POLYNOMIAL EXPANSION OF COMPRESSIBLE MODES IN ROTATING RIGID ELLIPSOIDS
J´er´emie Vidal(Leeds), Sylvie Su & David C´ebron (Grenoble)
Schematicmodel
I Rotating,stratifiedand electrically conducting fluid, I Ellipsoidalgeometry,
I Nonlinearcouplings: instabilities&turbulence.
MAC waves = flow dynamics
J´er´emie Vidal (University of Leeds) Polynomial compressible modes in ellipsoids March 27, 2019 1 / 2
POLYNOMIAL EXPANSION OF COMPRESSIBLE MODES IN ROTATING RIGID ELLIPSOIDS
J´er´emie Vidal(Leeds), Sylvie Su & David C´ebron (Grenoble)
Schematicmodel
I Rotating,stratifiedand electrically conducting fluid, I Ellipsoidalgeometry,
I Nonlinearcouplings: instabilities&turbulence.
MAC waves = flow dynamics I Acoustic wavessensitive toflow properties, I Modal acoustic velocimetry(Triana et al., 2014).
Acoustic waves = ”probes”
Nonlineareigenvalue problem ω2A2(u) +ωA1(u) +A0(u) =0.
J´er´emie Vidal (University of Leeds) Polynomial compressible modes in ellipsoids March 27, 2019 1 / 2
POLYNOMIAL EXPANSION OF COMPRESSIBLE MODES IN ROTATING RIGID ELLIPSOIDS
J´er´emie Vidal(Leeds), Sylvie Su & David C´ebron (Grenoble)
u=∇×A+∇Φ
I BC onA: non-penetration1n·(∇×A) = 0.
I BC on Φ: either free-surface (see the proceeding) or rigid1n·∇Φ = 0.
J´er´emie Vidal (University of Leeds) Polynomial compressible modes in ellipsoids March 27, 2019 2 / 2
POLYNOMIAL EXPANSION OF COMPRESSIBLE MODES IN ROTATING RIGID ELLIPSOIDS
J´er´emie Vidal(Leeds), Sylvie Su & David C´ebron (Grenoble)
u=∇×A+∇Φ
I BC onA: non-penetration1n·(∇×A) = 0.
I BC on Φ: either free-surface (see the proceeding) or rigid1n·∇Φ = 0.
J´er´emie Vidal (University of Leeds) Polynomial compressible modes in ellipsoids March 27, 2019 2 / 2