Review on Modern Volcanology

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Presentation transcript:

Review on Modern Volcanology Takeshi Nishimura Department of Geophysics, Tohoku University Understanding the Magma Activity beneath Volcanoes Magma or volcanic fluids distributions Magma locations and behavior from geophysical observation (seismic, GPS, tilt, strain meters, etc.)

Outline: 3D seismic velocity structure beneath volcanoes Survey of magma reservoir/conduit Dike intrusion A case of failed eruption Conduit process in shallow volcanic conduits Bubbly magma/gas pocket

Survey of Magma by Seismic Tomography From IRIS website 𝑉 𝑃 = 𝐾+(4/3)𝜇 𝜌 P-wave velocity S-wave velocity K : Bulk Modulus m : Rigidity r : Density 𝑉 𝑆 = 𝜇 𝜌

Seismic Tomography Image beneath North Eastern Japan Grid Spacing for tomography H 12.5km V 5-15 km low VP, low VS, low VP/VS Presence of H2O low VP, low VS, high VP/VS Partial Molten Rocks / Magma Reservoir Nakajima et al. (2001)

Seismic Tomography beneath Mt. Fuji Deep Low Frequency Earthquakes (DLF), which are often inferred to be related to magma activity, are located at the region of: low VP, low VS, low VP/VS Supersaturated H2O, CO2 low VP, low VS, high VP/VS Partial Molten Rocks / Magma Reservoir Nakamichi et al. (2007)

Shallow Structure of Bandai Volcano View of Mount Bandai from the north. Large crater formed by a sector collapse during the1888 Eruption High-velocity zone is recognized beneath the summit. No evidence on magma chamber & conduit at shallow depths. These are common features of active volcanoes. Yamawaki et al. (2004)

Magma Locations are Detected by Geodetic Measurements GPS, Tilt meter, Strain meter Spatial Distributions of Deformations enable us to estimate: Locations of the pressure source Shape of the pressure source (Dike, Spherical, etc.) Strength of the pressure source (Volume Change)

Failed Eruption: 1998 Activity of Iwate Volcano, Japan Permanent stations Borehole tilt & strain SP seismometer >20 SP seismometers 6 STS-2 stations 3 tilt& strain meters >10 GPS stations

Why the magma did not migrate upward but horizontally intrude? Magma rises up due to buoyancy: Magma can migrate up when the density of magma is less than that of the surrounding rocks

Schematic illustration of Magma Ascent in Shallow Depth Views from Theoretical considerations & Geological sample analyses Deformation &Pylocrasts Opening of Conduit ・Without Degassing → Explosive Eruption    (Plinian-type) ・With Degassing  → Non-Explosive Eruption           (Lava Dome) Degassing , Out gassing Gas bubble growth In Situ Observation of Volatile Behavior is Necessary, but Plinian-type rarely occur. Nucleation of gas bubbles

Good observation targets to clarify the magma behavior Vulcanian eruptions Good observation targets to clarify the magma behavior Short-duration Repeatability Small magnitude Observations close to active vents Sakurajima (photo by Dr. Yokoo) Suwanose-jima

Repetitive Eruption from Open Conduit DP

Tilt meter can detect a tiny uplift toward the active crater which are caused by pressurization of shallow conduit Semeru volcano explodes every a few to tens of minutes Tilt meter Installation of tilt meter on the summit of Semeru volcano, Indonesia Example of observation

Seismic and Tilt Stations of Suwanosejima Volcano, Japanr Active Crater (after HP of Japan Coast Guard) 4 km and 8 km wide in EW and NS directions. 799m height

Monitor Seismograms Explosion Earthquake (EX) Continuous Tremor Ash emissions generate continuous tremor Explosion Earthquake (EX) Continuous Tremor EX EX EX EX

Seismic and Tilt Data Just Before Explosion Continuous Tremor associated with Ash Emissions Seismic UD Uplift toward the crater Tilt 3 NS 350 m Tilt 2 NS 700 m Tilt 1 NS 1000m Accumulation of ash/gas constantly supplied from deep conduit is inferred to be the origin of explosion

Uplift toward the crater Time of Eruption

Comparison of Tilt Stacked for Seismic Amplitude Average Amplitude of Explosion Earthquakes 184 m m/s Large Explosions accompany : Large amplitude and Long Duration of Inflation 49 m m/s

Possible Mechanism of Explosion at Suwanosejima Gas flow is stopped by a plug formed at the top of conduit Gas/Ash Flux Volcano Inflation Plug: Magma rheological changed due to cooling, degassing, crystallizing or stiffening Pressure Build Up Probably, low-density Continuous tremor Continuous tremor Constant Gas/Ash Supply

Summary Density structure is quite important to understand the magma processes. Three dimensional heterogeneity of the density in volcanic edifices may control the magma ascent. Recent geophysical measurements at active volcanoes suggest gas phase expansions in magma, which must be low-density, at shallow depths. But, not confirmed. Shallow conduit shape is an important factor to understand the volcanic eruptions.