It is shown that the expressions for the correlation tensors of homoge
neous axisymmetric turbulence can be considerably simplified compared
to previous analyses of Batchelor (1946) and Chandrasekhar (1950). Rep
resentations of the axisymmetric two-point correlations tensors are fo
und, such that each measurable correlation corresponds to a single sca
lar function, and moreover such that the equations of continuity relat
ing different tensor components to each other take the most simple for
m. Reflectional symmetry in planes normal to but not in planes through
the axis of symmetry is demanded, which allows a full description of
states with rotation about the axis of symmetry. The second and third-
order velocity correlation tensors and the first-order pressure-veloci
ty correlation tensor are analysed with the new method. Small separati
on expansions of the correlation functions yield the quantities which
have to be measured to determine various terms in the governing equati
ons for the Reynolds stresses and the dissipation tenser. A scalar Poi
sson equation for the pressure-strain is derived, and the single-point
solution is written as a sum of integrals over measurable correlation
functions. The simplified analysis can be of great experimental impor
tance. It reveals in a simple way how a full experimental picture of h
omogeneous axisymmetric turbulence can be obtained by measuring compon
ents of the velocity at two points at variable distance from each othe
r on a line perpendicular to the mean flow in a wind tunnel. By using
the Fourier-Bessel transform it is also shown that the three-dimension
al energy, transfer, and pressure-strain spectra can be extracted from
such measurements.