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Seismic wave

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1150:. The misfit generated by a hypocenter calculation is known as "the residual". Residuals of 0.5 second or less are typical for distant events, residuals of 0.1–0.2 s typical for local events, meaning most reported P arrivals fit the computed hypocenter that well. Typically a location program will start by assuming the event occurred at a depth of about 33 km; then it minimizes the residual by adjusting depth. Most events occur at depths shallower than about 40 km, but some occur as deep as 700 km. 758: 595: 58: 1916: 388: 952: 1129: 529: 1928: 964:- is still an ongoing process. The path that a wave takes between the focus and the observation point is often drawn as a ray diagram. Each path is denoted by a set of letters that describe the trajectory and phase through the Earth. In general, an upper case denotes a transmitted wave and a lower case denotes a reflected wave. The two exceptions to this seem to be "g" and "n". 1940: 380: 1193:
stations are used and the errors cancel out, so the computed epicenter is likely to be quite accurate, on the order of 10–50 km or so around the world. Dense arrays of nearby sensors such as those that exist in California can provide accuracy of roughly a kilometer, and much greater accuracy is possible when timing is measured directly by
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At teleseismic distances, the first arriving P waves have necessarily travelled deep into the mantle, and perhaps have even refracted into the outer core of the planet, before travelling back up to the Earth's surface where the seismographic stations are located. The waves travel more quickly than if
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A Stoneley wave is a type of boundary wave (or interface wave) that propagates along a solid-fluid boundary or, under specific conditions, also along a solid-solid boundary. Amplitudes of Stoneley waves have their maximum values at the boundary between the two contacting media and decay exponentially
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in nature. Following an earthquake event, S-waves arrive at seismograph stations after the faster-moving P-waves and displace the ground perpendicular to the direction of propagation. Depending on the propagational direction, the wave can take on different surface characteristics; for example, in the
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The hypocenter/epicenter of an earthquake is calculated by using the seismic data of that earthquake from at least three different locations. The hypocenter/epicenter is found at the intersection of three circles centered on three observation stations, here shown in Japan, Australia and the United
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Rayleigh waves, also called ground roll, are surface waves that propagate with motions that are similar to those of waves on the surface of water (note, however, that the associated seismic particle motion at shallow depths is typically retrograde, and that the restoring force in Rayleigh and in
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The travel time must be calculated very accurately in order to compute a precise hypocenter. Since P waves move at many kilometers per second, being off on travel-time calculation by even a half second can mean an error of many kilometers in terms of distance. In practice, P arrivals from many
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The naming of seismic waves is usually based on the wave type and its path; due to the theoretically infinite possibilities of travel paths and the different areas of application, a wide variety of nomenclatures have emerged historically, the standardization of which - for example in the
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are able to record both P and S waves, but those at a greater distance no longer detect the high frequencies of the first S wave. Since shear waves cannot pass through liquids, this phenomenon was original evidence for the now well-established observation that the Earth has a liquid
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Patterns of seismic wave travel through Earth's mantle and core. S-waves can not travel through the liquid outer core, so they leave a shadow on Earth's far side. P-waves do travel through the core, but P-wave refraction bends seismic waves away from P-wave shadow
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are pressure waves that travel faster than other waves through the earth to arrive at seismograph stations first, hence the name "Primary". These waves can travel through any type of material, including fluids, and can travel nearly 1.7 times faster than the
670:. Surface waves diminish in amplitude as they get farther from the surface and propagate more slowly than seismic body waves (P and S). Surface waves from very large earthquakes can have globally observable amplitude of several centimeters. 658:. S-waves are slower than P-waves, and speeds are typically around 60% of that of P-waves in any given material. Shear waves can not travel through any liquid medium, so the absence of S-waves in earth's outer core suggests a liquid state. 1141:
of the P and S waves can be used to determine the distance to the event. In the case of earthquakes that have occurred at global distances, three or more geographically diverse observing stations (using a common
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is a wave path that begins traveling towards the surface as an S-wave. At the surface, it reflects as a P-wave. The P-wave then travels through the outer core, the inner core, the outer core, and the mantle.
