Quantitative assessment of the risk of submarine landslides is an essential part of the design process for offshore oil and gas developments in deep water, beyond the continental shelf. Landslides may be triggered by a reduction in shear strength of subsea sediments over a given zone, caused for example by seismic activity. Simple criteria are then needed to identify critical conditions whereby the zone of weakness could grow catastrophically to cause a landslide. A number of such criteria have been developed over the last decade, based either on ideas drawn from fracture mechanics, or considering the equilibrium of the initial weakened zone and adjacent process zones of gradually softening material. Accounting for the history of the weak zone initiation is critical for derivation of reliable propagation criteria, in particular considering dynamic effects arising from accumulating kinetic energy of the failing material, which will allow the failure to propagate from a smaller initial zone of weakened sediments. Criteria are developed here for planar conditions, taking full account of such dynamic effects, which are shown to be capable of reducing the critical length of the softened zone by 20% or more compared with criteria based on static conditions. A numerical approach is used to solve the governing dynamic equations for the sliding material, the results from which justify assumptions that allow analytical criteria to be developed for the case where the initial softening occurs instantaneously. The effect of more gradual softening is also explored.From the solution, the maximum value of ΔP is 1 À r whenx ¼ω 0 . Therefore, the critical process zone length for the static state is ω = ω 0 , and the critical length l c,s of the pre-softened Figure 8. Displacement distributions at quasi-critical conditions. 2322 W. ZHANG ET AL. Case 2.1 r ≥ (1 À r) / βThis case cannot occur, in that for high gravity loading the process zone cannot develop to the extent that the shear strength falls to τ r at the junction with the pre-softened zone, hence Δl fs remains at 0 (hence Case 1.1).Case 2.2 r < (1 À r) / β andω ¼ω f s ¼ω 0 þ βarcsin βr 1Àr À ÁThe shear stress at the interface between the process and fully softened zones reaches the residual value and propagation of the fully softened zone occurs, i.e. Δl fs > 0. Therefore, the length of the Figure 12. Profiles of shear stress and lateral force at the failure condition.