Math 2.0

Partial differential equations Definition

Kadomtsev–Petviashvili equation

Builds on Partial differential equationKorteweg–De Vries equationPartial derivative

Definition

Let σ∈{1,−1}\sigma \in \set{1, -1}. The Kadomtsev–Petviashvili equation is the partial differential equation ∂x(ut+6uux+uxxx)+3σuyy=0\partial_x \big( u_t + 6 u u_x + u_{xxx} \big) + 3 \sigma u_{yy} = 0 for an unknown real function u(x,y,t)u(x, y, t) of (x,y)∈ℝ2(x, y) \in \R^2 and t∈ℝt \in \R, where subscripts denote partial derivatives. The case σ=1\sigma = 1 is called KP-II and the case σ=−1\sigma = -1 is called KP-I.

Remarks

Example: let v(x,t)v(x, t) be a solution of the Korteweg–De Vries equation vt+6vvx+vxxx=0v_t + 6 v v_x + v_{xxx} = 0, and put u(x,y,t)=v(x,t)u(x, y, t) = v(x, t). Then the bracket vanishes and uyy=0u_{yy} = 0, so uu solves both KP-I and KP-II.

Non-example: u(x,y,t)=y2u(x, y, t) = y^2 is not a solution, because the first term is 00 while 3σuyy=6σ≠03 \sigma u_{yy} = 6 \sigma \ne 0.

Other normalisations are used, for example ∂x(ut+uux+ε2uxxx)+λuyy=0\partial_x(u_t + u u_x + \varepsilon^2 u_{xxx}) + \lambda u_{yy} = 0 with λ=±1\lambda = \pm 1. They reduce to the form above by scaling the variables, and the sign of the uyyu_{yy} term relative to the dispersive term decides between KP-I and KP-II.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Kadomtsev–Petviashvili_equation
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MSC35Q53, 35Q51
DefinesKadomtsev–Petviashvili equation
UsesPartial differential equation, Korteweg–De Vries equation, Partial derivative

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