Within the fault core, the fault gouge is known to deeply contribute to friction stability (Marone & Scholz, 1988;Reches & Lockner, 2010) and to play an important role in the sudden energy release during seismic sliding (Sammis et al., 1987). For local fault scale studies, one of the key points remains to be able to relate geological and physical properties of the gouge to the slip behavior and types of dynamic slip instabilities (Collettini et al., 2019;Leeman et al., 2015;). One way to determine the laboratory rock failure stability is to compare 𝐴𝐴 𝐴𝐴 , the loading stiffness of the fault, with its weakening rate 𝐴𝐴 𝐴𝐴𝑐𝑐 . Based on stick-slip theory (Byerlee & Brace, 1968;Marone, 1998;Scholz & Engelder, 1976)], slip instabilities may occur if the loading stiffness of the fault K (i.e., stiffness of the loading system) is lower than 𝐴𝐴 𝐴𝐴𝑐𝑐 ( 𝐴𝐴 𝐴𝐴𝑐𝑐 > 𝐴𝐴) . The friction obtained during gouge sliding can then be modeled either with classical slip-dependent laws (