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Monitoring Ground Deformation at Volcanoes: Case Studies of two New Methods—InSAR and GPS Geodesy Henry L. Turner GEOL 4553/5553 Volcanology April 7, 2009 • Volcano monitoring techniques • Ground deformation associated with volcanoes: Sources and spatial/temporal scales • Traditional methods for studying volcanic ground deformation • New methods—InSAR and GPS geodesy • Case studies using InSAR and GPS geodesy • Conclusions Volcano Monitoring Techniques From http://volcanoes.usgs.gov/About/What/Monitor/monitor.html Sources of ground deformation at Volcanoes • Movement of magma Influx of magma—inflation Outflux of magma—deflation Injection of sills, laccoliths, and dikes • Changes in the local hydrothermal system generally slow uplift or subsidence e.g., Yellowstone caldera • Gravitational spreading subsidence • Tectonic motion background motion Spatial/temporal scales of deformation • Movement of magma ranges from large scale, rapid deformation near the vent to smaller scale slower deformation distal to the volcano • Changes in the local hydrothermal system generally slow uplift or subsidence over relatively long time scales • Gravitational spreading slow subsidence • Tectonic motion background motion ≤ plate rates Traditional methods for studying volcanic ground deformation • Basic Field Measurements Fault offsets Opening of cracks • Traditional surveying Trilateration and Triangulation Leveling surveys Electronic Distance Measurements (EDM) • Tiltmeters • Strainmeters From Dvorak and Dzurisin, 1997. From Dvorak and Dzurisin, 1997. Basic Field Measurements Cracks in the crater floor at Mt. St. Helens. Orange line is ~1m long. Photographs by D.A. Swanson in August 1982. From http://volcanoes.usgs.gov/About/What/Monitor/Deformation/GrndDefrm.html Lava Dome Fault Scarp Crater Floor Measuring the distance between two benchmarks across a thrust fault at the base of the dome at Mt. St. Helens. This scarp developed on the crater floor in 1981 as magma rose into the lava dome (backgound) before erupting onto its surface. Photograph by T. Leighley on 26 August 1981. Sketch by B. Myers From http://volcanoes.usgs.gov/Products/Pglossary/fault_more.html Traditional surveying • Trilateration • Triangulation • Leveling surveys • Electronic Distance Measurements (EDM) Triangulation consists of a series of connected triangles which adjoin or overlap each other, angles being measured from determined fixed stations. A known base-line measurement is required. Three examples of triangulation systems are shown below. Trilateration uses electronic distance measuring equipment to directly measure the lengths of the sides of triangles from which the angles can be calculated. It is a very useful method for rough terrain where positions can be accurately carried forward. Leveling is the operation of determining differences of elevation by measuring vertical distances directly on a graduated rod with the use of a leveling instrument such as a dumpy level, transit or theodolite. The difference in elevation between two points can also be determined trigonometrically using vertical angles and horizontal or inclined distances. From http://education.qld.gov.au/curriculum/area/maths/compass/html/surveying/sutec.html Electronic Distance Measurements (EDM) Mt. St. Helens Closing distance between two benchmarks located on the dome and at the EDM station on the crater floor before the May 14, 1982, eruption (vertical red line). As magma pushed the side of the dome outward, the distance to the EDM station became smaller. The steep curves indicate that the dome moved outward at increasing rates right up to the eruption. For example, the dome was moving about 2 cm/day on May 2; the movement increased to about 200 cm/day by May 13. From http://volcanoes.usgs.gov/About/What/Monitor/Deformation/EDMMSH.html Photograph by R.B. Moore on 22 November 1977 Mokuaweoweo caldera, summit of Mauna Loa The distance between two benchmarks located on the east and west rim of Mokuaweoweo increased during the 1975 and 1984 eruptions of Mauna Loa. During the onset of