Seismic Barrier Protection Of Critical Infrastructure

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Seismic Barrier Protection of CriticalInfrastructureRobert Haupt, Vladimir Liberman, andMordechai RothschildMIT Lincoln Laboratory244 Wood St. Lexington, MA 020420781-981-5128 Haupt@LL.mit.eduDISTRIBUTION STATEMENT A. Approved for public release:distribution unlimited. This material is based upon worksupported under Air Force Contract No. FA8721-05-C-0002and/or FA8702-15-D-0001. Any opinions, findings, conclusionsor recommendations expressed in this material are those of theauthor(s) and do not necessarily reflect the views of the U.S. AirForce. 2016 Massachusetts Institute of Technology.Deliveredto the U.S. Government with Unlimited Rights, as defined inDFARS Part 252.227-7013 or 7014 (Feb 2014).Notwithstanding any copyright notice, U.S. Government rights inthis work are defined by DFARS 252.227-7013 or DFARS252.227-7014 as detailed above. Use of this work other than asspecifically authorized by the U.S. Government may violate anycopyrights that exist in this work.I. IntroductionAbstract - Each year, on average a major magnitude-8earthquake strikes somewhere in the world. In addition,10,000 earthquake related deaths occur annually, wherecollapsing buildings claim by far most lives. Moreover, inrecent events, industry activity of oil extraction andwastewater reinjection are suspect to cause earthquake swarmsthat threaten high-value oil pipeline networks, U.S. oil storagereserves, and civilian homes. Earthquake engineering buildingstructural designs and materials have evolved over many yearsto minimize the destructive effects of seismic surface waves.However, even under the best engineering practices,significant damage and numbers of fatalities can still occur.In this paper, we present a novel concept and approach toredirect and attenuate the ground motion amplitudes caused byearthquakes by implementing an engineered subsurfaceseismic barrier – creating a form of metamaterial. The barrieris comprised of borehole array complexes and trench designsthat impede and divert destructive seismic surface waves froma designated ‘protection zone’. The barrier is also designed todivert not only surface waves in the aerial plane, but includesvertical ‘V’ shaped muffler structures composed of opposingboreholes to mitigate seismic waves from diffracting andtraveling in the vertical plane.Computational 2D and 3D seismic wave propagationmodels developed at MIT Lincoln Laboratory suggest that theborehole array and trench arrangements are critical to theredirection and self-interference reduction of broadbandhazardous seismic waves in the vicinity of the structure toprotect. The computational models are compared withexperimental data obtained from large bench-scale physicalmodels that contain scaled borehole arrays and trenches. Theseexperiments are carried out at high frequencies, but withsuitable material parameters and bore-hole dimensions. Theyindicate that effects of a devastating 7.0-magnitude earthquakecan be reduced to those of a minor magnitude-2 or -3eathquake within a suitable protection zone. These results arevery promising, and warrant validation in field scale tests.Keywords – seismic, metamaterials, borehole structures,earthquake mitigationDamage caused by earthquakes to critical structuressuch as nuclear power plants, regional hospitals,military installations, airport runways, pipelines, dams,and other infrastructure facilities exacerbates thedisaster and adds tremendous cost and time of recovery.Even low energy earthquakes resulting from humanactivity can cause significant damage as well. Forexample, wastewater reinjection practices used by theoil industry resulted in over 900 earthquakes in 20142015 in the state of Oklahoma, with a recent 2016 quakeof magnitude 5.8. These continual earthquake swarms,although many small, threaten extremely high valueabove and below ground pipelines that control oilsupply, storage, and transport in the U.S., and is a majoreconomic and environmental concern.Figure 1 (left) describes pictorially the differentkinds of seismic waves, including body waves andsurface waves. From the civil engineeringstandpoint, the most destructive are surface waves(Rayleigh, Love, shear). To protect against them, alarge body of earthquake engineering has beendeveloped, and effective building practices are beingroutinely applied to new construction.However,existing high value structures are unlikely to beretrofitted, thus posing significant risk to lives,economy, and the environment. Here, we propose anovel concept to redirect and attenuate the groundmotion of earthquake surface waves byimplementing an engineered below-ground seismicbarrier around such high value structures. As shownschematically in Figure 1 (right), the structuresproposed employ borehole arrays and trenchcomponents to act as broadband seismic wavebarriers that conceptually create a cloaking devicethat significantly reduces the energy that wouldotherwise reach an area we desire to protect, such asa power plant, oil pipeline complex, or other criticalstructures.

