The generalized Kirchhoff equations and their application to the interaction between a rigid body and an arbitrary time-dependent viscous flow

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Falling styles of disks (2012, methodology): “…acceleration can easily be computed using the short-time variations of the force (respectively, torque) experienced by the body in presence of an imposed acceleration of the upstream flow, following the procedure described by Rivero, Magnaudet & Fabre (1991) (see also Mougin & Magnaudet 2002a).”
Bubbly and Buoyant Particle–Laden Turbulent Flows (2020, background): “…flow, Mougin and Magnaudet (2001) extended the case to a situation where the NS equations governing the liquid flow (Auguste and Magnaudet 2018; Mougin and Magnaudet 2002) are considered in conjunction with Newton’s laws for the translational and rotational 10 Mathai et al. Bubbles and Buoyant…”
Hydrodynamic interactions between two spherical bubbles rising side by side in a viscous liquid (2003, background): “It was recently shown (Mougin & Magnaudet 2002b) that this wake instability is the cause of the zigzagging/ spiralling motion of clean millimetric bubbles rising in low-viscosity liquids.”
Instabilities and transition of a sphere falling or ascending freely in a Newtonian fluid (2004, methodology): “The necessity of adopting the described implicit approach without splitting the force term on the right-hand side of (4.4a) is best clarified by reminding ourselves of the added mass effects (Mougin & Magnaudet 2002a).”