  The Bloch equation describes the evolution of classical particles tagged with
a magnetisation vector in a strong magnetic field and is fundamental to many
NMR and MRI contrast methods. The equation can be generalised to include the
effects of spin motion by including a spin flux, which typically contains a
Fickian diffusive term and/or a coherent velocity term. This form is known as
the Bloch-Torrey equation, and is fundamental to MR modalities which are
sensitive to spin dynamics such as diffusion MRI. Such modalities have received
a great deal of interest in the research literature over the last few years,
resulting in a huge range of models and methods.
  In this work we make make use of a more general Bloch-Torrey equation with a
generalised flux term. We show that many commonly employed approaches in
Diffusion MRI may be viewed as different choices for the flux terms in this
equation. This viewpoint, although obvious theoretically, is not usually
emphasised in the diffusion MR literature and points to interesting new
directions for methods development.
  In the interests of completeness, we describe all the necessary mathematical
and physical framework -- including the method used to solve the various
Bloch-Torrey equations. We then review the relevant portions of the diffusion
MRI literature and show how different flux choices lead to different models.
All the models considered here are continuum-based but we also discuss their
relationship to so-called microstructure methods and other more advanced ideas
such as time-dependent diffusivities.
