The distribution of earthquakes (yellow dots in the NASA picture below) and volcanoes (red dots) on the Earth’s surface marks the boundaries (blue lines) of tectonic plates. Plates can be oceanic or continental lithosphere, as well as both. Volcanism and seismicity are the expression of plate interactions at their margins. Ocean rifts, where seafloors spread, are divergent boundaries, along which plates separate. Mountain belts occur along convergent plate boundaries.

The eminent English geologist Arthur Holmes (1890 – 1965), considered the father of modern geology, was the first to provide a plausible mechanism for lithospheric plate motion. Holmes, who started studying physics and later moved to geology, was the first to propose a geological time scale based on recent discoveries about radioactivity. His first evaluation of the age of the Earth was 4 billion years, the first to get significantly close to modern assessments. At 23 he was already an authority of geology.

Before the scientific community accepted Wegener’s theories, he was the first to suggest the idea of convective motions in the mantle that would drag the overlying lithosphere portion (below). Holmes’ hypothesis is much remarkable, but still the forces involved in convective motions are too weak to displace a plate.

Actually, today we see lithosphere as an integral part of the convective cell, the outermost cold portion of the cell, not just a transported slab. At the spot where the hot expanding material rises, melted material is ejected at the surface (continental and ocean rift volcanism) creating new lithosphere. Ocean floors spread from the rift, lifted up by the raising hot material from the asthenosphere. Continental rifts are the place for upcoming formation of new oceans. In this way seafloor spreading separates the continents (as proposed by Wegener for South America and Africa). But if new lithospheric material is being formed, where does the excess material end up?

 Back to the hypsometric curve, we still have to explain the existence of the few elevation minimums – the ocean tranches. Seismology will come to help. In 1935, the Japanese seismologist Kiyoo Wadati (1902 – 1995), who inspired Charles Richter to create his earthquake magnitude scale, observed how at ocean trenches deep earthquakes extended along a tilted plane up to island arcs like Japan.

In 1949, the American seismologist Hugo Benioff (1899 – 1968), professor at the California Institute of Technology, noticed how earthquake hypocenters recorded along a 50 km belt off the North American Pacific coast were progressively deeper: those with hypocenters down to 300 km of depth were aligned along a 33° trend, while the deeper ones aligned along a 60° trend.

Those dipping seismic hypocenter alignment trends would represent lithosphere slabs dipping into the mantle, causing the deepening seismicity trends. They took the name of Benioff-Wadati zones (below), the most plausible places on Earth where to suppose the excess ocean lithosphere is being consumed (if we rule out the Earth is inflating!). At ocean trenches the ocean lithosphere is subducting, immersing into the asthenosphere.

The bending slab causes the formation of oceanic trenches. Island arcs form from melted material from the descending slab’s partial fusion, as it dips deeper into the mantle. Over the subduction slab is a wedge of asthenospheric material. These are convergent plate boundaries. There we find mountain belts and ocean trenches, the only possible zones where the cold portions of convective cells may descend. The slabs own “weight” would actually trigger the convective motions, as the slab dives into the upper mantle exerting a “pull” on the entire plate, while the expanding ridge “pushes” the plate away.