both eruptions (red lines), rising magma forced the caldera apart by about 50 cm. More was learned about the extension and eruption processes of Mauna Loa during this time period than in all earlier historic eruptions. From http://volcanoes.usgs.gov/About/What/Monitor/Deformation/EDMMaunaLoa.html Locations of baselines that are measured in the Long Valley Caldera, near Mammoth Lakes, Calif., using a two-color laser distance measuring instrument (geodimeter). The twocolor geodimeter measures distances to a precision of 0.5 to 1.0 mm for ranges between 3 and 8 km. The locations of these baselines are shown in relation to sources of inflation that have been modeled using both these data and leveling data. Plot of the changes in length of 8 frequently measured baselines. These baselines, which use the central station at CASA as a common end point, have been measured approximately 3 times each week since early 1984. The general trend of the data is 1) a general decrease in the rate of extension from 1983 through most of 1989, 2) an abrupt increase in the rate of extension on several baselines to 5 cm/ yr from late 1989 through early 1990, and 3) a decrease to 2 to 3 cm/yr extension rate that has persisted since mid-1990. From http://quake.wr.usgs.gov/research/deformation/twocolor/longvalley.html Tiltmeters Installing a tiltmeter on Montserrat in 1995. From http://volcanoes.usgs.gov/About/What/Monitor/Deformation/Tilt.html Pinnacle tiltmeters operate on the same principle as a carpenter’s level. At the core of each tiltmeter is a pair of orthogonal bubble levels with a precise curvature.Electrodes detect minute movements of the air bubble within a conductive fluid as the fluid seeks the lowest spot in the sensor.The series 5000 tiltmeter can resolve tilt as little as one billionth of a radian (or 0.00000005 degrees). From http://www.pinntech.com/subs/about/pubs/series5000.pdf Strainmeters Sacks-Evertson single-component dilatometer schematic How does a dilatometer work? Magma movements, earthquakes, and other natural phenomena deform the volcanic edifice. This distortion squeezes the dilatometer, which is filled with oil. The amount of strain is precisely measured by metering the flow of oil into or out of the dilatometer. Dilatometers are so sensitive that they can easily detect the small deformations of the Earth's crust caused by gravitational attractions of the sun and moon and by the loads applied to the Earth's surface by passing weather fronts. From http://hvo.wr.usgs.gov/volcanowatch/2000/00_04_27.html A. Linde’s models of single-component dilatometer data from Iceland NB that strain signal preceded Surface eruption by several hours! New methods—InSAR and GPS geodesy SAR Interferometry (InSAR) interferometry: interaction between superimposed wave trains Two waves traveling that are offset by amount, A …A is phase difference Use two antennae…one offset slightly closer to surface…difference is A One antenna transmits pulse, but returns received by both;…difference in distance of antennae from surface ensures that return arrives at one antenna before other, resulting in phase difference interferogram… two waves superimposed to generate one resultant wave resultant wave is record of interference of two waves may be displayed as image by assigning gray-scale or color spectrum to each cycle (crest to crest) each cycle is an interference fringe …image is an interferogram because phase difference is recorded: possible to measure cm offsets imaging geometry for a repeat-pass interferometer one interferogram is formed with images acquired from positions A1 and A2 (generate topography; DEM) second interferogram is formed with A1 and A2’ if an earthquake has occurred between time 1 and time 2 additional displacement affects the path length (surface change) satellites at positions A1 and A2 at time 1 satellite at position A2’ at time 2 centimeter-scale differences in elevation possible to detect topography generated from INSAR (ERS) DEM interferogram Siberia surface change from INSAR: displacement along strike-slip fault Landers, 1993 first example more fault ruptures… GPS