Microseism

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In seismology, a microseism is defined as a faint earth tremor caused by natural phenomena. [1] [2] Sometimes referred to as a "hum", [3] it should not be confused with the anomalous acoustic phenomenon of the same name. The term is most commonly used to refer to the dominant background seismic and electromagnetic noise signals on Earth, which are caused by water waves in the oceans and lakes. [4] [5] [6] [7] [8] Characteristics of microseism are discussed by Bhatt. [8] Because the ocean wave oscillations are statistically homogenous over several hours, the microseism signal is a long-continuing oscillation of the ground. [9] The most energetic seismic waves that make up the microseismic field are Rayleigh waves, but Love waves can make up a significant fraction of the wave field, and body waves are also easily detected with arrays. Because the conversion from the ocean waves to the seismic waves is very weak, the amplitude of ground motions associated to microseisms does not generally exceed 10 micrometers.

Contents

Detection and characteristics

As noted early in the history of seismology, [10] microseisms are very well detected and measured by means of a long-period seismograph, This signal can be recorded anywhere on Earth.

Power spectral density probability density function (color scale at right) for 20 years of continuous vertical component seismic velocity data recorded at Albuquerque, New Mexico by the ANMO station of the IRIS Consortium/USGS Global Seismographic Network. The high and low bounds are representative noise limits for seismographs deployed worldwide. The solid and dashed lines indicate the median and mode of the probability density function, respectively. ANMO 20 years.jpg
Power spectral density probability density function (color scale at right) for 20 years of continuous vertical component seismic velocity data recorded at Albuquerque, New Mexico by the ANMO station of the IRIS Consortium/USGS Global Seismographic Network. The high and low bounds are representative noise limits for seismographs deployed worldwide. The solid and dashed lines indicate the median and mode of the probability density function, respectively.

Dominant microseism signals from the oceans are linked to characteristic ocean swell periods, and thus occur between approximately 4 to 30 seconds. [11] Microseismic noise usually displays two predominant peaks. The weaker is for the larger periods, typically close to 16 s, and can be explained by the effect of surface gravity waves in shallow water. These microseisms have the same period as the water waves that generate them, and are usually called 'primary microseisms'. The stronger peak, for shorter periods, is also due to surface gravity waves in water, but arises from the interaction of waves with nearly equal frequencies but nearly opposite directions (the clapotis). These tremors have a period which is half of the water wave period and are usually called 'secondary microseisms'. A slight, but detectable, incessant excitation of the Earth's free oscillations, or normal modes, with periods in the range 30 to 1000 s, and is often referred to as the "Earth hum". [12] For periods up to 300 s, the vertical displacement corresponds to Rayleigh waves generated like the primary microseisms, with the difference that it involves the interaction of infragravity waves with the ocean bottom topography. [13] The dominant sources of this vertical hum component are likely located along the shelf break, the transition region between continental shelves and the abyssal plains.

As a result, from the short period 'secondary microseisms' to the long period 'hum', this seismic noise contains information on the sea states. It can be used to estimate ocean wave properties and their variation, on time scales of individual events (a few hours to a few days) to their seasonal or multi-decadal evolution. Using these signals, however, requires a basic understanding of the microseisms generation processes.

Generation of primary microseisms

The details of the primary mechanism was first given by Klaus Hasselmann, [5] with a simple expression of the microseism source in the particular case of a constant sloping bottom. It turns out that this constant slope needs to be fairly large (around 5 percent or more) to explain the observed microseism amplitudes, and this is not realistic. Instead, small-scale bottom topographic features do not need to be so steep, and the generation of primary microseisms is more likely a particular case of a wave-wave interaction process in which one wave is fixed, the bottom. To visualize what happens, it is easier to study the propagation of waves over a sinusoidal bottom topography. This easily generalizes to bottom topography with oscillations around a mean depth. [14]

