In order to validate a model for the mechanical behaviour of sheared fractures in rock, we executed three series of direct shear tests applying three different levels of constant normal stress, to different tangential displacements and in four directions. These shear tests were performed on numerous mortar casts of a natural fracture from the Guéret granite (in France). Each cast was used only once (given CTN and U). From shear test results (strength and dilatancy) and the damaged casts, we examined the interactions between shear parameters, shear strength, dilatancy, initial morphology and strength of the fracture walls, as well as damage of the asperities.The initial morphology of the fracture walls was analysed from roughness profiles. Roughness indices, statistical distributions of angularities and variograms of elevation were calculated from the data obtained from the roughness profiles. Analysis of this data indicates that roughness indices do not all evolve in the same way during the damage process. The variograms obtained before and after the shear tests show evidences of degradation, but this data could not be incorporated in the models. However the statistical distributions of angularities, easily calculated for the apparent (2D) angles, were introduced in one model.The progressive degradation of the fracture walls was studied from the profile traces and image analysis data. The trace of the roughness profiles demonstrated the effect of the fracture walls strength and of the deposition of material from one wall to the other. The image analysis of the damaged walls showed that the shape and location of damaged zones depend on the shear direction, with regard to the morphological structures of the walls.Shear strength modelization produced three models that are applicable respectively to the pre-peak, peak and post-peak phases. The developed equations permit the incremented calculation on the shear strength with respect to the tangential displacement. Since many phenomena and parameters act on the shear strength, the three equations that we developed imply the calculation of many other parameters (e.g. a vo , a csp , i p , U p , i and