- Richter magnitude scale
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Seismic wave • P-wave • S-wave
Measurement Mercalli scale • Richter scale
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The expression Richter magnitude scale refers to a number of ways to assign a single number to quantify the energy contained in an earthquake.
In all cases, the magnitude is a base-10 logarithmic scale obtained by calculating the logarithm of the amplitude of waves measured by a seismograph. An earthquake that measures 5.0 on the Richter scale has a shaking amplitude 10 times larger and corresponds to an energy release of √1000 ≈ 31.6 times greater than one that measures 4.0.
Developed in 1935 by Charles Richter in partnership with Beno Gutenberg, both of the California Institute of Technology, the scale was firstly intended to be used only in a particular study area in California, and on seismograms recorded on a particular instrument, the Wood-Anderson torsion seismograph. Richter originally reported values to the nearest quarter of a unit, but values were later reported with one decimal place. His motivation for creating the local magnitude scale was to measure the ratio of small to larger earthquakes.
His inspiration was the apparent magnitude scale used in astronomy to describe the brightness of stars and other celestial objects. Richter arbitrarily chose a magnitude 0 event to be an earthquake that would show a maximum combined horizontal displacement of 1 µm (0.00004 in) on a seismogram recorded using a Wood-Anderson torsion seismograph 100 km (62 mi) from the earthquake epicenter. This choice was intended to prevent negative magnitudes from being assigned. The smallest earthquakes that could be recorded and located at the time were of magnitude 3, approximately. However, the Richter scale has no lower limit, and sensitive modern seismographs now routinely record quakes with negative magnitudes.
ML (local magnitude) was not designed to be applied to data with distances to the hypocenter of the earthquake greater than 600 km (373 mi). For national and local seismological observatories the standard magnitude scale is today still ML. Unfortunately this scale saturates at M6.5, approximately, because the high frequency waves recorded locally have wavelengths shorter than the rupture lengths of large earthquakes.
To be able to measure the size of earthquakes around the globe, Gutenberg and Richter later developed a magnitude scale based on surface waves, surface wave magnitude MS; and another based on body waves, body wave magnitude mb. These are types of waves that are recorded at teleseismic distances. The two scales were adjusted such that they were consistent with the ML scale. This succeeded better with the Ms scale than with the mb scale. Both of these scales saturate when the earthquake is bigger than magnitude 8 and therefore the moment magnitude scale, Mw, was invented.
These older magnitude scales have been superseded by the implementation of methods for estimating the seismic moment, creating the moment magnitude scale, although the former are still widely used because they can be calculated quickly.
The Richter scale proper was defined in 1935 for particular circumstances and instruments; the instrument used saturated for strong earthquakes. The scale was replaced by the moment magnitude scale (MMS); for earthquakes adequately measured by the Richter scale, numerical values are approximately the same. Although values measured for earthquakes now are actually Mw (MMS), they are frequently reported as Richter values, even for earthquakes of magnitude over 8, where the Richter scale becomes meaningless. Anything above 5 is classed as a risk.[by whom?]
The Richter and MMS scales measure the energy released by an earthquake; another scale, the Mercalli intensity scale, classifies earthquakes by their effects, from detectable by instruments but not noticeable to catastrophic. The energy and effects are not necessarily strongly correlated; a shallow earthquake in a populated area with soil of certain types can be far more intense than a much more energetic deep earthquake in an isolated area.
There are several scales which have historically been described as the "Richter scale," especially the local magnitude ML and the surface wave Ms scale. In addition, the body wave magnitude, mb, and the moment magnitude, Mw, abbreviated MMS, have been widely used for decades, and a couple of new techniques to measure magnitude are in the development stage.
All magnitude scales have been designed to give numerically similar results. This goal has been achieved well for ML, Ms, and Mw. The mb scale gives somewhat different values than the other scales. The reason for so many different ways to measure the same thing is that at different distances, for different hypocentral depths, and for different earthquake sizes, the amplitudes of different types of elastic waves must be measured.
ML is the scale used for the majority of earthquakes reported (tens of thousands) by local and regional seismological observatories. For large earthquakes worldwide, the moment magnitude scale is most common, although Ms is also reported frequently.
