Abstracts with Programs - Geological Society of America
Abstracts with Programs - Geological Society of America
Abstracts with Programs - Geological Society of America
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SESSION NO. 28<br />
has been sheared during shock compression and from which short, parallel lamellae emanate<br />
in one direction, typically at an angle <strong>of</strong> 50-60°. Analysis <strong>of</strong> multiple sets <strong>of</strong> FFs in natural<br />
samples shows that all FF lamellae <strong>with</strong>in a sample trend in roughly the same direction, while<br />
the sheared PFs form conjugate sets at ~90° angles. The principal axis <strong>of</strong> stress <strong>of</strong> the shock<br />
wave is therefore assumed to lie at a 45° angle to the conjugate sets and parallel to the FF<br />
lamellae. Thus FFs can be used as indicators for the orientation <strong>of</strong> differential stress <strong>with</strong>in the<br />
shock wave.<br />
Although the generation <strong>of</strong> FFs as a shear-induced structure is clear in principle, details<br />
<strong>of</strong> their formation are not yet completely understood. Specifically, the quartz grain’s lattice is<br />
commonly distorted near the shear fracture, visible as an undulatory extinction pattern under<br />
the microscope. In conventional structural geology, the orientation <strong>of</strong> this lattice distortion forms<br />
as the result <strong>of</strong> “dragging” <strong>of</strong> material along the shear plane. Surprisingly, FFs show the exact<br />
opposite orientation.<br />
EBSD measurements are currently being performed on FFs to analyze lattice deformation<br />
at a high resolution. Based on these initial results, we suggest that lattice deformation along<br />
the PF is caused by elastic lattice strain accumulated during shearing in the shock wave,<br />
which is then rapidly released during unloading, resulting in the opening <strong>of</strong> the FF lamellae<br />
as extensional fractures (mode I) while rotating the lattice between two individual lamellae,<br />
causing additional mode II in-plane shear along the lamellae and resulting in a distortion<br />
pattern visible in EBSD measurements. Preliminary TEM analyses show that the junctions <strong>of</strong><br />
the FF lamellae <strong>with</strong> the PF are filled <strong>with</strong> vesicular amorphous material. Further EBSD and<br />
TEM work is planned to give more detailed insights into the kinematics <strong>of</strong> dynamic fracturing<br />
and shearing. A deeper understanding <strong>of</strong> this process can potentially be used to constrain<br />
and differentiate fracturing mechanisms in shock waves from fracturing in lower-dynamic,<br />
tectonic regimes.<br />
28-6 BTH 6 Grokhovsky, Victor<br />
THE FAILURE OF METEORITES IN IMPACT TESTS: THE EFFECT OF STRUCTURE AND<br />
TEMPERATURE<br />
GROKHOVSKY, Victor1 , GLADKOVSKY, Sergey2 , KOZLOVSKIKH, Ekaterina1 ,<br />
and PYATKOV, Anton1 , (1) Physico-Technical, Ural Federal University, Mira St, 19,<br />
Ekaterinburg, 620002, Russia, grokh47@mail.ru, (2) Institute <strong>of</strong> Engineering Science <strong>of</strong><br />
the Ural Branch <strong>of</strong> RAS, Ekaterinburg, 620219, Russia<br />
There are few data about mechanical properties and behavior <strong>of</strong> meteoroids under shock load,<br />
yet these properties are crucial to understanding how to deal <strong>with</strong> asteroidal and cometary<br />
threat. In addition meteoroids were loaded dynamically during mutual impact action, interaction<br />
<strong>with</strong> atmosphere and earth surface. However, previously the majority <strong>of</strong> strength data were<br />
obtained from compressive tests while only few experimental results in this field were related<br />
to tensile tests. In this work we present the numerical results on impact strength and crack<br />
propagation resistance <strong>of</strong> both different meteoritic materials and ice.<br />
Dynamic tests were performed using instrumented Tinius Olsen IT542 impact test machine<br />
at 300–77 K. Samples were prepared from monocrystalline and polycrystalline fragments <strong>of</strong><br />
octahedrite Sikhote-Alin IIAB, impact-reheated meteorite Dronino (Iron-ung), ataxite Chinga<br />
IVB, chondrite Tsarev L5 and ice. SEM JEOL JSM-66490LV and TESCAN VEGA were used for<br />
fracture surface analysis <strong>of</strong> studied fragments. The SEM pictures were quantitatively processed<br />
using image analysis system SIAMS 700.<br />
