The ocean floor consists of primary tectonic features that form at spreading ridges including abyssal hills, transform faults, and propagating ridges as well as volcanic seamounts which form in a variety of off-ridge settings. Seamounts are active or extinct volcanoes with heights that reach at least 1,000 m (Menard, 1964) although this definition has been broadened to include much smaller isolated volcanoes (Staudigel et al., 2010). They are basaltic in composition, volcanic in origin, and formed in one of three tectonic settings: near mid-ocean ridges, intraplate hotspots, and island arcs (Wessel, 2007). (a) The majority of small seamounts form near mid-ocean ridges. The lithosphere at divergent plate boundaries is thin and fractured; this allows magma to migrate through the lithosphere and form small seamounts that are tens to thousands of meters high (Batiza, 1981;Smith & Cann, 1990;Wessel, 2007). (b) Intraplate seamounts that form away from the spreading ridges, usually on older seafloor, are generally attributed to hotspots, although hotspots alone cannot easily explain the wide geographic spread of seamounts on the ocean floor (Vogt, 1974;Wessel, 2007). The hotspot hypothesis states that as the plate passes over a relatively stationary mantle upwelling (i.e., plume), melt generated at the lithosphere/asthenosphere migrates to the surface forming an age-progressive seamount chain (Morgan, 1971;Wilson, 1963). (c) Island arc seamounts form in the overriding plate at subduction zones. When the oceanic crust of the subducting plate reaches a depth of about 150 km it undergoes dehydration reactions that release water that lowers the melting temperature in the mantle wedge; the partial melt migrates to the surface forming island arc volcanoes (Fryer, 1996).The means of formation also has an effect on seamount size and distribution. For one, flanks of spreading centers tend to have many small seamounts (<2.5 km tall) since the lithosphere is thin (Batiza, 1981). However, if a seamount is created by a mantle plume beneath thick lithosphere, it can reach a peak of 3-10 km above the seafloor (Wessel, 2007). The distribution of seamounts differs among ocean basins and this variation can be due to the distribution of mantle plumes as well as changes in intraplate stresses. Researchers have found that the global distribution of seamounts height follows an exponential or a power-law model (Smith & Jordan, 1988;