Geodesy GPS Geodesy is a sophisticated way of surveying using a constellation of satellites as a “fixed” reference frame. Positions of fixed benchmarks can be determined at cm level accuracy. D Methods • Data acquisition Installation of geodetic network, campaign observations, & continuous site data • Data processing SVs transmit two microwave carrier (carry information) signals L1 (1575.42 MHz): carries navigation message; SPS code (SPS: standard positioning service) L2 (1227.60 MHz): measures ionospheric delay 3 binary codes shift L1 and/or L2 carrier phases C/A code (coarse acquisition) modulates L1 carrier phase …repeating 1 MHz pseudo random noise (PRN) code …pseudo-random because repeats every 1023 bits or every millisecond…each SV has its own C/A code …basis for civilian SPS P-code (precise) modulates both L1 and L2 …long (7 days) pseudo random 10 MHz noise code …basis for PPS (precise positioning service) …AS (anti-spoofing) encrypts P-code into Y-code (need classified module for receiver) navigation message modulates L1-C/A; 50 Mhz signal ….describes satellite orbits, clock corrections, etc. Using GPS geodesy, we can measure motions on the order of a few millimeters per year. This permits us to examine motion of lithospheric plates (cm/yr), some motions related to intraplate deformation, and other types of surface deformation (e.g. Volcanic). How do we accomplish this? • receivers that record both L1 and L2 • measurements acquired for minimum 2-3 days on site • sophisticated processing that uses all GPS data in GIPSY-OASIS II (JPL) with precise orbits & clocks • sites are fixed spots campaign: occupied intermittently marked by stainless steel pin that is epoxied into bedrock/monument continuous: occupied permanently receiver and antenna installed at site Using GPS geodesy to observe intraplate surface deformation We use a precise point-positioning approach Euler pole • establish positions of individual points relative to a global reference frame (ITRF00) using GIPSY • re-occupy individual points after appropriate time interval, which depends on estimates of plate deformation • calculate changes in point positions to constrain velocities of sites • determine surface deformation field by comparing velocities of sites with velocities predicted by plate velocity model Site velocities relative to fixed plate Site velocities relative to fixed plate Observed site velocities in ITRF00 Predicted linear plate velocities in ITRF00 Surface deformation field GIPSY Flow Chart Advantages of GPS Geodesy and InSAR for measuring volcanic ground deformation GPS Geodesy • High precision • Doesn’t require line of sight between benchmarks • Continuous sites operate without requiring presence of humanoids • Cheap InSAR • Measurements made remotely—no humanoid endangerment • Can acquire images from numerous volcanoes • Entire deformation field may be imaged rather than isolated points Limitations of GPS Geodesy and InSAR for measuring volcanic ground deformation GPS Geodesy • Sampling of deformation field limited to individual points, which must be chosen carefully • Meaurements of campaign sites and installation and maintenance of continuous sites may place humanoids in danger • Continuous sites may be destroyed by volcanic activity InSAR • Small scale deformation may not be imaged (need >2.8 cm) • Difficulties in using the technique on densely vegetated or snow covered volcanoes. Case studies using InSAR and GPS geodesy GPS Geodesy • Long Valley Caldera • Unzen Volcano • Mount Etna InSAR • Long Valley Caldera • Mount Etna • Galápagos Volcanoes • Mount Peulik, Westdahl, Makushin, and Okmok volcanoes, Alaska Long Valley Caldera and Mono-Inyo Craters Volcanic Field, California Long Valley caldera, located at the boundary between the Sierra Nevada and the Basin and Range Province, is one of the largest Quaternary rhyolitic volcanic centers in North America. The caldera is elliptical in shape and 10 by 20 miles (15 by 30 km) in size. The Long Valley caldera was produced by a catastrophic eruption about 730,000 years ago. The roof above the magma chamber collapsed, forcing 