Interference of ocean waves with a fixed bottom topography. Here waves with period 12 s interact with bottom undulations of 205 m wavelength and 20 m amplitude in a mean water depth of 100 m. These conditions give rise to a pressure pattern on the bottom that travels much faster than the ocean waves, and in the direction of the waves if their wavelength L1 is shorter than the bottom wavelength L2, or in the opposite direction if their wavelength is longer, which is the case here. The motion is exactly periodic in time, with the period of the ocean waves. The large wavelength in the bottom pressure is 1/(1/L1 - 1/L2). Interference of water waves with bottom topography, relevant for microseism generation.gif
Interference of ocean waves with a fixed bottom topography. Here waves with period 12 s interact with bottom undulations of 205 m wavelength and 20 m amplitude in a mean water depth of 100 m. These conditions give rise to a pressure pattern on the bottom that travels much faster than the ocean waves, and in the direction of the waves if their wavelength L1 is shorter than the bottom wavelength L2, or in the opposite direction if their wavelength is longer, which is the case here. The motion is exactly periodic in time, with the period of the ocean waves. The large wavelength in the bottom pressure is 1/(1/L1− 1/L2).

For realistic seafloor topography, that has a broad spatial spectrum, seismic waves are generated with all wavelengths and in all directions. Because the dynamic pressures of ocean waves fall off exponentially with depth, the primary microseism source mechanism is restricted to shallower regions of the world ocean (e.g., less than several hundred meters for 14 - 20 s wave energy).

Generation of secondary microseisms

The interaction of two trains of surface waves of different frequencies and directions generates wave groups. For waves propagating almost in the same direction, this gives the usual sets of waves that travel at the group speed, which is slower than phase speed of water waves (see animation). For typical ocean waves with a period around 10 seconds, this group speed is close to 10 m/s.

In the case of opposite propagation direction the groups travel at a much larger speed, which is now 2π(f1 + f2)/(k1−k2) with k1 and k2 the wave numbers of the interacting water waves.

Wave groups generated by waves with same directions. The blue curve is the sum of the red and black. In the animation, watch the crests with the red and black dots. These crests move with the phase speed of linear water waves, and the groups of large waves propagate slower (Animation) Wave group plus small.gif
Wave groups generated by waves with same directions. The blue curve is the sum of the red and black. In the animation, watch the crests with the red and black dots. These crests move with the phase speed of linear water waves, and the groups of large waves propagate slower (Animation)

For wave trains with a very small difference in frequency (and thus wavenumbers), this pattern of wave groups may have the same velocity as seismic waves, between 1500 and 3000 m/s, and will excite acoustic-seismic modes that radiate away.

Wave groups generated by waves with opposing directions. The blue curve is the sum of the red and black. In the animation, watch the crests with the red and black dots. These crests move with the phase speed of linear water waves, but the groups propagate much faster (Animation) Wave group minus small.gif
Wave groups generated by waves with opposing directions. The blue curve is the sum of the red and black. In the animation, watch the crests with the red and black dots. These crests move with the phase speed of linear water waves, but the groups propagate much faster (Animation)

As far as seismic and acoustic waves are concerned, the motion of ocean waves in deep water is, to the leading order, equivalent to a pressure applied at the sea surface. [5] This pressure is nearly equal to the water density times the wave orbital velocity squared. Because of this square, it is not the amplitude of the individual wave trains that matter (red and black lines in the figures) but the amplitude of the sum, the wave groups (blue line in figures).

Real ocean waves are composed of an infinite number of wave trains and there is always some energy propagating in the opposite direction. Also, because the seismic waves are much faster than the water waves, the source of seismic noise is isotropic: the same amount of energy is radiated in all directions. In practice, the source of seismic energy is strongest when there are a significant amount of wave energy traveling in opposite directions. This occurs when swell from one storm meets waves with the same period from another storm, [6] or close to the coast due coastal reflection.

