1992/08/21 by James H. Dieterich, M. F. Linker · 117 citations
Earth and Planetary Sciences · Engineering · Environmental Science · #Composite material #Engineering #High-pressure geophysics and materials #Instability #Landslides and related hazards #Materials science #Mechanics #Physics #Shear stress #Slider #Slip (aerodynamics) #Stiffness #Stress (linguistics) #Thermodynamics #earthquake and tectonic studies
paper · doi:10.1029/92gl01821
published in Geophysical Research Letters 19(16), 1691-1694 (American Geophysical Union)
openalex publication_date 1992/08/21 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
The stability of fault slip under conditions of varying normal stress is modeled as a spring and slider system with rate‐ and state‐dependent friction. Coupling of normal stress to shear stress is achieved by inclining the spring at an angle, ø, to the sliding surface. Linear analysis yields two conditions for unstable slip. The first, of a type previously identified for constant normal stress systems, results in instability if stiffness is below a critical value. Critical stiffness depends on normal stress, constitutive parameters, characteristic sliding distance and the spring angle. Instability of the first type is possible only for velocity‐weakening friction. The second condition yields instability if spring angle ø < ‐cot −1 μ ss , where μ ss is steady‐state sliding friction. The second condition can arise under conditions of velocity strengthening or weakening. Stability fields for finite perturbations are investigated by numerical simulation.