The seismic moment, Mo, is proportional to the area of the rupture times the average slip that took place in the earthquake, thus it measures the physical size of the event. Mw is derived from it empirically as a quantity without units, just a number designed to conform to the Ms scale. A spectral analysis is required to obtain Mo, whereas the other magnitudes are derived from a simple measurement of the amplitude of a specifically defined wave.
All scales, except Mw, saturate for large earthquakes, meaning they are based on the amplitudes of waves which have a wavelength shorter than the rupture length of the earthquakes. These short waves (high frequency waves) are too short a yardstick to measure the extent of the event. The resulting effective upper limit of measurement for ML is about 6.5 and about 8 for Ms.
New techniques to avoid the saturation problem and to measure magnitudes rapidly for very large earthquakes are being developed. One of these is based on the long period P-wave, the other is based on a recently discovered channel wave.
The energy release of an earthquake, which closely correlates to its destructive power, scales with the 3⁄2 power of the shaking amplitude. Thus, a difference in magnitude of 1.0 is equivalent to a factor of 31.6 ( = (101.0)(3 / 2)) in the energy released; a difference in magnitude of 2.0 is equivalent to a factor of 1000 ( = (102.0)(3 / 2) ) in the energy released. The elastic energy radiated is best derived from an integration of the radiated spectrum, but one can base an estimate on mb because most energy is carried by the high frequency waves.
The Richter magnitude of an earthquake is determined from the logarithm of the amplitude of waves recorded by seismographs (adjustments are included to compensate for the variation in the distance between the various seismographs and the epicenter of the earthquake). The original formula is:
where A is the maximum excursion of the Wood-Anderson seismograph, the empirical function A0 depends only on the epicentral distance of the station, δ. In practice, readings from all observing stations are averaged after adjustment with station-specific corrections to obtain the ML value.
Because of the logarithmic basis of the scale, each whole number increase in magnitude represents a tenfold increase in measured amplitude; in terms of energy, each whole number increase corresponds to an increase of about 31.6 times the amount of energy released, and each increase of 0.2 corresponds to a doubling of the energy released.
Events with magnitudes greater than about 4.6 are strong enough to be recorded by a seismograph anywhere in the world, so long as its sensors are not located in the earthquake's shadow.
The following describes the typical effects of earthquakes of various magnitudes near the epicenter. The values are typical only and should be taken with extreme caution, since intensity and thus ground effects depend not only on the magnitude, but also on the distance to the epicenter, the depth of the earthquake's focus beneath the epicenter, and geological conditions (certain terrains can amplify seismic signals).
Magnitude Description Earthquake effects Frequency of occurrence Less than 2.0 Micro Micro earthquakes, not felt. Continual 2.0–2.9 Minor Generally not felt, but recorded. 1,300,000 per year (est.) 3.0–3.9 Often felt, but rarely causes damage. 130,000 per year (est.) 4.0–4.9 Light Noticeable shaking of indoor items, rattling noises. Significant damage unlikely. 13,000 per year (est.) 5.0–5.9 Moderate Can cause major damage to poorly constructed buildings over small regions. At most slight damage to well-designed buildings. 1,319 per year 6.0–6.9 Strong Can be destructive in areas up to about 160 kilometres (99 mi) across in populated areas. 134 per year 7.0–7.9 Major Can cause serious damage over larger areas. 15 per year 8.0–8.9 Great Can cause serious damage in areas several hundred kilometres across. 1 per year 9.0–9.9 Devastating in areas several thousand kilometres across. 1 per 10 years (est.) 10.0+ Massive Never recorded, widespread devastation across very large areas; see below for equivalent seismic energy yield. Extremely rare (Unknown/May not be possible)
(Based on U.S. Geological Survey documents.)
The following table lists the approximate energy equivalents in terms of TNT explosive force – though note that the earthquake energy is released underground rather than overground. Most energy from an earthquake is not transmitted to and through the surface; instead, it dissipates into the crust and other subsurface structures. In contrast, a small atomic bomb blast (see nuclear weapon yield) will not simply cause light shaking of indoor items, since its energy is released above ground.
