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The Degasperis–Procesi (DP) equation is the nonlinear integrable PDE
*m*_{t}+*m*_{x}*u*+*3**m**u*_{x} = 0, where *m* = *u*−*u*_{xx}.
Like its more famous cousin, the Camassa–Holm shallow water equation
*m*_{t}+*m*_{x}*u*+*2**m**u*_{x} = 0,
it admits a particular type of solutions called **peakons** (peaked solitons).

The *n*-peakon solution is a superposition of *n* interacting
peak-shaped waves, each with its own time-dependent position
*x*_{k}(*t*)
and amplitude *m*_{k}(*t*):

These solutions must be interpreted in a suitable weak sense,
since *u* is not differentiable in the classical sense
everywhere (the derivative *u*_{x} is a piecewise
continuous function, which is undefined at the points
*x*_{k} where it has jump discontinuities).

(Read more about peakons on another page.)

While trying to understand what happens at a
"peakon–antipeakon collision" (see below), I found that the DP equation
(unlike the Camassa–Holm equation whose solutions must be continuous) also has
a class of even weaker solutions that I called **shockpeakons**,
where the wave profile *u* itself has jump discontinuities (shocks):

This formula gives a solution of the DP equation provided that the
positions *x*_{k},
amplitudes *m*_{k} and shock
strengths *s*_{k} satisfy a certain system of
3*n* ordinary differential equations. (Explicit solution formulas for
these ODEs when shocks are present are only known in a few simple
special cases, but the system can of course be approximately integrated
by numerical methods.)

It's quite unusual to have this kind of (relatively) explicit examples of very weak solutions to such a complicated PDE. Shockpeakons (and ordinary peakons) are useful as test cases when designing numerical methods for the DP equation.

Below is a movie showing a solution of the DP equation
where a shockpeakon forms at a collision between
a peakon (*m*_{1} > 0) and an antipeakon (*m*_{2} < 0).
(There is also a larger version with annotations: 4 MB GIF animation.)

In this example, the peakon is a little stronger than the antipeakon,
so the resulting shockpeakon moves to the right. (The total
momentum *m*_{1} + *m*_{2}, in this case a
positive number, is conserved throughout the process, and therefore
the newborn shockpeakon has positive momentum.)

For the Camassa–Holm equation, the behaviour is different: there the peakon and the antipeakon just pass through each other. Compare the following figures (click on the images for larger versions):

(To be precise: the CH figure shows the
so-called *conservative* solution. There is also a *dissipative* solution
where the peakon–antipeakon pair doesn't reappear after the collision and the
lower picture therefore would show just a single peakon,
and there are also intermediate cases where the peakon–antipeakon pair
reappears although with less energy than it had before the collision.)

Around the same time as I was playing around with explicit solutions and discovered shockpeakons, Giuseppe Maria Coclite and Kenneth Hvistendahl Karlsen released a preprint about discontinuous solutions to the DP equation in general, with focus on questions like existence and wellposedness in certain function spaces. This was very lucky for me, since they knew a lot of things that I didn't!

One thing that I learned from the paper of Coclite and Karlsen was the
concept of *entropy solution*. For weak solutions, the PDE itself
may not be enough to determine the solution uniquely. An *entropy
condition* is one kind of additional condition which can be imposed
on the solution in order to guarantee uniqueness. The general formulas
are a bit technical, so I will not go into that here, but for
shockpeakons the situation is simple: they are entropy solutions
provided that all *s*_{k} are nonnegative, meaning
that the jumps in the solution *u* must go from high on the left
to low on the right (as in the pictures and movies).

Even though the DP equation is formally integrable (it has a Lax pair,
etc.), the shockpeakon ODEs are still unsolved except in the trivial case
*n* = 1, and a in subcase of a symmetric special case of the
case *n* = 2. The methods used to compute the
*n*-peakon solution (without
shocks) don't seem to work when shocks are present, and some quantities that
are conserved for nice solutions are not conserved for discontinuous solutions.
So, who knows, maybe
the DP equation should *not* be considered integrable when
studying discontinuous solutions?

Last modified 2015-01-07. Hans Lundmark (hans.lundmark@liu.se)