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A quick way to determine the distance from a location to the origin of a seismic wave less than 200 km away is to take the difference in arrival time of the P wave and the S wave in
1146:) recording P-wave arrivals permits the computation of a unique time and location on the planet for the event. Typically, dozens or even hundreds of P-wave arrivals are used to calculate 654:
case of horizontally polarized S waves, the ground moves alternately to one side and then the other. S-waves can travel only through solids, as fluids (liquids and gases) do not support
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Other modes of wave propagation exist than those described in this article; though of comparatively minor importance for earth-borne waves, they are important in the case of
722:, a British mathematician who created a mathematical model of the waves in 1911. They usually travel slightly faster than Rayleigh waves, about 90% of the S wave velocity. 689:, in 1885. They are slower than body waves, e.g., at roughly 90% of the velocity of S waves for typical homogeneous elastic media. In a layered medium (e.g., the crust and 1280: 264: 1726: 1389: 914:. Presently the periods of thousands of modes have been observed. These data are used for constraining large scale structures of the Earth's interior. 1502: 1682: 1421: 366: 1346: 1113:
is a wave that begins traveling towards the center of the Earth as an S wave. Upon reaching the outer core the wave reflects as a P wave.
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other seismic waves is elastic, not gravitational as for water waves). The existence of these waves was predicted by John William Strutt,
567:(stiffness). The density and modulus, in turn, vary according to temperature, composition, and material phase. This effect resembles the 1133:
States. The radius of each circle is calculated from the difference in the arrival times of P- and S-waves at the corresponding station.
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Surface waves travel across the surface. Surface waves decay more slowly with distance than body waves which travel in three dimensions.
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Earthquakes create distinct types of waves with different velocities. When recorded by a seismic observatory, their different
467:(ambient vibration), which is persistent low-amplitude vibration arising from a variety of natural and anthropogenic sources. 872:, which involves an expansion and contraction of the whole Earth, and has a period of about 20 minutes; and the "rugby" mode 114: 1210: 899:
represents changes in Earth's rotation rate; although this occurs, it is much too slow to be useful in seismology. The mode
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describes a twisting of the northern and southern hemispheres relative to each other; it has a period of about 44 minutes.
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does not exist because it would require a change in the center of gravity, which would require an external force.
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Body waves travel through the interior of the Earth along paths controlled by the material properties in terms of
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This article is about waves that travel through Earth. For ocean waves sometimes called "seismic sea waves", see
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Particle motion of surface waves is larger than that of body waves, so surface waves tend to cause more damage.
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of the rock increases much more, so deeper means faster. Therefore, a longer route can take a shorter time.
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they had traveled in a straight line from the earthquake. This is due to the appreciably increased
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towards away from the contact. These waves can also be generated along the walls of a fluid-filled
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Robert Stoneley, 1929 – 2008.. Obituary of his son with reference to discovery of Stoneley waves.
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of the medium as well as the type of wave. Velocity tends to increase with depth through Earth's
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Seismic surface waves travel along the Earth's surface. They can be classified as a form of
631:. Typical speeds are 330 m/s in air, 1450 m/s in water and about 5000 m/s in 537: 487: 139: 1833: 1795: 1324: 1215: 1165:
and multiply by 8 kilometers per second. Modern seismic arrays use more complicated
1153: 650: 483: 471: 408: 387: 157: 119: 693:) the velocity of the Rayleigh waves depends on their frequency and wavelength. See also 505:. In geophysics; the refraction or reflection of seismic waves is used for research into 1544: 1838: 1815: 1805: 1785: 1174: 1128: 628: 528: 498: 420: 951: 17: 1960: 1853: 943:
has a solid core, although recent geodetic studies suggest the core is still molten.
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The first observations of free oscillations of the Earth were done during the great
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oscillation.Dashed lines give nodal (zero) lines. Arrows give the sense of motion.
