Kadomtsev–Petviashvili equation

In mathematics and physics, the Kadomtsev–Petviashvili equation (often abbreviated as KP equation) is a partial differential equation to describe nonlinear wave motion. Named after Boris Borisovich Kadomtsev and Vladimir Iosifovich Petviashvili, the KP equation is usually written as where . The above form shows that the KP equation is a generalization to two spatial dimensions, x and y, of the one-dimensional Korteweg–de Vries (KdV) equation. To be physically meaningful, the wave propagation direction has to be not-too-far from the x direction, i.e. with only slow variations of solutions in the y direction.

Like the KdV equation, the KP equation is completely integrable.[1][2][3][4][5] It can also be solved using the inverse scattering transform much like the nonlinear Schrödinger equation.[6]

In 2002, the regularized version of the KP equation, naturally referred to as the BenjaminBona–Mahony–KadomtsevPetviashvili equation (or simply the BBM-KP equation), was introduced as an alternative model for small amplitude long waves in shallow water moving mainly in the x direction in 2+1 space.[7]

where . The BBM-KP equation provides an alternative to the usual KP equation, in a similar way that the Benjamin–Bona–Mahony equation is related to the classical Korteweg–de Vries equation, as the linearized dispersion relation of the BBM-KP is a good approximation to that of the KP but does not exhibit the unwanted limiting behavior as the Fourier variable dual to x approaches . The BBM-KP equation can be viewed as a weak transverse perturbation of the Benjamin–Bona–Mahony equation. As a result, the solutions of their corresponding Cauchy problems share an intriguing and complex mathematical relationship. Aguilar et al. proved that the solution of the Cauchy problem for the BBM-KP model equation converges to the solution of the Cauchy problem associated to the Benjamin–Bona–Mahony equation in the -based Sobolev space for all , provided their corresponding initial data are close in as the transverse variable .[8]

History

The KP equation was first written in 1970 by Soviet physicists Boris B. Kadomtsev (1928–1998) and Vladimir I. Petviashvili (1936–1993); it came as a natural generalization of the KdV equation (derived by Korteweg and De Vries in 1895). Whereas in the KdV equation waves are strictly one-dimensional, in the KP equation this restriction is relaxed. Still, both in the KdV and the KP equation, waves have to travel in the positive x-direction.

Connections to physics

The KP equation can be used to model water waves of long wavelength with weakly non-linear restoring forces and frequency dispersion. If surface tension is weak compared to gravitational forces, is used; if surface tension is strong, then . Because of the asymmetry in the way x- and y-terms enter the equation, the waves described by the KP equation behave differently in the direction of propagation (x-direction) and transverse (y) direction; oscillations in the y-direction tend to be smoother (be of small-deviation).

The KP equation can also be used to model waves in ferromagnetic media,[9] as well as two-dimensional matter–wave pulses in Bose–Einstein condensates.

Limiting behavior

For , typical x-dependent oscillations have a wavelength of giving a singular limiting regime as . The limit is called the dispersionless limit.[10][11][12]

If we also assume that the solutions are independent of y as , then they also satisfy the inviscid Burgers' equation:

Suppose the amplitude of oscillations of a solution is asymptotically small — — in the dispersionless limit. Then the amplitude satisfies a mean-field equation of Davey–Stewartson type.

See also

References

  1. ^ Wazwaz, A. M. (2007). "Multiple-soliton solutions for the KP equation by Hirota's bilinear method and by the tanh–coth method". Applied Mathematics and Computation. 190 (1): 633–640. doi:10.1016/j.amc.2007.01.056.
  2. ^ Cheng, Y.; Li, Y. S. (1991). "The constraint of the Kadomtsev-Petviashvili equation and its special solutions". Physics Letters A. 157 (1): 22–26. Bibcode:1991PhLA..157...22C. doi:10.1016/0375-9601(91)90403-U.
  3. ^ Ma, W. X. (2015). "Lump solutions to the Kadomtsev–Petviashvili equation". Physics Letters A. 379 (36): 1975–1978. Bibcode:2015PhLA..379.1975M. doi:10.1016/j.physleta.2015.06.061.
  4. ^ Kodama, Y. (2004). "Young diagrams and N-soliton solutions of the KP equation". Journal of Physics A: Mathematical and General. 37 (46): 11169–11190. arXiv:nlin/0406033. Bibcode:2004JPhA...3711169K. doi:10.1088/0305-4470/37/46/006. S2CID 2071043.
  5. ^ Deng, S. F.; Chen, D. Y.; Zhang, D. J. (2003). "The multisoliton solutions of the KP equation with self-consistent sources". Journal of the Physical Society of Japan. 72 (9): 2184–2192. Bibcode:2003JPSJ...72.2184D. doi:10.1143/JPSJ.72.2184.
  6. ^ Ablowitz, M. J.; Segur, H. (1981). Solitons and the inverse scattering transform. SIAM.
  7. ^ Bona, J. L.; Liu, Y.; Tom, M. M. (2002). "The Cauchy problem and stability of solitary-wave solutions for RLW-KP-type equations". Journal of Differential Equations. 185 (2): 437–482. Bibcode:2002JDE...185..437B. doi:10.1006/jdeq.2002.4171.
  8. ^ Aguilar, J. B.; Tom, M.M. (2024). "Convergence of solutions of the BBM and BBM-KP model equations". Differential and Integral Equations. 37 (3/4): 187–206. arXiv:2204.06016. doi:10.57262/die037-0304-187.
  9. ^ Leblond, H. (2002). "KP lumps in ferromagnets: a three-dimensional KdV–Burgers model". Journal of Physics A: Mathematical and General. 35 (47): 10149–10161. Bibcode:2002JPhA...3510149L. doi:10.1088/0305-4470/35/47/313.
  10. ^ Zakharov, V. E. (1994). "Dispersionless limit of integrable systems in 2+1 dimensions". Singular limits of dispersive waves. Boston: Springer. pp. 165–174. ISBN 0-306-44628-6.
  11. ^ Strachan, I. A. (1995). "The Moyal bracket and the dispersionless limit of the KP hierarchy". Journal of Physics A: Mathematical and General. 28 (7): 1967. arXiv:hep-th/9410048. Bibcode:1995JPhA...28.1967S. doi:10.1088/0305-4470/28/7/018. S2CID 15334780.
  12. ^ Takasaki, K.; Takebe, T. (1995). "Integrable hierarchies and dispersionless limit". Reviews in Mathematical Physics. 7 (5): 743–808. arXiv:hep-th/9405096. Bibcode:1995RvMaP...7..743T. doi:10.1142/S0129055X9500030X. S2CID 17351327.

Further reading