PREDICTING EARTHQUAKES & EARTHQUAKE HAZARDS: WHY SO LITTLE SUCCESS? Seth Stein Northwestern University “Only fools and charlatans predict earthquakes” Charles Richter (1900-1985) Tohoku, Japan 2011 M 9.1 QuickTime™ and a decompressor are needed to.
Download ReportTranscript PREDICTING EARTHQUAKES & EARTHQUAKE HAZARDS: WHY SO LITTLE SUCCESS? Seth Stein Northwestern University “Only fools and charlatans predict earthquakes” Charles Richter (1900-1985) Tohoku, Japan 2011 M 9.1 QuickTime™ and a decompressor are needed to.
PREDICTING EARTHQUAKES & EARTHQUAKE HAZARDS: WHY SO LITTLE SUCCESS? Seth Stein Northwestern University “Only fools and charlatans predict earthquakes” Charles Richter (1900-1985) Tohoku, Japan 2011 M 9.1 QuickTime™ and a decompressor are needed to see this picture. Scientists will “be able to predict earthquakes in five years.” Louis Pakiser U.S. Geological Survey, 1971 1970’s optimism “We have the technology to develop a reliable prediction system already in hand.” Alan Cranston, U.S. senator, 1973 “The age of earthquake prediction is upon us” U.S. Geological Survey, 1975 Similar in Japan, China, USSR Meaningful prediction involves specifying the location, time, & size of an earthquake before it occurs Long-term forecast - Use earthquake history to predict next one - Use rate of motion accumulating across fault and amount of slip in past earthquakes Short-term prediction -Find precursors - changes in earth before earthquakes consistently resolvable from normal variability Despite some claims, no reliable method yet… Need to do consistently better than expected by chance from known statistics of earthquakes in an area Postdictions - Texas sharp shooter Shoot at barn and then draw target around bullet holes SAN FRANCISCO EARTHQUAKE April 18, 1906 3000 deaths 28,000 buildings destroyed (most by fire) $10B damage “The whole street was undulating as if the waves of the ocean were coming toward me.” “I saw the whole city enveloped in a pile of dust caused by falling buildings.” “Inside of twelve hours half the heart of the city was gone” Motion along ~ 500 km of previously unrecognized San Andreas Fault ~ 4 m of ground motion West side moved north USGS ELASTIC REBOUND Over many years, rocks on opposite sides of the fault move, but friction on fault "locks" it and prevents slip Eventually strain accumulated overcomes friction, and fault slips in earthquake Took 60 years to figure out why this happens! EARTH’S OUTER SHELL - PLATES Plates move at few cm/yr San Andreas fault: boundary between Pacific & North American plates Hard to predict when block will slip PARKFIELD, CALIFORNIA SEGMENT OF SAN ANDREAS M 5-6 earthquakes about every 22 years: 1857, 1881, 1901, 1922, 1934, and 1966 In 1985, expected next in 1988; U.S. Geological Survey predicted 95% confidence by 1993 Occurred in 2004 (16 years late) Discounting misfit of 1934 quake predicted higher confidence Science, 10/8//04 "Parkfield is geophysics' Waterloo. If the earthquake comes without warnings of any kind, earthquakes are unpredictable and science is defeated. " (The Economist) No precursors in seismicity (foreshocks), strainmeters, magnetometers, GPS, creepmeter $30 million spent on “Porkfield” project GPS: GLOBAL POSITIONING SYSTEM Satellites transmit radio signals Receivers on ground record signals and find their position from the time the signals arrive Find mm/yr motions from changes in position over time Stein & Wysession, 2003 San Andreas: GPS site motions show deformation accumulating that will be released in future earthquakes Like a deformed fence GPS SLIP RATE 35 mm/yr Z.-K. Shen Over time, slip in large earthquakes adds up to plate motion About 35 mm/yr motion between Pacific and North America shown by offset stream Expect large earthquakes about every 4 m / (35 mm/yr) or 115 years Last one here in 1857… San Andreas Fault “We are predicting another massive earthquake certainly within the next 30 years and most likely in the next decade or so.” W. Pecora, U.S. Geological Survey Director, 1969 1975 PALMDALE BULGE – uplift reported SAF USGS director stated that “a great earthquake” would occur “in the area ... possibly within the next decade” that might cause up to 12,000 deaths, 48,000 serious injuries, 40,000 damaged buildings, and up to $25 billion in damage. California Seismic Safety Commission stated that “the uplift should be considered a possible threat to public safety” and urged immediate preparations… 35 years later, nothing yet.. WHY CAN’T WE PREDICT EARTHQUAKES? So far, no clear evidence for consistent precursors before earthquakes. Maybe lots of tiny earthquakes happen frequently, but only a few grow by random process to large earthquakes In chaos theory, small perturbations can have unpredictable large effects - flap of a butterfly's wings in Brazil might set off a tornado