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Among the many types of seismic waves, one can make a broad distinction between
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zero crossings in radius. For spherically symmetric Earth the period for given
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waves. This distinction was recognized in 1830 by the French mathematician
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a Love wave sometimes called LT-Wave (Both caps, while an Lt is different)
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that produces low-frequency acoustic energy. Seismic waves are studied by
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Seismic, volcanic, or explosive energy that travels through Earth's layers
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in the planet increases with depth, which would slow the waves, but the
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a wave that travels along the boundary between the crust and mantle
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Some examples of spheroidal oscillations are the "breathing" mode
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In the case of local or nearby earthquakes, the difference in the
1127: 950: 772: 756: 593: 575:. Two types of particle motion result in two types of body waves: 527: 436: 416: 386: 378: 1699: 1439:"On waves propagated along the plane surface of an elastic solid" 745:(VSP) and making up the low frequency component of the source in 1883: 1491:. London, England: Cambridge University Press. pp. 144–178. 1366:[Memoir on the propagation of motion in elastic media]. 940: 391:
Velocity of seismic waves in Earth versus depth. The negligible
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International handbook of earthquake and engineering seismology
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An Introduction to Seismology, Earthquakes, and Earth Structure
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a wave that has been reflected off a discontinuity at depth d
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No letter is used when the wave reflects off of the surfaces
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Storchak, D. A.; Schweitzer, J.; Bormann, P. (2003-11-01).
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Mémoires de l'Académie des Sciences de l'Institut de France
1529:"Elastic waves at the surface of separation of two solids" 614:
Primary waves (P-waves) are compressional waves that are
1464:(2nd ed.). Cambridge University Press. p. 52. 1626:(4th ed.). Cambridge: Cambridge University Press. 544:
Body waves travel through the interior of the Earth.
1892: 1824: 1763: 1742: 1013:a reflection off a discontinuity in the inner core 649:Secondary waves (S-waves) are shear waves that are 1700:EDT: A MATLAB Website for seismic wave propagation 1085:an S wave ascending to the surface from the focus 1061:a P wave ascending to the surface from the focus 922:When an earthquake occurs, seismographs near the 741:, being an important source of coherent noise in 1309: 1307: 1305: 1124:Usefulness of P and S waves in locating an event 1503:"Schlumberger Oilfield Glossary. Stoneley wave" 825:is the azimuthal order number. It may take on 2 1443:Proceedings of the London Mathematical Society 1337:Seth Stein; Michael Wysession (1 April 2009). 1093:the wave reflects off the bottom of the ocean 1720: 490:, but drops sharply going from the mantle to 360: 8: 1533:Proceedings of the Royal Society of London A 1624:An introduction to the theory of seismology 1390:Burke Museum of Natural History and Culture 989:a wave that only travels through the crust 1727: 1713: 1705: 367: 353: 36: 1552: 1240:G. R. Helffrich & B. J. Wood (2002). 1584:"The IASPEI Standard Seismic Phase List" 1255:(2 August). Macmillan Magazines: 501–7. 997:a wave that reflects off the inner core 966: 918:P and S waves in Earth's mantle and core 463:. Seismic waves are distinguished from 1460:Sheriff, R. E.; Geldart, L. P. (1995). 