The highest values <strong>of</strong> impact strength (2210 kJ/m2 and 2070 kJ/m2 ) and maximum <strong>of</strong><br />
crack propagation energy were obtained for Chinga and Dronino iron meteorites which had<br />
submicroscopical (α+α +γ) and duplex (α+α ) structures, respectively. Decrease <strong>of</strong> the test<br />
2 2<br />
temperature down to 77 K led to decrease <strong>of</strong> impact strength values down to 47 kJ/m2 for<br />
Dronino and 1170 kJ/m2 for Chinga meteorites. Monocrystalline Sikhote-Alin meteorite samples<br />
demonstrated brittle transcrystalline fracture surface mode while polycrystalline Sikhote-Alin<br />
samples were characterized by intercrystalline fracture mechanism. In this case fracture<br />
energy was less than that for Tsarev L5 chondrite. The performed study clears up that the<br />
process <strong>of</strong> meteoritic materials failure is strongly affected by their chemical composition, type<br />
<strong>of</strong> microstructure and test temperature. It may be a result <strong>of</strong> different values <strong>of</strong> impact strength,<br />
impact testing parameters (ratio <strong>of</strong> crack initiation, propagation and total fracture energy) along<br />
the side <strong>with</strong> fracture mechanism transfer from ductile to brittle transcrystalline mode. This work<br />
was supported in part by the RFBR grant No 10-05-96047-r-ural-à.<br />
SESSION NO. 29, 08:30<br />
Tuesday, 6 September 2011<br />
T3D. Induced Seismicity – From Observation to<br />
Geomechanical Understanding (Posters)<br />
Ludwig-Maximilians-Universität München,<br />
Poster Hall P1 (E110, Senatsraum, 1st floor)<br />
29-1 BTH 27 Chernyavski, Vladimir M.<br />
MODELING OF THE TEMPORAL EVOLUTION OF EFFECTIVE STRESS, PORE PRESSURE,<br />
COMPACTION, FILTRATION, AND GROWING OF GAS HYDRATES IN THE CASE OF<br />
THE SEQUENTIAL ACCUMULATION OF SEDIMENTARY LAYERS WITH DIFFERENT<br />
RHEOLOGICAL PROPERTIES<br />
CHERNYAVSKI, Vladimir M., Institute <strong>of</strong> Mechanics, Lomonosov Moscow State University,<br />
Michurinskii pr. 1, Moscow, 119192, Russia, vcherniavski@gmail.com and SUETNOVA,<br />
Elena I., Institute <strong>of</strong> Physics <strong>of</strong> the Earth, Russian Academy <strong>of</strong> Sciences, B. Gruzinskaya<br />
10, IFZ, Moscow, 123995, Russia<br />
The processes <strong>of</strong> the evolutions <strong>of</strong> the effective stress, compaction, and fluid and gas filtrations<br />
in the permeable sedimentary rocks during their sequential accumulation are described in the<br />
frame <strong>of</strong> a poro-visco-elastic (Maxwell-type) constitutive law. But such a process is disturbed<br />
by the precipitation and accumulations <strong>of</strong> a species in its P-T stability zones. This processes<br />
lead to decreasing <strong>of</strong> porosity and permeability. Mathematical model <strong>of</strong> coupled processes<br />
<strong>of</strong> sediment compaction, pore fluid and gas migration and pore feeling by precipitation is<br />
developed.<br />
Mathematical formulation <strong>of</strong> physical problem <strong>of</strong> low-viscosity fluid- gas flow in a deformable<br />
poro-visco-elastic matrix <strong>with</strong> moving boundary consists <strong>of</strong> the system <strong>of</strong> nonlinear partial<br />
differential equations <strong>with</strong> appropriate boundary conditions. Because the permeability<br />
nonlinearly depends upon porosity, and the effective pressure gradient is interrelated <strong>with</strong><br />
deformation <strong>of</strong> sediment matrix under the loading, the dynamic <strong>of</strong> fluid is controlled by the<br />
behavior <strong>of</strong> deformable matrix.<br />
Calculations <strong>with</strong> parameters that are <strong>with</strong>in the framework <strong>of</strong> the available geophysical data<br />
show that the accumulation <strong>of</strong> sedimentary layers <strong>with</strong> a permeability or viscosity differing from<br />
that <strong>of</strong> the main basin fill leads <strong>with</strong> time to the formation, deep <strong>with</strong>in the basin, <strong>of</strong> layers that<br />
have a higher porosity and a different overhydrostatic pore pressure as compared <strong>with</strong> the<br />
surrounding layers. The lower-viscosity layer <strong>of</strong> sediment is compacted more rapidly, thereby<br />
creating an obstacle for the pore fluid and gas motion toward the surface. Subsequently, as the<br />
