We numerically investigate the properties of speckle patterns formed by nonlinear point scatterers. We show that, in the weak localization regime, dynamical instability appears, eventually leading to chaotic behavior of the system. Analysing the statistical properties of the instability thresholds for different values of the system size and disorder strength, a scaling law is emphasized. The later is also found to govern the smallest decay rate of the linear system, putting thus forward the crucial importance of interference effects. This is also underlined by the fact that coherent backscattering is still observed even in the chaotic regime.PACS numbers: 42.25.Dd 42.65.sf 42.65.-k As first described by Anderson in 1958, the impact of disorder on the transport properties of waves, depending on the dimensionality and the disorder strength, ranges from weak to strong localization. In the case of matter waves, the localization of Bose-Einstein condensates (BEC) is, at present, a very active research topic investigated by several experimental and theoretical groups [1,2,3,4,5,6,7,8], in particular with the recent observation of the (1D) localization of matter waves in a disordered optical potentials [9,10]. Although, in these experiments, the atom-atom interactions were negligible, the basic question remains how effects of interference between multiply scattered waves, such as weak or strong localization, are affected by interactions.BEC's in disordered potentials appear to be good candidates to study these questions, since, in the mean field regime, the condensate is still described by a single coherent wave function governed by a nonlinear wave equation (Gross-Pitaevski equation). Thus, the condensate in principle retains its ability to display interference effects also in presence of (not too strong) interactions. Similar nonlinear equations describe propagation of light in disordered nonlinear media [11]. In contrast, the situation is quite different in the case of electronic transport [12], where the interactions combined with finite temperature effects give rise to dephasing, which in general destroy the disorder-induced coherent effects.Even if the theoretical description of coherent effects in nonlinear disordered systems is far from complete, an important step was done recently by the development of a diagrammatic theory for coherent backscattering in presence of nonlinearity [13]. This approach relies on the assumption of a unique stationary solution of the nonlinear wave equation under consideration. This assumption is expected to be valid for very weak nonlinearities (which, however, may still considerably affect the height of the coherent backscattering cone [8,13]). On the other hand, it is known that larger nonlinearities can induce speckle instabilities, such that no stationary state is reached at long times [8,14]. A clear explanation for the physical origin of this effect, however, is still missing. Theoretical predictions of the nonlinearity threshold above which instabilities develop, were attemp...