in Texas If there’s nothing special about the tiny earthquakes that happen to grow into large ones, the time between large earthquakes is highly variable and nothing observable should occur before them. If so, earthquake prediction is either impossible or nearly so. At present No reliable method of predicting earthquakes No present approaches seem promising Barring conceptual breakthrough, earthquake prediction appears unlikely soon “It is hard to predict earthquakes, especially before they happen.” Hiroo Kanamori To design buildings and other mitigation measures, make maps that try to predict the hazard defined as maximum shaking (acceleration) that will occur in some time period Frankel et al., 1996 Map shows central US as hazardous as California How credible is it? Underprediction 2001 hazard map 2010 M7 earthquake shaking much greater than predicted for next 500 years http://www.oas.org/cdmp/document/seismap/haiti_dr.htm 6 mm/yr fault motion Even at fast moving (80 mm/yr ) & seismically very active plate boundaries with long seismic history, hard to assess earthquake hazard Map assumed high hazard in Tokai “gap” 2011 M 9.1 Tohoku, 1995 Kobe M 7.3 & others in areas mapped as low hazard Geller 2011 Planning assumed maximum magnitude 8 Seawalls 5-10 m high Tsunami runup approximately twice fault slip (Plafker, Okal & Synolakis 2004) M9 generates much larger tsunami NYT CNN Lack of M9s in record seemed consistent with model that M9s only occur where lithosphere younger than 80 Myr subducts faster than 50 mm/yr (Ruff and Kanamori, 1980) Disproved by Sumatra 2004 M9.3 and dataset reanalysis (Stein & Okal, 2007) Short record at most SZs didn’t include larger multisegment ruptures Stein & Okal, 2011 Tsunami radiates energy perpendicular to fault Thus largest landward of highest slip patches http://www.coastal.jp/tsunami2011/index.ph p?FrontPage http://www.geol.tsukuba.ac.jp/~ yagi-y/EQ/Tohoku/ Historical record of large tsunamis QuickTime™ and a decompressor are needed to see this picture. NYT 4/20/11 NY Times 3/21/11 Maps fail because of - bad physics (incorrect description of earthquake processes) -bad assumptions (mapmakers’ choice of poorly known parameters) - bad data (lacking, incomplete, or underappreciated) - bad luck (low probability events) and combinations of these Accuracy of hazard map prediction depends on accuracy of answers assumed to hierarchy of four basic questions Where will large earthquakes occur? When will they occur? How large will they be? How strong will their shaking be? Uncertainty & map failure result because these are often poorly known “A game of chance against nature, of which we still don't know all the rules” (Lomnitz, 1989) Where will large earthquakes occur? When will large earthquakes occur? How large will they be? How strong will the shaking be? Slow plate boundary Africa-Eurasia convergence rate varies smoothly (5 mm/yr) NUVEL-1 Argus, Gordon, DeMets & Stein, 1989 Swafford & Stein, 2007 GSHAP 1999 Slow plate boundary Africa-Eurasia convergence rate varies smoothly (5 mm/yr) NUVEL-1 Argus, Gordon, DeMets & Stein, 1989 2003 2004 M 6.4 Swafford & Stein, 2007 M 6.3 GSHAP 1999 2008 Wenchuan earthquake (Mw 7.9) was not expected: map showed low hazard USGS Hazard map - assumed steady state - relied on lack of recent seismicity Didn’t use GPS data showing 1-2 mm/yr Earthquakes prior to the 2008 Wenchuan event Aftershocks of the Wenchuan event delineating the rupture zone M. Liu Long record needed to see real hazard 1933 M 7.3 1929 M 7.2 Swafford & Stein, 2007 Map depends greatly on assumptions & thus has large uncertainty GSC “Our glacial loading model suggests that earthquakes may occur anywhere along the rifted margin which has been glaciated.” Stein et al., 1979 1985 Concentrated hazard bull's-eyes at historic earthquake sites 2005 Diffuse hazard along margin Plate Boundary Earthquakes •Major fault loaded rapidly at constant rate •Earthquakes spatially focused & temporally quasi-periodic Past is fair predictor Plate B Plate A Earthquakes at different time Intraplate Earthquakes •Tectonic loading collectively accommodated by a complex system of interacting faults •Loading rate on a given fault is slow & may not be constant •Earthquakes can cluster on a fault for a while then shift Past can be poor predictor Stein, Liu & Wang 2009 New Madrid 1991: because paleoseismology shows large events in 900 & 1450 AD, like those of 1811-12 GPS studies started, expecting to find strain accumulating consistent with large events ~500 years apart Science, April 1999 We found little or no motion: Seismicity migrates Recent cluster transient, possibly ending Hazard overestimated Similar behavior in other continental interiors “Large continental interior earthquakes reactivate ancient faults … geological studies indicate that earthquakes on these