Figure 1. Left: Typical seismic wave types caused by earthquakes. Statistically, surface seismic waves (Rayleigh – groundroll, Love, Shear) can cause significant damage and destruction to man-nade structures in critical infrastructure. Right: Notionalborehole array concept that diverts and absorbs hazardous seismic waves prior to reaching critical infrastructure.II. Prior InvestigationsSeveral “earthquake cloaking” concepts havebeen proposed recently. The main limitation of theall the published approaches so far is the narrowband resonant nature of the structures, which do notaddress the typical bandwidth of a real-life tremor.Furthermore, there are limitations to scalability tolow frequencies (large structures) as well asapplicability to shear waves.(Colombi, et al,, Scientific Reports 2016, 6,19238.) suggested that tall above-ground structures,such as trees or steel towers, can be placedstrategically to absorb some of the ground vibrationsand dissipate seismic energy. However, from theprevious measurements and calculations, onlyenergy at discrete resonant frequencies can bedissipated with this approach. Furthermore, in orderto access frequencies below 1-10 Hz, the height ofthe above ground structures would have to be severalhundred meters, which is impractical.A second approach (Kim and Das, ModernPhysics Letters B 2013, 27) suggested that buryinglarge resonator tanks underground would convert theincident seismic energy into acoustic energy and,thereafter, into heat. Our analysis of this approachwith 3-dimensional finite element modeling foundthat only energy at discrete resonances can bedissipated. Furthermore, seismic shear waves cannotcouple into acoustic air filled resonator structures,thus reducing bthe utility of this approach preciselyfor the more damaging type of waves. Finally,because of great impedance mismatch between hardground and air, coupling of the resonances into theunderground tanks would be extremely inefficient, asmost of the energy would be reflected.A third approach (Krödel, S, et al. ExtremeMechanics Letters 2015, 4, 111-117)proposed burying seismic dampers into the groundfor energy dissipation. Once again, this approach isnarrowband and requires multiple resonant dampers,each working in a separate frequency band, to covera practical range of frequencies. In a scaledexperiment in a tank of sand, researchers found thatmany dozen different-size resonators would berequired to cover the relevant frequency spectrum.Scaling such approaches to full size would beimpractical.Finally, in the only controlled experimentsperformed in earth to date (Brule, et al., PhysicalReview Letters 2014, 112), a team from InstituteFresnel and Menard Construction company haveexcavated an array of several dozen holes in asedimentary basin outside of Grenoble, France. Theteam has studied elastic wave attenuation through thearray of these holes at a source frequency of 50 Hz,provided by a vibrocompactor. This experiment hasgenerated a large amount of excitement in thepopular media as it was the first and the only largescale demonstration of elastic wave diversion in soil.A modest attenuation of 3-5 dB was achieved by theborehole array. The major limitation of this

experiment is its reliance on the phononic crystalapproach, which is inherently narrowband and, often,direction-dependent. Furthermore, scaling thisphononic crystal design to frequencies below 1 Hzand to hard soil conditions that are prevalent in mostlocations would result in impractically large sizes forthe array structure.III. ‘V’ Shaped Opposing Borehole MufflerStructureBy contrast to the previously exploredapproaches, our design involves a broadbandborehole array structure, combining attenuation fromscattering theory as well as reflective muffler designsto enable not only aerial plane seismic wavediversion, but also vertical-depth plane protection.As described below, the muffler structures attenuateboth shear waves and surface waves, over thefrequency ranges relevant to earthquakes in both theaerial and vertical orientation planes.IV. Computer Modeling and Bench ScaleMeasurementsWe initially studied the phenomenology andfeasibility of using subsurface man-made structures toattenuate and divert hazardous seismic waves using 2Dand 3D computer numerical models. Our effortinvolved 1) identifying hazardous seismic waves fromearthquakes, 2) developing computational model ofseismic wave propagation in complex geological media,and 3) developing metamaterial models applicable toseismic cloaking to induce seismic wave diversion andattenuation. Modeling results show subsurface boreholearrays may reduce the seismic energy from hazardousearthquakes in the vicinity of high value structuralassets. Such seismic barrier structures may span 100s ofmeters to a kilometer in aerial range, with well depths of100 meters or less, and costs that would justifyconstruction. We conclude that such barrier arrays mayreduce seismic wave amplitudes by 30 – 50 dB thatwould otherwise reach a high value asset facility. Amodel is shown below using a recent Californiaearthquake’s parameters for input in figure 2.

