The transition zone is part of the Earth's mantle, and is located between the lower mantle and the upper mantle, between a depth of 410 and 660 km (250 to 400 mi). The Earth's mantle, including the transition zone, consists primarily of peridotite, an ultramafic igneous rock.

The mantle was divided into the upper mantle, transition zone, and lower mantle as a result of sudden seismic-velocity discontinuities at depths of 410 and 660 km (250 to 400 mi). This is thought to occur as a result of rearrangement of grains in olivine (which constitutes a large portion of peridotite) at a depth of 410 km, to form a denser crystal structure as a result of the increase in pressure with increasing depth. Below a depth of 660 km, evidence suggests due to pressure changes ringwoodite minerals change into two new denser phases, bridgmanite and periclase. This can be seen using body waves from earthquakes, which are converted, reflected or refracted at the boundary, and predicted from mineral physics, as the phase changes are temperature and density-dependent and hence depth dependent.

410 km discontinuity – phase transition

A peak is seen in seismological data at about 410 km as is predicted by the transition from α- to β-Mg2SiO4 (olivine to wadsleyite). From the Clapeyron slope, this change is predicted to occur at shallower depths in cold regions, such as where subducting slabs penetrate into the transition zone, and at greater depths in warmer regions, such as where mantle plumes pass through the transition zone.[1] Therefore, the exact depth of the "410 km discontinuity" can vary.

660 km discontinuity – phase transition

The 660 km discontinuity appears in PP precursors (a wave which reflects off the discontinuity once) only in certain regions but is always apparent in SS precursors. It is seen as single and double reflections in receiver functions for P to S conversions over a broad range of depths (640–720 km, or 397–447 mi). The Clapeyron slope predicts a deeper discontinuity in cold regions and a shallower discontinuity in hot regions.[1] This discontinuity is generally linked to the transition from ringwoodite to bridgmanite and periclase.[2] This is thermodynamically an endothermic reaction and creates a viscosity jump. Both characteristics cause this phase transition to play an important role in geodynamical models. Cold downwelling material might pond on this transition.[3]

Other discontinuities

There is another major phase transition predicted at 520 km for the transition of olivine (β to γ) and garnet in the pyrolite mantle.[4] This one has only sporadically been observed in seismological data.[5]

Other non-global phase transitions have been suggested at a range of depths.[1][6]

References

  1. 1 2 3 C.M.R. Fowler, The Solid Earth (2nd Edition), Cambridge University Press 2005.
  2. ↑ Ito, E; Takahashi, E (1989). "Postspinel transformations in the system Mg2SiO4–Fe2SiO4 and some geophysical implications". Journal of Geophysical Research: Solid Earth. 94 (B8): 10637–10646. Bibcode:1989JGR....9410637I. doi:10.1029/jb094ib08p10637.
  3. ↑ Fukao, Y.; Obayashi, M. (2013). "Subducted slabs stagnant above, penetrating through, and trapped below the 660 km discontinuity". Journal of Geophysical Research: Solid Earth. 118 (11): 5920–5938. Bibcode:2013JGRB..118.5920F. doi:10.1002/2013jb010466. S2CID 129872709.
  4. ↑ Deuss, Arwen; Woodhouse, John (2001-10-12). "Seismic Observations of Splitting of the Mid-Transition Zone Discontinuity in Earth's Mantle". Science. 294 (5541): 354–357. Bibcode:2001Sci...294..354D. doi:10.1126/science.1063524. ISSN 0036-8075. PMID 11598296. S2CID 28563140.
  5. ↑ Egorkin, A. V. (1997-01-01). "Evidence for 520-Km Discontinuity". In Fuchs, Karl (ed.). Upper Mantle Heterogeneities from Active and Passive Seismology. NATO ASI Series. Springer Netherlands. pp. 51–61. doi:10.1007/978-94-015-8979-6_4. ISBN 9789048149667.
  6. ↑ Khan, Amir; Deschamps, Frédéric (2015-04-28). The Earth's Heterogeneous Mantle: A Geophysical, Geodynamical, and Geochemical Perspective. Springer. ISBN 9783319156279.
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