150 cubic miles (600 cubic km) of rhyolitic magma to the surface in the form of Plinian ash columns and associated air falls and ash flows. The volume of ash is comparable to similar caldera-forming eruptions at Yellowstone. Photo from http://www.es.ucsc.edu/~anewman/research/LVC.html Owens River Gorge Photo by R. Forrest Hopson. Bishop Tuff The Bishop tuff was erupted during the catastrophic eruption that created Long Valley caldera. After the catastrophic eruption, volcanism continued on the caldera floor, producing a thin layer of rhyolitic tephra and lava. Pressure increased within the magma chamber and forced the overlying rocks upward, forming a resurgent dome. The resurgent dome formed within 100,000 years after the caldera. Eruptions 500,000, 300,000, and 100,000 years ago along the periphery of the resurgent dome produced thick, steep-sided rhyolitic lava flows and domes. These volcanic products are the youngest lavas to originate from the magma chamber. Dixon et al., 1997 Newman et al., 2001 Simons and Fialko Interferogram from a descending orbit with radar acquisition dates of June 6, 1996, and July 12, 1998. The InSAR data reveal a domal uplift of the Earth surface within the Long Valley caldera, with a maximum displacement of ~10 cm in the satellite line of sight (LOS) direction. We invert the InSAR data for two ``endmember'' source geometries, a sill, and a prolate finite spheroid of arbitrary orientation. Because details of the source geometry cannot be resolved with only one component of the displacement field, we include in our analysis the two-color laser geodimeter data (data courtesy of J. Langbein, USGS). http://www.cacr.caltech.edu/SDA/insar.html http://igpphelp.ucsd.edu/~fialko/ Unzen, Japan Location: 32.75 N, 130.30 E Elevation: 4,457, feet (1,359 m) Photo from Steve O'Meara Volcano Watch International Unzen is a large complex volcano made of several adjacent and overlapping lava domes. The volcano covers much of the Shimabara Peninsula and is east of the city of Nagasaki. In 1792, collapse of the Mayu-yama lava dome created an avalanche and tsunami that killed an estimated 14,524 people. Most of the people were killed by the tsunami. After the 1792 eruption Unzen was dormant for 198 years. The 1990 eruption was preceded by a swarm of earthquakes that began in November 1989. A phreatic eruption on November 17, 1990, marked the onset of the most recent eruption of Unzen. The eruption resumed on February 12, 1991. A volcanic dome made of dacite lava began to grow on May 20, 1991. The dome continued to grow for four more years. During this time pyroclastic flows were frequently generated by the collapses of lava blocks from margins of the dome. During 1991-1994, approximately ten thousand pyroclastic flows were counted on Unzen. Landslides also generated large pyroclastic flows that traveled as far as 3.4 miles (5.5 km) from the dome. On June 3, 1991, one of these pyroclastic flows killed 43 people, including noted volcanologists Maurice and Katia Krafft and Harry Glicken. Pyroclastic flows from Unzen during intense activity on June 3-4, 1991. Matsushima and Takagi, 2000 Horizontal displacement at FGI continuous GPS station. The rapid expansion by the rise of magma was observed from the end of February to the beginning of April 1993. In mid-April the movement was reversed, and stopped early in May. Displacement observed from Jan 24, 1994 to Feb. 27 (35 days). Values are horizontal/vertical displacements in unit of meter. Wide arrows represent the directions of inflation of the Lava dome. Etna, Italy Location: 37.73N, 15.00E Elevation: 10,991 feet (3,350 m) Looking south along the coast of Sicily to Etna. Taormina is in the foreground. Photograph by Mike Lyvers taking during the 1993 eruption. Bonaccorso et al., 2002 Aloisi et al., 2003 October 2002 eruption July 2001 eruption Massonnet et al., 1995 Hawaii upper images: DEMS lower image: surface change Mt. Etna Westdahl, Unimak Island, Alaska Location: 54.00 N, 164.85 W Elevation: 5,118 ft. (1,560 m) Westdahl is a glacier-covered shield volcano located on Unimak Island. This volcano's most