Figure 2. Finite Difference Model of the effects on seismic wave propagation from seismic cloaking – barrierstructure. The seismic event is modeled for the response of the source function estimated for the Hector Mineearthquake in 1991 (Mag. 7.1 - USGS). Typical seismic frequencies are less than 1 Hz with minimal power above 1Hz. Top: Areal view of seismic wave snapshots, with and without cloaking structures. Bottom: Vertical – depth viewsnapshot of the effects of the cloaking – barrier device. Using a single vertical borehole array or trench maysignificantly reduce the surface wave energy reaching a protected region. However, energy is able to diffract aroundthe barrier. Using a V-shaped muffler is more effective in blocking surface waves in the 3D extent.We next studied borehole arrays and trenchesembedded in elastic media analogous to rock andcompact soil using a machined table-top scaled physicalmodel and compared with 3D computer modelingresults. The effort focused on examining the effects ofbarrier structures on seismic wave propagation,diversion, scattering, and attenuation through spatialmeasurements from controlled seismic sources. Thesolid model was composed of Delrin plastic with a Pwave speed of 1700m/s, S-wave speed of 855m/s, and adensity of 1.41g/cm3 representing reasonable earthmaterial analogs and is shown in figure 3. We observethat both 3D modeling of the Delrin block andmeasurements compare well within a factor of 2demonstrating that our modeling approach is valid andsupports merit to the seismic barrier concept.We next compare the effects of the barrierstructures on seismic wave reduction in terms ofearthquake magnitudes. In this analysis, we referencethe seismic power drop in dB to magnitude drop usingthe seismic moment magnitude scale, Mw. In figures 5and 6, the V-trench structure as modeled and measuredin the Delrin block is capable of reducing the seismicenergy reaching a protection zone from seriouslydestructiveand dangerous levels down to minor damage withminimal risk of incurring fatalities.Figure 3. Table-top experimental configuration.Delrin blocks were machined to contain boreholes inprescribed patterns or trenches defining a V-shapedmuffler and compared with homogeneous solidblocks.

Figure 4. 3D Finite Element Model of the effects on seismic wave propagation from V-shaped muffler seismiccloaking – barrier structure. The seismic event is modeled for the response of a Ricker Waveform source function.Figure 5. Measurement results showing effects of V-trench machined in delrin block Table-top experimentalconfiguration.Left: 4 accelerometer time series traces measured in the center line across a homogeneous solid delrin blockrelative to the transducer source location. Receiver 1, 3, 4, and 7 are 1, 3, 4, and 7 inches from the source. Particlevelocities are computed by integrating the measured accelerations and then applying a high-pass filter to removelow frequency drift. A single 10kHz Ricker vertical load burst is recorded as it travels from its source. Each tracerecords a similar time series, showing a direct surface wave arrival (circled outline) followed by later reflectionarrival interference from the delrin block side and bottom boundaries. The first break of the direct arrivals show awave speed of 1693m/s. Spherical spreading and delrin attenuation losses are not compensated in the measurementplots. At the observed wave speed, the P-wave length is estimated at 17mm.Right: 4 accelerometer time series traces measured in the center line across the delrin block that contains a Vtrench barrier structure perpendicularly oriented to the direction of elastic wave propagation relative to the

transducer source location. Receiver 1, 3, 4, and 7 are 1, 3, 4, and 7 inches from the source, where receivers 3 and4 are between the near and far trench walls. The trench barrier structure is shown in the green schematic to theright. The times series traces show that the direct surface wave is reflected off the near trench wall where, no tovery little direct wave is observed inside the keep out zone between the near and far trench walls. The reflectedarrival interference from the bottom surface is observed at the surface between the trench walls. In this geometry,elastic waves are able to leak through the aperture at the trench bottom and travel to the surface. These amplitudes,however, are lower than those of the peak surface wave that would be observed in the same locations if the barriercloaking structure is not present.We also model above the Delrin block and vibrational source using the 3D model described and observe that thecomputer models and measurements compare very closely as depicted in figure 6.Figure 6. 3D Finite Element Model of the effects on seismic wave propagation from V-shaped muffler seismiccloaking – barrier structure. Top: Model geometry and mesh representing geological media and V-shaped mufflerborehole / trench component structures. Bottom: In this simple analysis, the power drop observed in the measurementand model studies are presented in terms of Mw reduction. The V-trench structure shows that a magnitude 7.0earthquake energy intensity can be reduced to 5.4 – 5.0 for the peak power of the direct destructive surface wave. Theleakage through the aperture is measured to show a modest reduction. However, when modeling the earth, where theboundaries are infinite, diffraction leakage through the aperture is small and would provide a significant reduction.Discussion - ConclusionsConstructing subsurface borehole arrays have thepotential to divert, attenuate, and cause self-interferenceof seismic waves from earthquakes and significantlyreduce the impact of hazardous waves reaching adesignated building structure. Modeling and benchscale measurement results support this concept. Ournext milestone is to conduct measurement and modelingof a controlled outdoor experiment where we use awater well drilling truck to drill the borehole array. Acommercial seismic source will then be used to simulatethe close to those of an earthquake. We will thenmeasure before and after the emplacement of theborehole array to estimate it effectiveness: the amountof seismic wave power drop in a ‘protection zone’.

seismic wave propagation in complex geological media, and 3) developing metamaterial models applicable to seismic cloaking to induce seismic wave diversion and attenuation. Modeling results show subsurface borehole arrays may reduce the seismic energy from hazardous earthquakes in the vicinity of high value structural assets.

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