A42 FRAGILE EARTH: <strong>Geological</strong> Processes from Global to Local Scales<br />
overlying sedimentary layers accumulate, the compaction process leads to the formation <strong>of</strong> two<br />
zones above and below the lower-viscosity layer, in each <strong>of</strong> which the porosity decrease <strong>with</strong><br />
increasing depth becomes more pronounced <strong>with</strong> time. The pore pressure in the lower zone<br />
increases more rapidly than in the upper one due to a rapid porosity decrease in the lowerviscosity<br />
layer. On model examples shown as a sequential accumulation <strong>of</strong> porous sediments<br />
<strong>with</strong> different viscosity quantitatively affects on the evolution and contemporary values <strong>of</strong><br />
effective stress, pore pressure, fluid and gas filtration and accumulation <strong>of</strong> gas hydrates in<br />
the pores.<br />
29-2 BTH 28 Eckert, Andreas<br />
CO2 INJECTION IN ANTICLINE RESERVOIRS: STRUCTURAL INFLUENCES ON MAXIMUM<br />
SUSTAINABLE PORE PRESSURE AND SEISMICITY RELATED TO FAULT REACTIVATION<br />
ECKERT, Andreas, PARADEIS, Matthew, and AMIRLATIFI, Amin, Petroleum Engineering,<br />
Missouri University <strong>of</strong> Science and Technology, Rolla, MO 65409, eckertan@mst.edu<br />
Anticline structures are one <strong>of</strong> the most common structural traps for hydrocarbon reservoirs<br />
and are thus becoming prime targets for geologic CO sequestration into saline formations.<br />
2<br />
The injection <strong>of</strong> CO into geologic formations increases the formation pore pressure and<br />
2<br />
induces geomechanical risks such as fracture reactivation or the generation <strong>of</strong> new fractures.<br />
This will result in seismicity and lastly generate preferred fluid flow pathways along which<br />
dissolved CO may escape into the atmosphere. In order to assess these geomechanical risks<br />
2<br />
a thorough simulation coupling fluid flow through porous media and geomechanics <strong>of</strong> a realistic<br />
representation <strong>of</strong> the formation <strong>of</strong> interest is required.<br />
In this study we use a one-way coupling approach transferring pore pressure results<br />
from a reservoir simulator to geomechanical models using finite element analysis. From<br />
the mechanical finite element models, we initially determine the maximum sustainable pore<br />
pressure before CO injection. Our geomechanical models show that structural parameters<br />
2<br />
such as anticline amplitude and wavelength, layer thickness and intra-bedding friction under<br />
various stress regimes have a significant impact on the maximum sustainable pore pressure in<br />
the reservoir.<br />
After injection we study the spatial and temporal CO plume evolution in the reservoir<br />
2<br />
and transfer the resulting pore pressures back to the geomechanical models. We include a<br />
preferably oriented fault in the model and propose 2 procedures to simulate fault reactivation.<br />
Our models show that CO induced pore pressure increase can trigger reactivation <strong>of</strong> pre-<br />
2<br />
existing structures and based on the resulting fault slip the resulting seismic magnitudes can<br />
be estimated.<br />
29-3 BTH 29 López, Allan<br />
TRIGGERED SEISMICITY EXPECTED IN HYDROELECTRIC RESERVOIRS CLOSE TO THE<br />
SUBDUCTION ZONE IN COSTA RICA<br />
LÓPEZ, Allan, Engineering Geology, I.C.E, UEN PYSA, Sabana Norte, San Josè 1000<br />
Costa Rica, alopezs@ice.go.cr<br />
The tectonic stress field imparted by the subducting Cocos plate on the Caribbean plate along<br />
the central pacific region in southern Costa Rica and the changes in the associated fluid<br />
pressure and friction during impoundment and drawdown <strong>of</strong> hydropower reservoirs, determine<br />
the reactivation <strong>of</strong> faults and pre-existing discontinuities and the formation <strong>of</strong> new ones. The<br />
geomechanical attributes <strong>of</strong> the present day stress field, the rockmass properties and the ways<br />
in which they are combined according to the local and regional geological structure, lithology<br />
and rock matrix in association <strong>with</strong> the prevailing tectonic regimes, control the likelihood <strong>of</strong><br />
fault reactivation. Some variables such as impoundment-drawdown rates and speeds can be<br />
modified, but it can not be done for the subduction related and background seismicity. In this<br />
