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6 Transient growth of perturbation energy in conservative systems

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rencontre du non-lin´eaire 2020 1

Transient growth of perturbation energy in conservative systems

Kevin Ha1, Jean-Marc Chomaz1 & Sabine Ortiz2

1 LadHyX, Ecole Polytechnique, CNRS UMR 7646, 91128 Palaiseau

2 IMSIA, ENSTA Paristech, EDF/CNRS/CEA/ENSTA UMR 9219, F-91762 Palaiseau [email protected]

When the classical problem of the rotation of a rigid body is considered, it is well-known that a rotation around the axis M2 corresponding to the intermediate moment of inertia J2 is unstable. We demonstrate in the present work that a rotation around the two other axis M1, M3, which are known to be stable, exhibits transient growth of perturbation energy. This transient growth becomes extremely large if the moment of the stable axis considered (J1 orJ3) is close to J2. This initial transient growth of the perturbation leads to an extremely extended nutation of the rotation axis around the considered axis when the initial perturbation is optimized. In the case of a rotation around M3 with J3 close to J2, the leading initital perturbation is along the initial axisM1. When its initial amplitude M1 reaches a threshold of order p

J3/J2−1, the trajectory changes from a nutation around the M3 axis toward a trajectory where the initial rotation is periodically transferred from the M3 to the M2 direction. The same mechanism of large transient growth of perturbation is generic to any conservative systems and in particular to the triadic resonance in wave systems such as inertial waves.

Figure 1. Energy sphere in a (M10, M20, M30)-space withMn0 =Mn/√

Jnwhen J3=J2(1 +ε) with ε1. The M1 andM3 axes are circled by blue and red ellipses which are the line intersections between the energy sphere and the momentum ellipsoid for M2 ∈]2J1E,2J2E] andM2 ∈]2J2E,2J3E] respectively. The lines of equation M2 = 2J2E represented in dash-dotted dark lines separate the two previous bassins of solutions.

R´ ef´ erences

1. H.K. Moffatt, Note on the triad interactions of homogeneous turbulence,J. Fluid Mech.,741, 1469–7645 (2014).

2. L. Van Damme, P. Mardesic & D. Sugny, The tennis racket effect in a three-dimensional rigid body, Physica D : Nonlinear Phenomena,318, 17–25 (2017).

c Non Lin´eaire Publications, Avenue de l’Universit´e, BP 12, 76801 Saint- ´Etienne du Rouvray cedex

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