• From spheres to circular cylinders: the stability and flow structures of bluff ring wakes (2003, methodology): “The present numerical technique has been successfully applied to the wake of a circular cylinder (Thompson et al. 2001b).”
• Secondary instabilities in the flow around two circular cylinders in tandem (2010, background): “Mode A is proposed to be an instability of elliptical type (Williamson 1996; Leweke & Williamson 1998b; Thompson et al. 2001).”
• Direct numerical simulations of forced and unforced separation bubbles on an airfoil at incidence (2008, background): “In the light of these differences it has been suggested that mode-A is caused by elliptic instability ( Thompson, Leweke & Williamson 2001 ), and that mode-B is in fact a manifestation of the instability of two-dimensional hyperbolic streamlines, analogous to that of elliptic instability (Leweke & W”
• Quantitative numerical analysis of flow past a circular cylinder at Reynolds number between 50 and 200 (2013, background): “D case (Re = 200, Lz = 12), and after an initial start-up period of about 60 time units, the flow remained quite a long time in a state that appeared to be saturated with highly ordered but rather weak mode A (Williamson, 1996a; Thompson et al., 2001) instability structures.”