“…The evolution of the percolation parameter implies that a large amount of energy may have been released during the early-stage fracturing (as revealed by the high p at the end of the first formation stage of each pattern), after which tectonic or hydraulic forces could not be elevated to such high levels because they would be dissipated by the shearing and coalescence of the existing large structures [Petit and Mattauer, 1995;Park et al, 2010]. However, relatively small-scale fractures can form during later phases of tectonism [de Joussineau and Aydin, 2007;Park et al, 2010]. A likely universal scaling behavior may exist in a multiscale fracture system [Odling et al, 1999;Marrett et al, 1999;Bour et al, 2002;Du Bernard et al, 2002;Bertrand et al, 2015], whereas inconsistent scaling exponents separated by characteristic lengths can also occur [Ouillon et al, 1996;Hunsdale and Sanderson, 1998 Geophysical Research Letters 10.1002/2015GL067277 may be caused by the different growth mechanisms of jointing and faulting [Pollard and Segall, 1987;de Joussineau and Aydin, 2007], the influence of lithological layering [Ouillon et al, 1996;Hunsdale and Sanderson, 1998;Odling et al, 1999;Putz-Perrier and Sanderson, 2008], and the nature of driving forces (i.e., boundary or body forces) associated with distinct spatial organization of strains [Bonnet et al, 2001;Davy et al, 2010].…”