context adequate modeling <strong>of</strong> the reactivation must take into consideration the stress and fluid<br />
pressures required to start the hydr<strong>of</strong>racturing, opening and sliping <strong>of</strong> faults networks.<br />
In one <strong>of</strong> the analyzed cases in a reservoir <strong>with</strong> a maximum depth <strong>of</strong> 162 meters in Tertiary<br />
turbidites crosscrossed by NW dextral active faults and reverse NWW structures <strong>with</strong>in a stress<br />
field <strong>with</strong> a subhorizontal σ trending towards N22°E, the hydr<strong>of</strong>racturing must be at least 9.<br />
1<br />
02652e + 006 Pa to start and 4. 82652e + 006 Pa to open the existing faults. The Slip Tendency<br />
analysis indicates that only the reverse faults dipping less than 15 ° are prone to reactivate<br />
under the stated conditions while the dextral shears shall move when their strikes are in the<br />
range <strong>of</strong> N40°W to N10°E. The sensitivity <strong>of</strong> these variables in a scenario <strong>with</strong> a major seismic<br />
event has been shaped by a Coulomb Stress Failure modeling, which indicated that the stress<br />
transfer induced by a maximum credible Mw 6,5 earthquake <strong>with</strong> inverse geometry and 30%<br />
<strong>of</strong> dextral component would not increase the seismic hazard at any depth in the area <strong>of</strong> direct<br />
influence <strong>of</strong> the reservoir.<br />
29-4 BTH 30 Haghi, Amir Hossein<br />
EVALUATION AND ANALYSIS OF RESERVOIR FLUID FLOW EFFECT ON FIELD<br />
STRESS; A NEW APPROACH TO ALLEVIATE INDUCED SEISMICITY IN HYDROCARBON<br />
RESERVOIRS<br />
HAGHI, Amir Hossein, Research Center <strong>of</strong> Petroleum University <strong>of</strong> Technology, Tehran,<br />
1453953153, Iran, amirh886@yahoo.com, KHARRAT, Riyaz, Petroleum University<br />
<strong>of</strong> Technology, Tehran, 1453953153, Iran, and ASEF, M.R., Geology, Tarbiat Moalem<br />
University, Tehran, 1453953153, Iran<br />
Annually, natural and artificial earthquakes cause irreparable damages for human communities.<br />
Induced seismicity which refers to human-made shocks and tremors that alters the stresses<br />
state on the Earth’s crust, invigorates in form <strong>of</strong> hydrocarbon reservoir-induced seismic that is<br />
related to operations <strong>with</strong> changing reservoir stress states. As it is provided in many references<br />
and research projects, reservoir stress field is a strong function <strong>of</strong> reservoir pore pressure.<br />
Hence long term production and injection scenarios or stimulation activities influence the stress<br />
state <strong>of</strong> reservoir based on time and place in the reservoir span.<br />
Among all indicated parameters including long term production-injection operations,<br />
stimulation, and reservoir pressure variations in time and place, there is another key parameter<br />
named fluid flow rate which could be controlled by us to calm down stress disruption and thus<br />
alleviate induced seismicity magnitude in hydrocarbon reservoirs. During reservoir stimulation,<br />
long term production- injection, the only parameter which is altered dramatically and caused<br />
some hazards is the fluid flow rate in the well and all situations in reservoir. Reservoir pressure<br />
is a strong function <strong>of</strong> fluid flow rate and thus filed stress could be formulized based on that in<br />
reservoir as well.<br />
In this approach using diffusivity equation in reservoir space and solving it <strong>with</strong> analytical and<br />
numerical methods, reservoir pressure is related to fluid flow in all distance from the producing<br />
well to reservoir boundary for all times steps. Accordingly, reservoir stress state could be<br />
formulated based on production flow rates. During single or multi wall production, sensitive<br />
locations around the flowing wells have the biggest chance for induced seismicity. Regarding<br />
that flow rate is the only attainable tool in order to control the intensity <strong>of</strong> stress confliction,<br />
this method proves numerically “How much dividing the producing fluid flow into several ways<br />
will lessen the chance <strong>of</strong> stress confliction and induced seismicity in Hydrocarbon Reservoir<br />
Spaces”.<br />
The accuracy <strong>of</strong> this method is confirmed using production data and numerical models <strong>of</strong> two<br />
giant hydrocarbon fields located in western section <strong>of</strong> Persian Gulf, Southern Iran.