Vortex shedding model of a flapping flag
By S. Michelin, Stefan G. Llewellyn Smith, B. Glover. Journal of Fluid Mechanics, 2008
185 citations recorded by the source corpus.
Subfields: Aerospace Engineering, Computational Mechanics, Condensed Matter Physics
View Paper: https://www.semanticscholar.org/paper/28b04cb149f90a8f65695f49cdc08e70e039a8c2
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
- Olivier Doaré
- S. Michelin
- Michael J. Shelley
- Daegyoum Kim
- Morteza Gharib
- Cecilia Huertas Cerdeira
- J. Cossé
- Jun Zhang
In Computational Mechanics
- Olivier Doaré
- S. Michelin
- S. G. Smith
- Michael J. Shelley
- Jun Zhang
- Morteza Gharib
- John O. Dabiri
- David J. Smith
In Condensed Matter Physics
- S. Michelin
- Michael J. Shelley
- S. G. Smith
- Jun Zhang
- Olivier Doaré
- Charles S. Peskin
- Eric Lauga
- David J. Smith
Citations in the corpus
- Flapping and Bending Bodies Interacting with Fluid Flows (2011, background): “In a closely related approach, Michelin et al. (2008) have also developed a simpler, but fully nonlinear, model wherein the continuous vortex sheet shed by the flexible flag is replaced by the shedding of discrete point vortices with unsteady strengths.”
- Resonance and propulsion performance of a heaving flexible wing (2009, methodology): “with wp the principal value of the relative tangential velocity on the wing [28]”
- Piezoelectric coupling in energy-harvesting fluttering flexible plates: linear stability analysis and conversion efficiency (2011, background): “Both local [44] and global [20] analyses of the nonlinear regime have been performed for compliant panels or plates placed in an axial flow.”
- Flapping dynamics of an inverted flag (2013, background): “These are non-dimensional bending stiffness β and mass ratio µ defined as follows (Connell & Yue 2007; Alben & Shelley 2008; Michelin et al. 2008): β = B ρf U2L3 and µ= ρsh ρf L , (2.1) where B is the flexural rigidity of the sheet (B = Eh3/12(1 − ν2)), ρf is fluid density, and ρs is sheet density.”