faults tend to be temporally clustered and that recurrence intervals are on the order of tens of thousands of years or more.” (Crone et al., 2003) Liu, Stein & Wang 2011 during the period prior to the period instrumental events Earthquakes in North China Beijing Bohai Bay Ordos Plateau 1303 Hongtong M 8.0 Weihi rift Large events often pop up where there was little seismicity! Liu, Stein & Wang 2011 during the period prior to the period instrumental events Earthquakes in North China Beijing Bohai Bay Ordos Plateau Weihi rift 1556 Huaxian M 8.3 Large events often pop up where there was little seismicity! Liu, Stein & Wang 2011 during the period prior to the period instrumental events Earthquakes in North China Beijing Bohai Bay Ordos Plateau Weihi rift 1668 Tancheng M 8.5 Large events often pop up where there was little seismicity! Liu, Stein & Wang 2011 during the period prior to the period instrumental events Earthquakes in North China 1679 Sanhe M 8.0 Beijing Bohai Bay Ordos Plateau Weihi rift Large events often pop up where there was little seismicity! Liu, Stein & Wang 2011 during the period prior to the period instrumental events Earthquakes in North China 1975 Haicheng M 7.3 Beijing 1976 TangshanBohai Bay M 7.8 Ordos Plateau 1966 Xingtai M 7.2 Weihi rift Large events often pop up where there was little seismicity! No large (M>7) events ruptured the same fault segment twice in past 2000 years Historical Instrumental Weihi rift In past 200 years, quakes migrated from Shanxi Graben to N. China Plain Maps are like ‘Whack-a-mole’ - you wait for the mole to come up where it went down, but it’s likely to pop up somewhere else. Where will large earthquakes occur? When will large earthquakes occur? How large will they be? How strong will the shaking be? EARTHQUAKE RECURRENCE IS HIGHLY VARIABLE Sieh et al., 1989 Extend earthquake history with paleoseismology M>7 mean 132 yr s 105 yr Estimated probability in 30 yrs 7-51% Assumed probability of large earthquake & thus hazard depend on recurrence model & position in earthquake cycle Time dependent predicts lower until ~2/3 mean recurrence Results depend on both model choice & assumed mean recurrence Hebden & Stein, 2008 Not clear which model works best where %106 154% 2% in 50 yr (1/2500 yr) Effect larger in Memphis Large uncertainty in maps Where will large earthquakes occur? When will large earthquakes occur? How large will they be? How strong will the shaking be? Gutenberg-Richter relationship (1944): log10 N = a -b M N = number of earthquakes occurring ≥ M a = activity rate (y-intercept) b = slope (commonly called b-value) M = Magnitude Simple power-law distribution controlled by the scale invariance of earthquakes (e.g. Turcotte, 1997) Useful for estimating the recurrence of large earthquakes from a given fault or region Mmax crucial for hazard models GUTENBERG-RICHTER RELATIONSHIP: INDIVIDUAL FAULTS Wasatch instrumental data Characteristic Basel, Switzerland historical data Uncharacteristic paleoseismic data paleoseismic data Youngs & Coppersmith, 1985 Meghraoui et al., 2001 Largest events deviate in either direction, often when different data mismatch When more frequent than expected termed characteristic earthquakes. Alternative are uncharacteristic earthquakes These - at least in some cases - are artifacts of short history that overpredict or underpredict hazard SHORT HISTORY SIMULATIONS 10,000 synthetic earthquake histories for G-R relation with slope b=1 Gaussian recurrence times for M> 5, 6, 7 Various history lengths given in terms of Tav, mean recurrence for M>7 For histories = 0.5 Tav any M7 earthquakes appear characteristic, since can’t observe fractions of earthquakes Thus either overestimate rate of largest earthquakes or underestimate Mmax Stein & Newman 2004 SHORT SIMULATIONS Often overestimate rate of largest earthquakes or underestimate Mmax Where will large earthquakes occur? When will large earthquakes occur? How large will they be? How strong will the shaking be? Effects of assumed ground motion model trade off with Mmax Effect as large as one magnitude unit Frankel model, developed for maps, predicts significantly greater shaking for M > 7 Frankel M 7 similar to Atkinson & Boore or Toro M 8 Models use various combinations, e.g. 1996 averaged Frankel & Toro models; Atkinson & Boore not used Newman et al., 2001 PREDICTED HAZARD ALSO DEPENDS GREATLY ON 180% - Assumed maximum magnitude of largest events -Assumed ground motion model -Neither are well known since large earthquakes rare Newman et al., 2001 275% What to do Realistically assess uncertainties and present them candidly to allow users to decide how much credence to place Develop methods to objectively test hazard maps and thus guide future improvements Global warming forecasts present uncertainties by showing factor of 3 range of model predictions