Following, 31.623 to the power of 0 equals 1, 31.623 to the power of 1 equals 31.623 and 31.623 to the power of 2 equals 1000. Therefore, an 8.0 on the Richter scale releases 31.623 times more energy than a 7.0 and a 9.0 on the Richter scale releases 1000 times more energy than a 7.0.
Approximate Magnitude Approximate TNT for
Seismic Energy Yield
Joule equivalent Example 0.0 15 g 63 kJ 0.2 30 g 130 kJ Large hand grenade 0.5 85 g 360 kJ 1.0 480 g 2.0 MJ Small construction site blast 1.5 2.7 kg 11 MJ 2.0 15 kg 63 MJ 2.5 85 kg 360 MJ 3.0 480 kg 2.0 GJ 3.5 2.7 metric tons 11 GJ PEPCON fuel plant explosion, 1988 3.87 9.5 metric tons 40 GJ Explosion at Chernobyl nuclear power plant, 1986 3.91 11 metric tons 46 GJ Massive Ordnance Air Blast bomb 4.0 15 metric tons 63 GJ 4.3 43 metric tons 180 GJ Kent Earthquake (Britain), 2007 4.5 85 metric tons 360 GJ Tajikistan earthquake, 2006 5.0 480 metric tons 2.0 TJ Lincolnshire earthquake (UK), 2008
5.5 2.7 kilotons 11 TJ Little Skull Mtn. earthquake (Nevada, USA), 1992
5.6 3.8 kilotons 16 TJ Newcastle Earthquake Australia, 1989
Sparks Earthquake (Oklahoma, USA), 2011
6.0 15 kilotons 63 TJ Double Spring Flat earthquake (Nevada, USA), 1994 6.3 43 kilotons 180 TJ MW Rhodes earthquake (Greece), 2008
Christchurch earthquake (New Zealand), 2011
6.4 60 kilotons 250 TJ Kaohsiung earthquake (Taiwan), 2010
Vancouver earthquake (Canada), 2011
6.5 85 kilotons 360 TJ MS Caracas earthquake (Venezuela), 1967
MW Eureka earthquake (California, USA), 2010
6.6 120 kilotons 500 TJ MW San Fernando earthquake (California, USA), 1971 6.7 170 kilotons 710 TJ MW Northridge earthquake (California, USA), 1994 6.8 240 kilotons 1.0 PJ MW Nisqually earthquake (Anderson Island, WA), 2001
6.9 340 kilotons 1.4 PJ MW San Francisco Bay Area earthquake (California, USA), 1989
7.0 480 kilotons 2.0 PJ MW Java earthquake (Indonesia), 2009
7.1 680 kilotons 2.8 PJ MW Messina earthquake (Italy), 1908
7.2 950 kilotons 4.0 PJ Vrancea earthquake (Romania), 1977
MW Baja California earthquake (Mexico), 2010
7.5 2.7 megatons 11 PJ MW Kashmir earthquake (Pakistan), 2005
7.6 3.8 megatons 16 PJ MW Gujarat earthquake (India), 2001
7.7 5.4 megatons 22 PJ MW Sumatra earthquake (Indonesia), 2010 7.8 7.6 megatons 32 PJ MW Tangshan earthquake (China), 1976
8.0 15 megatons 63 PJ MS Mino-Owari earthquake (Japan), 1891
San Juan earthquake (Argentina), 1894
San Francisco earthquake (California, USA), 1906
MS Queen Charlotte Islands earthquake (B.C., Canada), 1949
MW Chincha Alta earthquake (Peru), 2007
MS Sichuan earthquake (China), 2008
Kangra earthquake, 1905
8.1 21 megatons 89 PJ México City earthquake (Mexico), 1985
Guam earthquake, August 8, 1993
8.35 50 megatons 210 PJ Tsar Bomba - Largest thermonuclear weapon ever tested 8.5 85 megatons 360 PJ MW Sumatra earthquake (Indonesia), 2007 8.7 170 megatons 710 PJ MW Sumatra earthquake (Indonesia), 2005 8.75 200 megatons 840 PJ Krakatoa 1883 8.8 240 megatons 1.0 EJ MW Chile earthquake, 2010, 9.0 480 megatons 2.0 EJ MW Lisbon earthquake (Portugal), All Saints Day, 1755
MW 2011 Tōhoku earthquake and tsunami (Japan)
9.15 800 megatons 3.3 EJ Toba eruption 75,000 years ago; among the largest known volcanic events. 9.2 950 megatons 4.0 EJ MW Anchorage earthquake (Alaska, USA), 1964
MW Sumatra-Andaman earthquake and tsunami (Indonesia), 2004
9.5 2.7 gigatons 11 EJ MW Valdivia earthquake (Chile), 1960 10.0 15 gigatons 63 EJ Never recorded 12.55 100 teratons 420 ZJ Yucatán Peninsula impact (creating Chicxulub crater) 65 Ma ago (108 megatons; over 4x1030 ergs = 400 ZJ). 32 1.5×1043 tons 6.3×1052 J Approximate magnitude of the starquake on the magnetar SGR 1806-20, registered on December 27, 2004.
