We have investigated the superfluid transition of 3 He in different samples of silica aerogel. By comparing new measurements on a 99.5% sample with previous observations on the behaviour of 3 He in 98% porous aerogel we have found evidence for universal behaviour of 3 He in aerogel. We relate both the transition temperature and superfluid density to the correlation length of the aerogel.The properties of bulk 3 He are well understood. The extreme purity of 3 He at low temperatures makes it an ideal system to study the agreement between theoretical and experimental results on non-conventional Cooper pairing in the absence of disorder. Disorder plays a crucial role in suppressing the pairing interaction in high T c superconductors, the other well established non swave paired system. The superfluid transition of 3 He confined to a sample of very porous silica aerogel was first reported four years ago [1,2]. The aerogel provides a structural disorder background [4] to the liquid. 3 He is compressible, and the density can be continuously tuned by ≈30% while maintaining a fixed disorder. The 3 He zero temperature coherence length ξ 0 , defined as ξ 0 =hv f /k B T c , varies from 180Å to over 700Å as a function of density. Because the Cooper pairs in 3 He form in a p-wave state, quasiparticle scattering from the aerogel strands is pairbreaking [3]. Thus the 3 He-in-aerogel system is well suited to the exploration of the effect of impurity scattering and disorder on the superfluid transition and phase diagram.The superfluidity of 3 He in silica aerogel has been studied using torsional oscillators [1,[4][5][6], NMR [2,6-9] and sound propagation [10,11] techniques. These measurements show that both the superfluid transition temperature (T c ) and superfluid density (ρ s ) of the 3 He are suppressed by the disorder, but that the transition remains sharp [1]. This suppression is sensitive to both the density and the microstructure of the aerogel sample.The simplest model for the effect of impurity scattering on the 3 He superfluid transition is the homogeneous scattering model (HSM) which is based on the AbrikosovGorkov model for a superconductor with magnetic impurities that induce pair-breaking via spinflip scattering [12]. This mechanism is similar to that of diffuse scattering of Cooper paired 3 He from a surface [13], and is unable to explain the observed behaviour. Specifically, the observed suppression of the superfluid density is much greater than predicted by this model. More sophisticated models, such as the isotropic inhomogeneous scattering model (IISM) [14][15][16] proposed by Thuneberg and coworkers are able to quantitatively predict the superfluid transition temperature of 3 He in aerogel (for small suppressions) and have had success at qualitatively explaining the observed superfluid densities.In this Letter we present data from several different experiments on 3 He in aerogel, including new results on 3 He confined to a 99.5% porosity sample. This sample is a factor of four more dilute than any previously i...