Published online by Cambridge University Press: 28 October 2011
We investigate the mixing properties of scalars stirred by spatially smooth, divergence-free flows and maintained by a steady source–sink distribution. We focus on the spatial variation of the scalar field, described by the dissipation wavenumber, , that we define as a function of the mean variance of the scalar and its gradient. We derive a set of upper bounds that for large Péclet number () yield four distinct regimes for the scaling behaviour of , one of which corresponds to the Batchelor regime. The transition between these regimes is controlled by the value of and the ratio , where and are, respectively, the characteristic length scales of the velocity and source fields. A fifth regime is revealed by homogenization theory. These regimes reflect the balance between different processes: scalar injection, molecular diffusion, stirring and bulk transport from the sources to the sinks. We verify the relevance of these bounds by numerical simulations for a two-dimensional, chaotically mixing example flow and discuss their relation to previous bounds. Finally, we note some implications for three-dimensional turbulent flows.