Abstract
Abstract
Solutions u(x) to the class of inhomogeneous nonlinear ordinary differential equations taking the form
u
″
+
u
2
=
α
f
(
x
)
for parameter α are studied. The problem is defined on the x line with decay of both the solution u(x) and the imposed forcing f(x) as |x| → ∞. The rate of decay of f(x) is important and has a strong influence on the structure of the solution space. Three particular forcings are examined primarily: a rectilinear top-hat, a Gaussian, and a Lorentzian, the latter two exhibiting exponential and algebraic decay, respectively, for large x. The problem for the top hat can be solved exactly, but for the Gaussian and the Lorentzian it must be computed numerically in general. Calculations suggest that an infinite number of solution branches exist in each case. For the top-hat and the Gaussian the solution branches terminate at a discrete set of α values starting from zero. A general asymptotic description of the solutions near to a termination point is constructed that also provides information on the existence of local fold behaviour. The solution branches for the Lorentzian forcing do not terminate in general. For large α the asymptotic analysis of Keeler, Binder and Blyth (2018 J. Fluid Mech.
832 73–96) is extended to describe the behaviour on any given solution branch using a method for glueing homoclinic connections.
Funder
International Centre for Mathematical Sciences
Institute of Mathematics and its Applications
London Mathematical Society Scheme 4
Subject
Applied Mathematics,General Physics and Astronomy,Mathematical Physics,Statistical and Nonlinear Physics