Silica cycle

Source: Wikipedia, the free encyclopedia.
authigenic silica. Green arrows correspond to biological (pelagic) fluxes. Values of flux as published by Tréguer & De La Rocha.[1]
Fluxes in teramoles of silicon per year (Tmol Si yr−1).

The silica cycle is the

sequestration of carbon through continental weathering, biogenic export and burial as oozes on geologic timescales.[4]

Overview

Silicon is the seventh most abundant element in the universe and the second most abundant element in the Earth's crust (the most abundant is oxygen). The weathering of the Earth's crust by rainwater rich in carbon dioxide is a key process in the control of

hydrated form of silica found only as an unstable solution in water, yet it plays a central role in the silica cycle.[1]

Silicifiers are organisms that use silicic acid to precipitate

photoautotrophic processing of C and N.[10][8][11][1]

The diatoms dominate the fixation and export of

preservation potential of biogenic siliceous compounds compared to organic carbon makes opal accumulation records of interest in paleoceanography and paleoclimatology
.

Understanding the silica cycle is important for understanding the functioning of marine food webs, biogeochemical cycles, and the biological pump. Silicic acid is delivered to the ocean through six pathways as illustrated in the diagram above, which all ultimately derive from the weathering of the Earth's crust.[12][1]

Terrestrial silica cycling

Silica is an important nutrient utilized by plants, trees, and grasses in the terrestrial

dissolution is estimated to occur at a rate double that of global silicate mineral weathering.[3]
Considering biogeochemical cycling within ecosystems, the import and export of silica to and from terrestrial ecosystems is small.

Weathering

Silicate minerals are abundant in rock formations all over the planet, comprising approximately 90% of the Earth's crust.[4] The primary source of silicate to the terrestrial biosphere is weathering
. The process and rate of weathering is variable, depending on rainfall, runoff, vegetation, lithology, and topography.

Given sufficient time, rainwater can dissolve even a highly resistant silicate-based mineral such as quartz.[13] Water breaks the bonds between atoms in the crystal:[14] Hydrolysis of a silica mineral

The overall reaction for the dissolution of quartz results in silicic acid

SiO2 + 2H2O → H4SiO4

Another example of a silicate-based mineral is enstatite (MgSiO3). Rainwater weathers this to silicic acid as follows:[15]

Reverse weathering

In recent years, the effect of reverse weathering on

authigenic silicate clays through the process of reverse weathering constitutes a removal of 20-25% of silicon input.[17]

Reverse weathering is often found in river deltas as these systems have high sediment accumulation rates and are observed to undergo rapid diagenesis.[18] The formation of silicate clays removes reactive silica from the pore waters of sediment, increasing the concentration of silica found in the rocks that form in these locations.[18]

Silicate weathering also appears to be a dominant process in deeper

methanogenic sediments, whereas reverse weathering is more common in surface sediments, but still occurs at a lower rate.[19]

Sinks

The major sink of the terrestrial silica cycle is export to the ocean by rivers. Silica that is stored in plant matter or dissolved can be exported to the ocean by rivers. The rate of this transport is approximately 6 Tmol Si yr−1.[20][3] This is the major sink of the terrestrial silica cycle, as well as the largest source of the marine silica cycle.[20] A minor sink for terrestrial silica is silicate that is deposited in terrestrial sediments and eventually exported to the Earth's crust.

Marine inputs

  • Inputs to the marine silica cycle adapted from Treguer et al., 1995[21]
    Inputs to the marine silica cycle
    adapted from Treguer et al., 1995[21]

Riverine

As of 2021, the best estimate of the total riverine input of silicic acid is 6.2 (±1.8) Tmol Si yr−1.

fluvial system has been reviewed by Frings and others in 2016,[24] who suggested a value of 1.9(±1.0) Tmol Si yr−1. Therefore, the total riverine input is 8.1(±2.0) Tmol Si yr−1.[1]

Aeolian

No progress has been made regarding

aeolian dust deposition into the ocean [25] and subsequent release of silicic acid via dust dissolution in seawater since 2013, when Tréguer and De La Rocha summed the flux of particulate dissolvable silica and wet deposition of silicic acid through precipitation.[12] Thus, the best estimate for the aeolian flux of silicic acid, FA, remains 0.5(±0.5) Tmol Si yr−1.[1]