Depending on the geological context, the noise recorded by a seismic station on land can be representative of the sea state close to the station (within a few hundred kilometers, for example in Central California), or a full ocean basin (for example in Hawaii). [7] In order to understand the noise properties, it is thus necessary to understand the propagation of the seismic waves.

Rayleigh waves constitute most of the secondary microseismic field. Both water and solid Earth particles are displaced by the waves as they propagate, and the water layer plays a very important role in defining the celerity, group speed and the transfer of energy from the surface water waves to the Rayleigh waves. The generation of secondary-microseism Love waves involves mode conversion by non-planar bathymetry and, internally, through seismic wavespeed homogeneity within the Earth. [15]

Seasonal and secular microseism variations

Seasonality variation in microseisms offers valuable insights into the dynamics of the Earth's surface and subsurface processes. Globally observable microseisms are generated by ocean waves. Seasonal changes in oceanic and atmospheric conditions, such as wave height, storm activity, and wind patterns, contribute to the observed variations in microseism intensity and frequency content. For instance, during the northern and southern hemisphere winters, storm activity and wave energy are on average higher in the corresponding winter hemispheres and microseism signals become more pronounced. In contrast, during hemispherical summers, when oceanic and atmospheric conditions are relatively calmer, the microseism signal exhibits its lowest annual intensity. By studying the seasonality variation of microseisms, researchers can gain a better understanding of the underlying physical processes and their influence on the Earth's dynamic systems. [16] Because they are driven by ocean wave energy, microseism signals around the Earth also show large spatial scale variations that reflect average wave energy over large expanses of the global oceans.

Decadal scale studies have shown that microseism energy is growing as global storms, and their associated waves, increase in intensity [17] due to rising temperatures in the oceans and atmosphere attributed to anthropogenic global warming [18] [19] [20]

Body wave microseisms

Body wave microseisms are a type of seismic wave that propagates through the Earth's interior, distinct from surface waves. These microseisms are generated by various sources, including atmospheric pressure fluctuations, oceanic interactions, and anthropogenic activities. Unlike surface waves, which predominantly travel along the Earth's surface, body wave microseisms propagate through the deeper layers of the Earth. Seasonal variations in body-wave noise has been reported, consistent with differences in storm activity between the northern and southern hemisphere. [21]