IPCC 2007 Warming by 2099 The AOGCMs cannot sample the full range of possible warming, in particular because they do not include uncertainties in the carbon cycle. In addition to the range derived directly from the AR4 multi-model ensemble, Figure 10.29 depicts additional uncertainty estimates obtained from published probabilistic methods using different types of models and observational constraints: the MAGICC SCM and the BERN2.5CC coupled climate-carbon cycle EMIC tuned to different climate sensitivities and carbon cycle settings, and the C4MIP coupled climate-carbon cycle models. Based on these results, the future increase in global mean temperature is likely to fall within –40 to +60% of the multi-model AOGCM mean warming simulated for each scenario. This range results from an expert judgement of the multiple lines of evidence presented in Figure 10.29, and assumes that the models approximately capture the range of uncertainties in the carbon cycle. The range is well constrained at the lower bound since climate sensitivity is better constrained at the low end (see Box 10.2), and carbon cycle uncertainty only weakly affects the lower bound. The upper bound is less certain as there is more variation across the different models and methods, partly because carbon cycle feedback uncertainties are greater with larger warming. In addition to comparing maps, comparing model predictions shows the large uncertainties resulting from different assumptions Shows contributions to logic tree before subjective weighting Testing analogy: evidence-based medicine objectively evaluates widely used treatments Although more than 650,000 arthroscopic knee surgeries at a cost of roughly $5,000 each were being performed each year, a controlled experiment showed that "the outcomes were no better than a placebo procedure." QuickTime™ and a decompressor are needed to see this picture. Need objective criteria to test maps by comparison to what happened after they were published. One is to compare maximum acceleration observed over the years to that predicted by both map and null hypotheses. A simple null hypothesis is regionally uniformly distributed seismicity. Japanese map seems to be doing worse than this null hypothesis, implying overparametrized model Geller 2011 Detailed model of segments with 30 year probabilities Off Sanriku-oki North ~M8 0.2 to 10% Off Sanriku-oki Central~M7.7 80 to 90% Off Miyagi ~M7.5 > 90% Off Fukushima ~M7.4 7% Off Ibaraki ~M6.7 – M7.2 90% Expected Earthquake Sources 50 to 150 km segments M7.5 to 8.2 (Headquarters for Earthquake Research Promotion) Sanriku to Boso M8.2 (plate boundary) 20% Sanriku to Boso M8.2 (Intraplate) 4-7% J. Mori Giant earthquake broke all of the segments Expected Earthquake Sources 50 to 150 km segments M6.7 to 8.2 (Headquarters for Earthquake Research Promotion) 2011 Tohoku Earthquake 450 km long fault, M 9.1 (Aftershock map from USGS) J. Mori Some testing challenges 1) Short time record: can in some cases be worked around. For example, North China record probably has almost or all M7s in 2000 years. Paleoseismology can go back even further, with higher probability of missing some. 2) Subjective nature of hazard mapping, resulting from need to chose faults, maximum magnitude, recurrence model, and ground motion model. This precludes the traditional method of developing a model from the first part of a time series and testing how well it does in the later part. That works if the model is "automatically" generated by some rules (e.g. least squares, etc). In the earthquake case, this can't be done easily because we know what happens in the later part of the series. Summary - Hazard maps depend dramatically on unknown and difficult-to-assess parameters and hence on the mapmakers’ preconceptions - thus have large uncertainties that are generally underestimated and not communicated to public - sometimes either underpredict hazard (too much aseismic slip) in areas where large earthquakes occur - or overpredict hazard (too much seismic slip) Without objective testing, maps won’t improve & seismology will keep having to explain away embarrassing failures Challenge: Users Want Predictions Future Nobel Prize winner Kenneth Arrow served as a military weather forecaster. As he described, “my colleagues had the responsibility of preparing long-range weather forecasts, i.e., for the following month. The statisticians among us subjected these forecasts to verification and found they differed in no way from chance. The forecasters themselves were convinced and requested that the forecasts be discontinued. The reply read approximately: "The commanding general is well aware that the forecasts are no good. However, he needs them for planning purposes." Gardner, D., Future Babble: Why Expert Predictions Fail - and Why We Believe Them Anyway, 2010