A new analytical method is presented for studying in a uniform way the
spin dynamics in NMR experiments performed under the conditions of ma
gic angle spinning. It was derived on the basis of the formalized Floq
uet theory and consists in transforming the Fourier-state representati
on of the NMR signal into an integral one. The;integral representation
proves to be well suited in combination with Rayleigh-Schrodinger per
turbation theory for both the fast and the slow spinning regimes. The
corresponding perturbation expansions can be readily extended to highe
r-order correction terms, which also allows the inclusion of more mode
rate spinning speeds. Explicit expressions of the perturbation series
were derived for both spinning regimes and applied to the case of isol
ated dipolar-coupled spin-1/2 pairs for which the results can be compa
red with those obtained by the exact evaluation of the equation of mot
ion.