Sandy beaches

A 2019 study has proposed that, in the

abiotic sand grains and dissolved them over time.[26] To test this, the researchers placed sand samples in closed containers with different kinds of water and rotated the containers to simulate wave action. They discovered that the higher the rock/water ratio within the container, and the faster the container spun, the more silica dissolved into solution. After analyzing and upscaling their results, they estimated that anywhere from 3.2 ± 1.0 – 5.0 ± 2.0 Tmol Si yr−1 of lithogenic DSi could enter the ocean from sandy beaches, a massive increase from a previous estimate of 0.3 Tmol Si yr−1.[27] If confirmed, this represents a significant input of dissolved LSi that was previously ignored.[26][1]

Marine silica cycling

marine and terrestrial silica cycle
Marine[28] and terrestrial[3][29][30][31][18] contributions to the silica cycle are shown, with the relative movement (flux) provided in units of Tmol Si/yr.[20] Marine biological production primarily comes from diatoms.[32] Estuary biological production is due to sponges.[33] Values of flux as published by Tréguer & De La Rocha.[20] Reservoir size of silicate rocks, as discussed in the sources section, is 1.5x1021 Tmol.[34]
Low-temperature processes controlling silicon dissolution in seawater[1]

Siliceous organisms in the ocean, such as

marine sediments on the seafloor each year, demonstrating that silicon recycling is a dominant process in the oceans.[3] This rapid recycling is dependent on the dissolution of silica in organic matter in the water column, followed by biological uptake in the photic zone. The estimated residence time of the silica biological reservoir is about 400 years.[3] Opal silica is predominately undersaturated in the world's oceans. This undersaturation promotes rapid dissolution as a result of constant recycling and long residence times. The estimated turnover time of Si is 1.5x104 years.[20] The total net inputs and outputs of silica in the ocean are 9.4 ± 4.7 Tmol Si yr−1 and 9.9 ± 7.3 Tmol Si yr−1, respectively.[20]

Biogenic silica production in the photic zone is estimated to be 240 ± 40 Tmol Si year −1.[20] Dissolution in the surface removes roughly 135 Tmol Si year−1, while the remaining Si is exported to the deep ocean within sinking particles.[3] In the deep ocean, another 26.2 Tmol Si Year−1 is dissolved before being deposited to the sediments as opal rain.[3]  Over 90% of the silica here is dissolved, recycled and eventually upwelled for use again in the euphotic zone.[3]

Sources

The major sources of marine silica include rivers, groundwater flux, seafloor weathering inputs, hydrothermal vents, and atmospheric deposition (aeolian flux).[15]  Rivers are by far the largest source of silica to the marine environment, accounting for up to 90% of all the silica delivered to the ocean.[15][20][35] A source of silica to the marine biological silica cycle is silica that has been recycled by upwelling from the deep ocean and seafloor.

The diagram on low-temperature processes shows how these can control the dissolution of (either amorphous or crystallized) siliceous minerals in seawater in and to the coastal zone and in the deep ocean, feeding submarine groundwater (FGW) and dissolved silicon in seawater and sediments (FW).[1] These processes correspond to both low and medium energy flux dissipated per volume of a given siliceous particle in the coastal zone, in the continental margins, and in the abysses and to high-energy flux dissipated in the surf zone.[1]

Sinks

Rapid dissolution in the surface removes roughly 135 Tmol opal Si year−1, converting it back to soluble silicic acid that can be used again for biomineralization.[20] The remaining opal silica is exported to the deep ocean in sinking particles.[20] In the deep ocean, another 26.2 Tmol Si Year−1 is dissolved before being deposited to the sediments as opal silica.[20]  At the sediment water interface, over 90% of the silica is recycled and upwelled for use again in the photic zone.[20] Biogenic silica production in the photic zone is estimated to be 240 ± 40 Tmol si year −1.[36] The residence time on a biological timescale is estimated to be about 400 years, with each molecule of silica recycled 25 times before sediment burial.[20]

Deep seafloor deposition is the largest long-term sink of the marine silica cycle (6.3 ± 3.6 Tmol Si year−1), and is roughly balanced by the sources of silica to the ocean.[15] The silica deposited in the deep ocean is primarily in the form of siliceous ooze. When opal silica accumulates faster than it dissolves, it is buried and can provide a diagenetic environment for marine chert formation.[37]  The processes leading to chert formation have been observed in the Southern Ocean, where siliceous ooze accumulation is the fastest.[37]  Chert formation however can take tens of millions of years.[38] Skeleton fragments from siliceous organisms are subject to recrystallization and cementation.[37] Chert is the main fate of buried siliceous ooze and permanently removes silica from the oceanic silica cycle.

