A geometric formulation of the conservation of wave action and its implications for signature and the classification of instabilities

Action, symplecticity, signature and complex instability are fundamental concepts in Hamiltonian dynamics which can be characterized in terms of the symplectic structure. In this paper, Hamiltonian PDEs on unbounded domains are characterized in terms of a multisymplectic structure where a distinct differential two–form is assigned to each space direction and time. This leads to a new geometric formulation of the conservation of wave action for linear and nonlinear Hamiltonian PDEs, and, via Stokes's theorem, a conservation law for symplecticity. Each symplectic structure is used to define a signature invariant on the eigenspace of a normal mode. The first invariant in this family is classical Krein signature (or energy sign, when the energy is time independent) and the other (spatial) signatures are energy flux signs, leading to a classification of instabilities that includes information about directional spatial spreading of an instability. The theory is applied to several examples: the Boussinesq equation, the water–wave equations linearized about an arbitrary Stokes's wave, rotating shallow water flow and flow past a compliant surface. Some implications for non–conservative systems are also discussed.

[1]  J. Williamson On the Algebraic Problem Concerning the Normal Forms of Linear Dynamical Systems , 1936 .

[2]  P. Sturrock In What Sense Do Slow Waves Carry Negative Energy , 1960 .

[3]  M. Kruskal,et al.  Asymptotic Theory of Hamiltonian and other Systems with all Solutions Nearly Periodic , 1962 .

[4]  Paul Garabedian,et al.  Lectures on partial differential equations , 1964 .

[5]  G. Whitham A general approach to linear and non-linear dispersive waves using a Lagrangian , 1965, Journal of Fluid Mechanics.

[6]  Vladimir E. Zakharov,et al.  Stability of periodic waves of finite amplitude on the surface of a deep fluid , 1968 .

[7]  G. Batchelor,et al.  An Introduction to Fluid Dynamics , 1968 .

[8]  W. D. Hayes,et al.  Conservation of action and modal wave action , 1970, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[9]  G. Whitham,et al.  Linear and Nonlinear Waves , 1976 .

[10]  V. Arnold Mathematical Methods of Classical Mechanics , 1974 .

[11]  V. A. I︠A︡kubovich,et al.  Linear differential equations with periodic coefficients , 1975 .

[12]  A. Weinstein Bifurcations and Hamilton's principle , 1978 .

[13]  D. G. Andrews,et al.  On wave-action and its relatives , 1978, Journal of Fluid Mechanics.

[14]  R. A. Cairns The role of negative energy waves in some instabilities of parallel flows , 1979, Journal of Fluid Mechanics.

[15]  J. Adam,et al.  ‘Explosive’ resonant wave interactions in a three-layer fluid flow , 1979, Journal of Fluid Mechanics.

[16]  G. P. Thomas,et al.  Finite-amplitude deep-water waves on currents , 1979, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[17]  P. Killworth,et al.  Ageostrophic instability of ocean currents , 1982, Journal of Fluid Mechanics.

[18]  Roger H.J. Grimshaw,et al.  Wave Action and Wave-Mean Flow Interaction, with Application to Stratified Shear Flows , 1984 .

[19]  P. Saffman,et al.  Stability of water waves , 1986, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[20]  R. MacKay,et al.  Flux and differences in action for continuous time Hamiltonian systems , 1986 .

[21]  Y. Hayashi,et al.  Stable and unstable shear modes of rotating parallel flows in shallow water , 1987, Journal of Fluid Mechanics.

[22]  A. Craik,et al.  Three-wave resonance for free-surface flows over flexible boundaries , 1988 .

[23]  F. Henyey,et al.  The energy and action of small waves riding on large waves , 1988, Journal of Fluid Mechanics.

[24]  R. Salmon,et al.  Semigeostrophic theory as a Dirac-bracket projection , 1988, Journal of Fluid Mechanics.

[25]  The superharmonic normal mode instabilities of nonlinear deep-water capillary waves , 1988 .

[26]  M. Longuet-Higgins,et al.  The orbiting double pendulum: an analogue to interacting gravity waves , 1988, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[27]  R. MacKay Flux over a saddle , 1990 .

[28]  Dennis M. Bushnell,et al.  Status of Transition Delay Using Compliant Walls , 1990 .

[29]  Movement of eigenvalues of Hamiltonian equilibria under non-Hamiltonian perturbation , 1991 .

[30]  Periodic and quasi-periodic Hamiltonian motions as relative equilibria , 1992 .

[31]  On the period-energy relation , 1992 .

[32]  Anthony Bloch P.S.Krishnaprasad,et al.  Dissipation Induced Instabilities , 1993, chao-dyn/9304005.

[33]  Stability of three-dimensional progressive gravity waves on deep water to superharmonic disturbances , 1993 .

[34]  G. Triantafyllou Note on the Kelvin–Helmholtz instability of stratified fluids , 1994 .

[35]  Spatial bifurcations of interfacial waves when the phase and group velocities are nearly equal , 1995 .

[36]  Michael L. Overton,et al.  Stability theory for dissipatively perturbed hamiltonian systems , 1995 .

[37]  T. Bridges Periodic patterns, linear instability symplectic structure and mean-flow dynamics for three-dimensional surface waves , 1996, Philosophical Transactions of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[38]  T. Bridges Multi-symplectic structures and wave propagation , 1997, Mathematical Proceedings of the Cambridge Philosophical Society.

[39]  T. Bridges,et al.  Reappraisal of the Kelvin–Helmholtz problem. Part 1. Hamiltonian structure , 1997, Journal of Fluid Mechanics.

[40]  T. Bridges,et al.  Reappraisal of the Kelvin–Helmholtz problem. Part 2. Interaction of the Kelvin–Helmholtz, superharmonic and Benjamin–Feir instabilities , 1997, Journal of Fluid Mechanics.