scholarly journals Numerical study of blow-up in solutions to generalized Kadomtsev-Petviashvili equations

2014 ◽  
Vol 19 (6) ◽  
pp. 1689-1717 ◽  
Author(s):  
Christian Klein ◽  
◽  
Ralf Peter
Keyword(s):  
Blow Up ◽  
Nonlinearity ◽  
2017 ◽  
Vol 30 (7) ◽  
pp. 2566-2591 ◽  
Author(s):  
Anna Kazeykina ◽  
Christian Klein
Keyword(s):  
Blow Up ◽  

Author(s):  
C. J. Budd ◽  
V. A. Galaktionov ◽  
Jianping Chen

We study the behaviour of the non-negative blowing up solutions to the quasilinear parabolic equation with a typical reaction–diffusion right-hand side and with a singularity in the space variable which takes the formwhere m ≧ 1, p > 1 are arbitrary constants, in the critical exponent case q = (p–1)/m > 0. We impose zero Dirichlet boundary conditions at the singular point x = 0 and at x = 1, and take large initial data. For a class of ‘concave’ initial functions, we prove focusing at the origin of the solutions as t approaches the blow-up time T in the sense that x = 0 belongs to the blow-up set. The proof is based on an application of the intersection comparison method with an explicit ‘separable’ solution which has the same blow-up time as u. The method has a natural generalisation to the case of more general nonlinearities in the equation. A description of different fine structures of blow-up patterns in the semilinear case m = 1 and in the quasilinear one m > 1 is also presented. A numerical study of the semilinear equation is also made using an adaptive collocation method. This is shown to give very close agreement with the fine structure predicted and allows us to make some conjectures about the general behaviour.


Author(s):  
Christian Klein ◽  
Christof Sparber ◽  
Peter Markowich

Using a Fourier spectral method, we provide a detailed numerical investigation of dispersive Schrödinger-type equations involving a fractional Laplacian in an one-dimensional case. By an appropriate choice of the dispersive exponent, both mass and energy sub- and supercritical regimes can be identified. This allows us to study the possibility of finite time blow-up versus global existence, the nature of the blow-up, the stability and instability of nonlinear ground states and the long-time dynamics of solutions. The latter is also studied in a semiclassical setting. Moreover, we numerically construct ground state solutions of the fractional nonlinear Schrödinger equation.


2004 ◽  
Vol 14 (10) ◽  
pp. 1425-1450 ◽  
Author(s):  
CRISTINA BRÄNDLE ◽  
PABLO GROISMAN ◽  
JULIO D. ROSSI

We present adaptive procedures in space and time for the numerical study of positive solutions to the following problem: [Formula: see text] with p,m>0. We describe how to perform adaptive methods in order to reproduce the exact asymptotic behavior (the blow-up rate and the blow-up set) of the continuous problem.


2018 ◽  
Vol 100 (4) ◽  
pp. 291-308
Author(s):  
K. Achille Adou ◽  
K. Augustin Touré ◽  
A. Coulibaly

1998 ◽  
Vol 08 (08) ◽  
pp. 1363-1386 ◽  
Author(s):  
C. BESSE ◽  
C. H. BRUNEAU

This paper is devoted to the numerical approximation of the elliptic-hyperbolic form of the Davey–Stewartson equations. A well-suited finite differences scheme that preserves the energy is derived. This scheme is tested to compute the famous dromion 1–1 and dromion 2–2 solutions. The accuracy of Crank–Nicolson scheme is discussed and it is shown that it induces a phase error. The qualitative behaviour of the solutions is then studied; in particular the influence of the initial datum and of the various parameters is pointed out. Finally, numerical experiments show the existence of blow-up solutions.


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