The various schemes for studying rigidly rotating perfect fluids in general
relativity are reviewed. General conclusions one may draw from these are:
(i) There is a need to restrict the scope of the possible ansatze, and (ii)
the angular behaviour is a valuable commodity. This latter observation fol
lows from a large number of analytic models exhibiting a NUT-like behaviour
. A method of getting around problem (ii) is presented on a simple example.
To alleviate problem (i) for rigidly rotating perfect fluids, approximatio
n schemes based on a series expansion in the angular velocity are suggested
. A pioneering work, due to Hartle, explores the global properties of match
ed space-times to quadratic order in the angular velocity.
As a first example of the applications, it is shown that the rigidly rotati
ng incompressible fluid cannot be Petrov type D.