On the Extraction of Ring Current Ion Pitch-Angle Distributions from ENA Images E. C. Roelof and R. Demajistre There is growing evidence that pitch-angle distributions (PADs) of ring current ions (10-200 keV) are strongly affecting the brightness variations in energetic neutral atom (ENA) images being obtained with the IMAGE/HENA camera [C:son Brandt et al., this Conference]. Because the evolution of these PADs is a critical diagnostic of the injection and transport of ring current ions, the extraction of the global behavior of PADs from the ENA images is a priority task. The mathematical difficulty is that a single ENA image is 2-dimensional, whereas the energetic ion distribution is three-dimensional (L, MLT, alpha). The extraction process therefore requires the assumption of the invariance of the ion magnetic moment sin^2 alpha/B, and it depends on comparing lines of sight from different pixels that view high altitudes and low altitudes along the same field lines (similar ranges of L and MLT). The observational difficulty is that the ENA emission from low altitudes can easily be more than an order of magnitude brighter than that from high altitudes on the same field line. The source of this ENA emission is the charge exchange of energetic singly-charged ions with exospheric atoms at altitudes of ~ 300-400 km. It is here that the densities of atomic oxygen and helium (and perhaps di-atomic nitrogen) overwhelm the density of the geocoronal hydrogen that is the converter of ring current ions into ENAs at all higher altitudes. This bright low altitude emission is from too small a volume to be resolved by the HENA camera pixels (6 degrees x 6 degrees), and (to complicate matters further) the "point spread" function of the instruments causes the bright emission to "bloom" into adjacent pixels. However, the basic formulas for calculating exospheric ENA emission [Roelof, Adv. Space Res., 20(3), 361-366, 1997] have now been combined with the HENA point-spread function in computer for comparison with IMAGE/HENA images of 10-100 keV ENA hydrogen. Examples will be presented of how these simulations are used to constrain the global spatial dependence of PADs in the IMAGE/HENA images of the storm-time ring current. _______________ Submitted to the Spring 2001 AGU Meeting, Boston, Massachusetts