Shock waves are sites of efficient energy dissipation where directed kinetic energy is converted into heat and potentially other forms of energy. As astrophysical shocks are typically collisionless (Coulomb collisions can be neglected to a good approximation), the energy must be dissipated through collective electromagnetic processes, and a significant fraction of the dissipated energy may be converted into magnetic fields and non-thermal particles. The theory of how particles are accelerated at shocks into non-thermal power-law like distributions is now well established, although it is increasingly evident that we must understand the interplay between the accelerating particles and the plasmas that support the magnetic field fluctuations that ultimately dictate the energetic particle transport. I will review the current status of the limits of shock acceleration in different environments, and highlight some recent observational developments.