- Quakes using the more modern magnitude scales will denote their abbreviations: MW and MS. Those that have no denoted prefix are ML. Please be advised that the magnitude "number" (example 7.0) displayed for those quakes on this table may represent a significantly greater or lesser release in energy than by the correctly given magnitude (example MW).
- Largest earthquakes by magnitude
- Seismic scale
- Mercalli intensity scale
- Moment magnitude scale
- Japan Meteorological Agency seismic intensity scale
- Order of magnitude
- Rohn Emergency Scale for measuring the magnitude (intensity) of any emergency
- ^ The Richter Magnitude Scale
- ^ "USGS Earthquake Magnitude Policy". USGS. March 29, 2010. http://earthquake.usgs.gov/aboutus/docs/020204mag_policy.php.
- ^ William L. Ellsworth (1991). SURFACE-WAVE MAGNITUDE (Ms) AND BODY-WAVE MAGNITUDE (mb). USGS. http://www.johnmartin.com/earthquakes/eqsafs/safs_694.htm. Retrieved 2008-09-14.
- ^ Kanamori
- ^ Richter, C.F., 1936. "An instrumental earthquake magnitude scale", Bulletin of the Seismological Society of America 25, no., 1-32.
- ^ Richter, C.F., "Elementary Seismology", edn, Vol., W. H. Freeman and Co., San Francisco, 1956.
- ^ Hanks, T. C. and H. Kanamori, 1979, "Moment magnitude scale", Journal of Geophysical Research, 84, B5, 2348.
- ^ "Richter scale". Glossary. USGS. March 31, 2010. http://earthquake.usgs.gov/hazards/qfaults/glossary.php.
- ^ Di Giacomo, D., Parolai, S., Saul, J., Grosser, H., Bormann, P., Wang, R. & Zschau, J., 2008. Rapid determination of the enrgy magnitude Me, in European Seismological Commission 31st General Assembly, Hersonissos.
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- ^ USGS: Measuring the Size of an Earthquake, Section 'Energy, E'
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- ^ This is what Richter wrote in his Elementary Seismology (1958), an opinion copiously reproduced afterwards in Earth's science primers. Recent evidence shows that earthquakes with negative magnitudes (down to −0.7) can also be felt in exceptional cases, especially when the focus is very shallow (a few hundred metres). See: Thouvenot, F.; Bouchon, M. (2008). What is the lowest magnitude threshold at which an earthquake can be felt or heard, or objects thrown into the air?, in Fréchet, J., Meghraoui, M. & Stucchi, M. (eds), Modern Approaches in Solid Earth Sciences (vol. 2), Historical Seismology: Interdisciplinary Studies of Past and Recent Earthquakes, Springer, Dordrecht, 313–326.
- ^ 
- ^ USGS: List of World's Largest Earthquakes
- ^ FAQs – Measuring Earthquakes
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- IRIS Real-time Seismic Monitor of the Earth
- USGS: magnitude and intensity comparison
- USGS: Earthquake Magnitude Policy
- USGS: 2000–2006 Earthquakes worldwide
- USGS: 1990–1999 Earthquakes worldwide
- Alaska Railroad Earthquake with a table of yield-to-magnitude relations.
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