Catastrophic landslides cause billions of dollars in damages and claim thousands of lives annually, whereas slow-moving landslides with negligible inertia dominate sediment transport on many weathered hillslopes. Surprisingly, both failure modes are displayed by nearby landslides (and individual landslides in different years) subjected to almost identical environmental conditions. Such observations have motivated the search for mechanisms that can cause slow-moving landslides to transition via runaway acceleration to catastrophic failure. A similarly diverse range of sliding behavior, including earthquakes and slow-slip events, occurs along tectonic faults. Our understanding of these phenomena has benefitted from mechanical treatments that rely upon key ingredients that are notably absent from previous landslide descriptions. Here, we describe landslide motion using a rate-and state-dependent frictional model that incorporates a nonlocal stress balance to account for the elastic response to gradients in slip. Our idealized, one-dimensional model reproduces both the displacement patterns observed in slowmoving landslides and the acceleration toward failure exhibited by catastrophic events. Catastrophic failure occurs only when the slip surface is characterized by rate-weakening friction and its lateral dimensions exceed a critical nucleation length h * that is shorter for higher effective stresses. However, landslides that are extensive enough to fall within this regime can nevertheless slide slowly for months or years before catastrophic failure. Our results suggest that the diversity of slip behavior observed during landslides can be described with a single model adapted from standard fault mechanics treatments.landslides | slope failure | rate and state friction | pore-water pressure | effective stress L aboratory experiments (1, 2) and numerical models (3,4) suggest that for slow-moving landslides that persist over periods of years to centuries (5) the shear strength that resists motion increases with slip rate-a characteristic referred to as rate strengthening-whereas the opposite is true for landslides that exhibit runaway acceleration and catastrophic failure. Two primary mechanisms are invoked frequently to describe the former rate-strengthening behavior. The first characterizes landslide materials as viscoplastic (i.e., Bingham-plastic), so that an increase in velocity corresponds with an increase in strain rate and viscous resistance. These models are able to reproduce field-based measurements of velocity for seasonally active slow-moving landslides (3). However, this constitutive behavior contradicts measurements that suggest landslide displacement is dominated by frictional sliding along basal and lateral faults (6); furthermore, such rheological models are unable to capture the transition from slow sliding to catastrophic failure. The second modeling approach applies Coulomb friction and invokes shear-zone dilatancy to regulate porewater pressure changes so that sliding increases strength because of ...