recent activity dates back to February 1978. Lu et al., 2000 Observed interferogram 1993-1998 Modeled interferogram for 0.5 km3 magma intrusion The model suggests that a magma body about 8 km (5 miles) beneath the center of the volcano expanded by about 50 million cubic meters (65 million cubic yards) from 1993 to 1998. If the model is correct, the summit area would have been uplifted about 17 cm. Name: PEULIK VOLCANO Type: STRATOVOLCANO WITH SUMMIT DOMES Location: 540 KM SOUTHWEST OF ANCHORAGE Latitude, Longitude: 57°45'N, 156°21'W Elevation: 1474 M From http://www.avo.alaska.edu/avo4/atlas/Peulik.htm This interferogram represents deformation between October 1996 to September 1997. It shows a striking bull's-eye fringe pattern centered on the southwest flank of the volcano. Six fringes that represent about a total of about 17 cm (6.7 inches) of uplift map out the deformation pattern in considerable detail. Other interferograms for the period from September 1997 to September 1998 reveal one more fringe, corresponding to about 3 cm (1.1 inches) of additional uplift. Conclusions • GPS geodesy and InSAR are powerful new techniques for monitoring surface deformation at volcanoes and can help in forecasting eruptive activity • Like any method of observation, both have their limitations— therefore, using multiple methodologies will give us the best picture of deformation References Volcano World, http://volcano.und.nodak.edu/vw.html USGS Volcano Hazards Program, http://volcanoes.usgs.gov/About/What/Monitor/monitor.html Aloisi, M., Bonaccorso, A., Gambino, S., Mattia, M., and Puglisi, G., 2003, Etna 2002 eruption imaged from continuous tilt and GPS data, GRL, 30, 23. Amelung, F., Jónsson, S. Zebker, H., and Segall, P., 2000, Widespread uplift and ‘trapdoor’ faulting on Galápagos volcanoes observed with radar interferometry, Nature, 407, 993–996. Battaglia, M, Segall, P., Murray, J., Cervelli, P., and Langbein, J., 2003, The mechanics of unrest at Long Valley caldera, California: 1. Modeling the geometry of the source using GPS, leveling and two-color EDM data, Journal of Volcanology and Geothermal Research, 127, 3-4, 195–217. Bonaccorso, A., Aloisi, M., and Mattia, M., 2002, Dike emplacement forerunning the Etna July 2001 eruption modeled through continuous tilt and GPS data, GRL, 29, 13. Bonforte, A., and Puglisi, G., 2003, Magma uprising and flank dynamics on Mount Etna volcano, studied using GPS data (1994–1995), JGR, 108, B3. Dixon, T. H., Mao, A., Bursik, M. I., Heflin, M. B. Langbein, J. Stein, R. S., and Webb F. H., 1997, Continuous monitoring of surface deformation at Long Valley Caldera, California, with GPS, JGR, 102, 12,017–12,034. Dvorak, J. and Berrino, G., 1991, Recent ground movement and seismic activity in Campi Flegrei, Southern Italy: Episodic growth of a resurgent dome, JGR, 96, 2309–2323. Dvorak, J. and Dzurisin, D., 1997, Volcano geodesy: The search for magma reservoirs and the formation of eruptive vents, Reviews of Geophysics, 35, 343–384. Lu Z., Power, J. A., McConnell, V. S., Wicks, C., and Dzurisin, D., 2002, Preeruptive inflation and surface interferometric coherence characteristics revealed by satellite radar interferometry at Makushin Volcano, Alaska: 1993–2000, JGR, 107, B11. Lu Z., Wicks, C., Dzurisin, D., Power, J. A., Moran, S. C., and Thatcher, W., 2002, Magmatic inflation at a dormant stratovolcano: 1996–1998 activity at Mount Peulik volcano, Alaska, revealed by satellite radar interferometry, JGR, 107. Lu Z., Wicks, C., Dzurisin, D., Thatcher, W., Freymueller, J. T., McNutt, S. R., and Mann, D., 2000, Aseismic inflation of Westdahl volcano, Alaska, revealed by satellite radar interferometry, GRL, 27, 1567–1570. Lundgren, P., Berardino, P., Coltelli, M., Gornaro, G., Lanari, R., Puglisi, G., Sansosti, E., and Tesauro, M., 2003, Coupled magma chamber inflation and sector collapse slip observed with synthetic aperture radar interferometry on Mt. Etna volcano, JGR, 108, B5. 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W., 1997, Catastrophic collapse at stratovolcanoes induced by gradual volcano spreading, Nature, 387, 387–390.