  A way to describe the hydrodynamics of the quark-gluon plasma using a DBI
action is proposed, based on the model found by Heisenberg for high energy
scattering of nucleons. The expanding plasma is described as a shockwave in a
DBI model for a real scalar standing in for the pion, and I show that one
obtains a fluid description in terms of a relativistic fluid that near the
shock is approximately ideal ($\eta\simeq 0$) and conformal. One can introduce
an extra term inside the square root of the DBI action that generates a shear
viscosity term in the energy-momentum tensor near the shock, as well as a bulk
viscosity, and regulates the behaviour of the energy density at the shock,
making it finite. The resulting fluid satisfies the relativistic Navier-Stokes
equation with $u^\mu, \rho,P,\eta$ defined in terms of $\phi$ and its
derivatives. One finds a relation between the parameters of the theory and the
QGP thermodynamics, $\a/\b^2=\eta/(sT)$, and by fixing $\a$ and $\b$ from usual
(low multiplicity) particle scattering, one finds $T\propto m_\pi$.
