The Burgers' model of compressible fluid dynamics in one dimension is exten
ded to include the effects of pressure back-reaction The system consists of
two coupled equations: Burgers' equation with a pressure gradient (essenti
ally the one-dimensional;Navier-Stokes equation) and an advection-diffusion
equation for the pressure held. It presents a minimal model of both adiaba
tic gas dynamics and compressible magnetohydrodynamics. From the magnetic p
erspective, it is the simplest possible system which allows for "Alfvenizat
ion," i.e., energy transfer between the fluid and magnetic field excitation
s. For the special case of equal fluid viscosity and (magnetic) diffusivity
, the system is completely integrable, reducing to two decoupled Burgers' e
quations in the characteristic variables v+/-v(sound) (v+/-v(Alfven)) For a
rbitrary diffusivities, renormalized perturbation theory is used to calcula
te the effective transport coefficients for forced "Burgerlence." It is sho
wn that energy equidissipation, not equipartition, is fundamental to the tu
rbulent state. Both energy and dissipation are localized to shocklike struc
tures, in which wave steepening is inhibited by small-scale forcing and by
pressure back reaction. The spectral forms predicted by theory are confirme
d by numerical simulations.