See also

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References

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  2. ↑ Ebel, John E. (2002), "Watching the Weather Using a Seismograph", Seismological Research Letters, 73 (6): 930–932, Bibcode:2002SeiRL..73..930E, doi:10.1785/gssrl.73.6.930.
  3. ↑ Ardhuin, Fabrice, Lucia Gualtieri, and Eleonore Stutzmann. "How ocean waves rock the Earth: two mechanisms explain seismic noise with periods 3 to 300 s." Geophys. Res. Lett. 42 (2015).
  4. ↑ Longuet-Higgins, M. S. (1950), "A theory of the origin of microseisms", Philosophical Transactions of the Royal Society A , 243 (857): 1–35, Bibcode:1950RSPTA.243....1L, doi:10.1098/rsta.1950.0012, S2CID   31828394
  5. 1 2 3 Hasselmann, K. (1963), "A statistical analysis of the generation of micro-seisms", Rev. Geophys., 1 (2): 177–210, Bibcode:1963RvGSP...1..177H, doi:10.1029/RG001i002p00177, hdl: 21.11116/0000-0007-DD32-8
  6. 1 2 Kedar, S.; Longuet-Higgins, M. S.; Graham, F. W. N.; Clayton, R.; Jones, C. (2008), "The origin of deep ocean microseisms in the north Atlantic ocean" (PDF), Proc. R. Soc. Lond. A, 464 (2091): 1–35, Bibcode:2008RSPSA.464..777K, doi:10.1098/rspa.2007.0277, S2CID   18073415
  7. 1 2 Ardhuin, F.; Stutzmann, E.; Schimmel, M.; Mangeney, A. (2011), "Ocean wave sources of seismic noise" (PDF), J. Geophys. Res., 115 (C9): C09004, Bibcode:2011JGRC..116.9004A, doi:10.1029/2011jc006952
  8. 1 2 Bhatt, Kaushalendra M (2014). "Microseisms and its impact on the marine-controlled source electromagnetic signal". Journal of Geophysical Research: Solid Earth. 119 (12): 2169–9356. Bibcode:2014JGRB..119.8655B. doi: 10.1002/2014JB011024 .
  9. ↑ "Microseism" . Retrieved 2008-08-25.
  10. ↑ Gutenberg, Beno (1936). "On microseisms". Bulletin of the Seismological Society of America. 26 (2). doi:10.1785/BSSA0260020111.
  11. ↑ Ruff, L.J. "Hurricane Season & Microseisms". MichSeis. Archived from the original on 2008-05-29. Retrieved 2008-08-26.
  12. ↑ Rhie, J.; Romanowicz, B. (2004). "Excitation of Earth's continuous free oscillations by atmosphere-ocean-seafloor coupling". Nature. 431 (7008): 552–556. doi:10.1038/nature02942.
  13. ↑ Ardhuin, F.; Gualtieri, L.; Stutzmann, E. (2015), "How ocean wagves rock the Earth: two mechanisms explain microseisms with periods 3 to 300 s", Geophys. Res. Lett., 42 (3): 765–772, Bibcode:2015GeoRL..42..765A, doi: 10.1002/2014GL062782
  14. ↑ Ardhuin, Fabrice. "Large scale forces under surface gravity waves at a wavy bottom: a mechanism for the generation of primary microseisms." Geophys. Res. Lett. 45 (2018), doi: 10.1029/2018GL078855.
  15. ↑ Gualtieri, Lucia (9 November 2020). "The origin of secondary microseism Love waves". Proceedings of the National Academy of Sciences. 117 (47): 29504–29511. Bibcode:2020PNAS..11729504G. doi: 10.1073/pnas.2013806117 . PMC   7703644 . PMID   33168742.
  16. ↑ Schimmel, M.; Stutzmann, E.; Ardhuin, F.; Gallart, J. (July 2011). "Polarized Earth's ambient microseismic noise: POLARIZED MICROSEISMIC NOISE". Geochemistry, Geophysics, Geosystems. 12 (7): n/a. doi: 10.1029/2011GC003661 . hdl: 10261/171829 . S2CID   58926177.
  17. ↑ Reguero, Borja; Losada, Inigo J.; Mendez, Fernand J. (2019). "A recent increase in global wave power as a consequence of oceanic warming". Nature Communications. 10: 205. doi: 10.1038/s41467-018-08066-0 . PMC   6331560 .
  18. ↑ Aster, Richard C.; McNamara, Daniel E.; Bromirski, Peter D. (2008). "Multidecadal climate-induced variability in microseisms". Seismological Research Letters. 79 (2): 94–202. doi:10.1785/gssrl.79.2.194.
  19. ↑ Bromirski, Peter (2023). "Climate-Induced Decadal Ocean Wave Height Variability From Microseisms: 1931–2021". Journal of Geophysical Research: Oceans. 128: e2023JC019722. doi: 10.1029/2023JC019722 .
  20. ↑ Aster, Richard C.; Ringler, Adam T.; Anthony, Robert E.; Lee, Thomas A. (2023). "Increasing ocean wave energy observed in Earth's seismic wavefield since the late 20th century". Nature Communications. 14. doi: 10.1038/s41467-023-42673-w . PMC   10620394 .
  21. ↑ Koper, K. D.; de Foy, B. (2008-12-01). "Seasonal Anisotropy in Short-Period Seismic Noise Recorded in South Asia". Bulletin of the Seismological Society of America. 98 (6): 3033–3045. Bibcode:2008BuSSA..98.3033K. doi:10.1785/0120080082. ISSN   0037-1106.
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