The siliceous ooze is eventually subducted under the crust and metamorphosed in the

upper mantle.[39] Under the mantle, silicate minerals are formed in oozes and eventually uplifted to the surface. At the surface, silica can enter the cycle again through weathering.[39] This process can take tens of millions of years.[39] The only other major sink of silica in the ocean is burial along continental margins (3.6 ± 3.7 Tmol Si year −1), primarily in the form of siliceous sponges.[15] Due to the high degrees of uncertainty in source and sink estimations, it's difficult to conclude if the marine silica cycle is in equilibrium. The residence time of silica in the oceans is estimated to be about 10,000 years.[15] Silica can also be removed from the cycle by becoming chert
and being permanently buried.

Anthropogenic influences

The rise in agriculture of the past 400 years has increased the exposure rocks and soils, which has resulted in increased rates of silicate weathering. In turn, the leaching of

ocean sediment export in the future.[15]

In 2019 a group of scientists suggested acidification is reducing diatom silica production in the Southern Ocean.[40][41]

marine microorganisms
that construct silica shells


Role in climate regulation

The silica cycle plays an important role in long term global climate regulation. The global silica cycle also has large effects on the

hydrologic cycle through the chemical reaction displayed above.[4] Over geologic timescales, the rates of weathering change due to tectonic activity. During a time of high uplift rate, silicate weathering increases which results in high CO2 uptake rates, offsetting increased volcanic CO2 emissions associated with the geologic activity. This balance of weathering and volcanoes is part of what controls the greenhouse effect
and ocean pH over geologic time scales.

Biogenic silica accumulation on the sea floor contains lot of information about where in the ocean

glacial/interglacial perturbations, and thus an excellent proxy for evaluating climate changes.[44][45]

Isotope ratios of oxygen (O18:O16) and silicon (Si30:Si28) are analysed from biogenic silica preserved in lake and marine sediments to derive records of past climate change and nutrient cycling (De La Rocha, 2006; Leng and Barker, 2006). This is a particularly valuable approach considering the role of diatoms in global carbon cycling. In addition, isotope analyses from BSi are useful for tracing past climate changes in regions such as in the Southern Ocean, where few biogenic carbonates are preserved.

The

silicon isotope compositions in fossil sponge spicules (δ30Si) are being increasingly often used to estimate the level of silicic acid in marine settings throughout the geological history, which enables the reconstruction of past silica cycles.[46]

See also

References

  1. ^
    S2CID 233993801. Material was copied from this source, which is available under a Creative Commons Attribution 4.0 International License
    .
  2. ^ .
  3. ^ .
  4. ^ .
  5. ^ Garrels, R.M. (1983) "The carbonate-silicate geochemical cycle and its effect on atmospheric carbon dioxide over the past 100 million years". American Journal of Science, 283: 641-683.
  6. .
  7. .
  8. ^ .
  9. .
  10. .
  11. .
  12. ^ .
  13. .
  14. .
  15. ^ .
  16. ^ .
  17. .
  18. ^ .
  19. .
  20. ^ .
  21. .
  22. ^ .
  23. .
  24. .
  25. ^ Tegen, I. and Kohfeld, K. E. (2006) "Atmospheric Transport of Silicon". In: The Silicon Cycle: Human Perturbations and Impacts on Aquatic Systems, edited by: Ittekot, V., Unger, D., Humborg, C., and Tac An, N. T., 7: 81–91, Island Press.
  26. ^
    ISSN 2296-6463
    .
  27. ^ Wollast, R., & Mackenzie, F.T. (1983). "Global Cycle of Silica". In S.R. Aston (Ed.), Silicon Geochemistry and Biogeochemistry, Academic Press, pages 39–76.
  28. OCLC 60651167
    .
  29. .
  30. .
  31. ^ .
  32. .
  33. .
  34. .
  35. .
  36. ^ .
  37. .
  38. ^ .
  39. ^ New threat from ocean acidification emerges in the Southern Ocean, Phys.org, 26 August 2019.
  40. ^ Information, US Department of Commerce, NOAA National Centers for Environmental. "World Ocean Atlas 2009". www.nodc.noaa.gov. Retrieved 17 April 2018.{{cite web}}: CS1 maint: multiple names: authors list (link)
  41. .
  42. ^ DeMaster, D.J. (1981)."The supply and accumulation of silica in the marine environment". Geochimica et Cosmochimica Acta 45: 1715-1732.
  43. ^ Cortese, G., Gersonde, R. (2004). "Opal sedimentation shifts in the World Ocean over the last 15 Myr". Earth and Planetary Science Letters 224: 509-527.
  44. PMID 33384908. Material was copied from this source, which is available under a Creative Commons Attribution 4.0 International License
    .