- History
- Connections to physics
- Limiting behavior
- See also
- References
- External links
In mathematics and physics, the Kadomtsev–Petviashvili equation – or KP equation, named after Boris Borisovich Kadomtsev and Vladimir Iosifovich Petviashvili – is a partial differential equation to describe nonlinear wave motion. 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. It can also be solved using the inverse scattering transform much like the nonlinear Schrödinger equation.
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, 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.
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
- Novikov–Veselov equation
- Schottky problem
- Dispersionless KP equation
References
- {{Cite journal|first1=B. B.|last1=Kadomtsev|first2=V. I.|last2=Petviashvili|title=On the stability of solitary waves in weakly dispersive media|journal=Sov. Phys. Dokl.|volume=15|year=1970|pages=539–541|bibcode = 1970SPhD...15..539K }}. Translation of {{cite journal| title=Об устойчивости уединенных волн в слабо диспергирующих средах | journal=Doklady Akademii Nauk SSSR | volume=192 | issue= | pages=753–756}}
- {{Springer|id=K/k120110|first=Emma|last=Previato|authorlink=Emma Previato}}
External links
- {{mathworld|urlname=Kadomtsev-PetviashviliEquation|title=Kadomtsev–Petviashvili equation}}
- {{scholarpedia | urlname=Kadomtsev-Petviashvili_equation | title=Kadomtsev–Petviashvili equation | curator=Gioni Biondini and Dmitri Pelinovsky }}
- {{cite web | url=http://www.amath.washington.edu/~bernard/kp.html | title=The KP page | author=Bernard Deconinck | publisher=University of Washington, Department of Applied Mathematics }}