1313: 1296: 1232: 797:while interference of Love waves gives 525:, which travel at the Earth's surface. 48: 521:, which travel through the Earth, and 1622:Bullen, K.E.; Bolt, Bruce A. (1985). 1577: 1575: 973:the wave reflects off the outer core 7: 1939: 1286:from the original on 24 August 2016. 777:The scheme of motion for spheroidal 769:oscillation for two moments of time. 1410:Sammis, C.G.; Henyey, T.L. (1987). 1157:P- and S-waves separating with time 891:Of the fundamental toroidal modes, 789:Free oscillations of the Earth are 501:help scientists locate the quake's 962:IASPEI Standard Seismic Phase List 383:p-wave and s-wave from seismograph 25: 1177:within the planet, and is termed 761:The sense of motion for toroidal 1938: 1927: 1926: 1914: 1527:Stoneley, R. (October 1, 1924). 813:is the angular order number (or 56: 1488:Some problems of geodynamics; 
 917: 1677:. Cambridge University Press. 1588:Seismological Research Letters 1416:. Academic Press. p. 12. 821:for more details). The number 1: 1647:. Amsterdam: Academic Press. 1413:Geophysics Field Measurements 474:of a seismic wave depends on 451:, who record the waves using 1021:an S wave in the inner core 711:Love waves are horizontally 532:Body waves and surface waves 1874:Precession of the equinoxes 1620:The notation is taken from 1029:a P-wave in the outer core 1005:a P-wave in the inner core 1988: 1791:Geophysical fluid dynamics 1675:Introduction to Seismology 1673:Shearer, Peter M. (2009). 729: 720:Augustus Edward Hough Love 704: 677: 642: 607: 507:Earth's internal structure 399:-wave velocity is non-zero 265:Coordinating Committee for 29: 1908: 1341:. John Wiley & Sons. 1211:Adams–Williamson equation 845:. It means the wave with 815:spherical harmonic degree 743:vertical seismic profiles 415:that travels through the 296:Adams–Williamson equation 1077:an S wave in the mantle 912:1960 earthquake in Chile 795:spheroidal oscillation S 423:. It can result from an 244:Seismic intensity scales 239:Seismic magnitude scales 1801:Near-surface geophysics 1437:Rayleigh, Lord (1885). 1362:Poisson, S. D. (1831). 1053:a P wave in the mantle 668:mechanical surface wave 1849:Earth's magnetic field 1600:10.1785/gssrl.74.6.761 1554:10.1098/rspa.1924.0079 1462:Exploration Seismology 1316:, Chapter 8 (Also see 1158: 1134: 956: 799:toroidal oscillation T 786: 770: 600: 533: 400: 384: 306:Earthquake engineering 18:Body wave (seismology) 1921:Geophysics portal 1844:Earth's energy budget 1485:Love, A.E.H. (1911). 1221:Reflection seismology 1156: 1131: 955:Earthquake wave paths 954: 931:, as demonstrated by 776: 760: 597: 531: 443:and a large man-made 390: 382: 329:Earth Sciences Portal 301:Flinn–Engdahl regions 267:Earthquake Prediction 1242:"The Earth's mantle" 933:Richard Dixon Oldham 589:SimĂ©on Denis Poisson 472:propagation velocity 291:Shear wave splitting 1893:Related disciplines 1859:Geothermal gradient 1545:1924RSPSA.106..416S 1167:earthquake location 857:does not depend on 843:radial order number 819:Spherical harmonics 191:Epicentral distance 1776:Geophysical survey 1323:2013-11-11 at the 1179:Huygens' Principle 1159: 1135: 957: 787: 771: 601: 534: 492:Earth's outer core 439:movement, a large 401: 385: 168:Induced seismicity 115:Remotely triggered 1954: 1953: 1869:Mantle convection 1684:978-0-521-88210-1 1641:Lee, William H.K. 1423:978-0-08-086012-1 1195:cross-correlation 1104: 1103: 433:volcanic eruption 427:(or generally, a 377: 376: 16:(Redirected from 1979: 1942: 1941: 1930: 1929: 1919: 1918: 1864:Gravity of Earth 1729: 1722: 1715: 1706: 1688: 1659: 1658: 1637: 1618: 1612: 1611: 1579: 1570: 1565: 1559: 1558: 1556: 1539:(738): 416–428. 1524: 1518: 1517: 1515: 1514: 1505:. 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Index

Body wave (seismology)
Tsunami
a series
Earthquakes

Types
Mainshock
Foreshock
Aftershock
Blind thrust
Doublet
Interplate
Intraplate
Megathrust
Remotely triggered
Slow
Submarine
Supershear
Tsunami
Earthquake swarm
Fault movement
Volcanism
Induced seismicity
Epicenter
Epicentral distance
Hypocenter
Shadow zone
Seismic waves
P wave
S wave

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