transformation properties of divergence (of a vector field) Hi,
If I have a divergence free vector field defined on a smooth manifold, and I apply some diffeomorphism, what can I say about what happens to the vector field?  The example I am using is of an open or closed (pick one) disk embedded in 3 dimensions and we contract the disk to a line.  Perhaps the question could be answered by giving first only the most general transformation that could be applied to the vector field (probably general linear transformation) followed by others that may depend increasingly on the metric (which I may want to ignore since I am more interested in diffeomorphisms rather than smooth maps) and yet further depending on the properties of the vector field.
thanks
 A: The divergence of a vector field depends on a volume form, which is a nowhere-zero $n$-form on an oriented $n$-manifold.  Given a volume form, most diffeomorphisms change it, but there is a large and rich group of diffeomorphisms that preserve it. For instance,
Calabi showed (by an elementary construction) that there is a
deformation retraction from the space of all smooth diffeomorphisms on a manifold to the space of
 volume-preserving diffeormorphisms --- basically because the set of choices for positively-oriented volume forms is contractible.  (Note: this retraction cannot be made to preserve the group structure). I.e, you can do basically
anything you want with volume preserving vector fields except things that are obviously impossible (like a diffeomorphism of a ball to a proper subset of the ball).  Quite a lot is also known about the group structure of volume-preserving diffeomorphisms,
as well, if there are questions that involve actual group relations.
There are topological and differentiable consequences of a vector field being divergence free, which are of course preserved by
diffeomorphisms.   On a closed manifold, the Poincaré recurrence theorem states that for almost every x in $M^n$, the
 flow line of a divergence free vector field returns infinitely often to every neighborhood of its starting point.  This is because for any set of positive measure, the forward flow-tube builds up volume at a steady rate, so if there's an upper bound, it has to come back and intersect itself. 
The diffeomorphic image of a divergence free vector field has the property that it can be multiplied by a smooth function --- that is, the speed of the flow can be regulated --- to make it divergence free again.   Given a diffeomorphism, just multiply by the ratio of the volume in the domain to the volume in the range.  I.e., just like in a stream, the flow slows down when it spreads out and has to speed up to maintain flow through a small gap.
Divergence free vector fields are in 1-1 correspondence with closed $n-1$ forms, by the correspondence
$$X \leftrightarrow i_X(\Omega), $$
where $X$ is the vector field, $\Omega$ is the volume form, and $i_X$ means stick $X$ in the first slot of $\Omega$, thought of as a function from an n-tuple of vectors to the real numbers.  You can think of $i_X(\Omega)$ as the flux or flow rate of the vector field $X$ through an infinitesimal element of $n-1$-dimensional area. If $X$ is the instantaneous flow of the Mississippi river in time units of second, and you integrate $i_X(dV)$ on a surface that cuts across the entire river, you get the amount of water per second flowing through the Mississippi at that place.
It's easy to work with closed $n-1$ forms, by
starting with a basis for cohomology, then modifying by $d(n-2$ form$)$.   You can take a diffeomorphism that is the time t flow of a divergence free vector field, and it will preserve divergence-freeness of any other vector field.  This does not get all
examples even near the identity, but by integrating time-dependent families of divergence free vector fields, you get arbitrary  volume-preserving vector field that are isotopic to the identity, and containing a neighborhood of the identity.
