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THE SEDIMENT & ROCK MECHANICS LAB AT
PENN STATE
Equipment | Example Lab Data | Projects | Papers
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Back Row: Steve Swavely, Ki-Bok Min, Jon Samuelson, Matt Ikari, Rob Skarbek, Bryan
Kaproth, Demian Saffer, Derek Elsworth, Igor Faoro,
Josh Taron; Front Row: Ryan Jacoby, Hui Long, Insun Song, Andy
Rathbun, Peter “Tejas” Flemings, Chris
Marone, Brett Carpenter, Andre Niemeijer |
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We maintain a state-of-the-art
sediment mechanics laboratory, which hosts a high-pressure consolidation and
permeability system, as well as several computers for laboratory data
reduction. It is housed in a large shared rock/sediment mechanics laboratory
at Penn State, along with a biaxial shearing apparatus and true triaxial
system developed and maintained by Chris Marone. Our facility is equipped for
uniaxial sediment consolidation studies at loads up to 50 kN
(corresponding to stresses up to 100 MPa on 25 mm diameter samples), for
high-precision constant-flow rate permeability measurements on 25 mm, 38 mm
and 50 mm diameter core samples, and for triaxial deformation and
permeability measurements at confining pressures up to 70 MPa. The systems
are optimized for high-precision, long-term measurement of hydraulic and
mechanical properties, in which long duration stability of pressure/volume,
temperature, and load frame control are essential (for example, flow-through
permeability and/or consolidation experiments on fine-grained mudstones and shales that typically require several days to a few weeks
to complete). All of the
equipment can operate under either manual or computer control; typical tests
are run in computer control. We measure (or control) fluid volumes to +/- 1
mm3 (1 microliter), displacements to +/-
1 micron or less, and displacement rates to a precision of +/- 10-2
micron/min. We typically measure or control stress to +/- 1 kPa, but this can be modified by swapping load cells and
pressure transducers. For uniaxial deformation experiments, the sample cell
is a high-pressure fixed-ring oedometer vessel
designed jointly by Saffer and a private vendor (below). It consists of a cell base and top, which bolt together
at a mid-point allowing for easy sample insertion and access. The vessel
includes two fluid ports at the top, and two at the base. One pressure/volume
controller connected at the top and the other at the base – in order to
conduct singly or doubly drained consolidation experiments and flow-through
permeability measurements. The sample cell is rated to 10 MPa internal pore
pressure.
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For triaxial experiments, we use
three different cells: a low-pressure cell rated to 3 MPa confining pressure
(shown below), a medium-pressure
cell rated to 14 MPa, and a triaxial core holder rated for 70 MPa confining
pressure and up to 150 degrees C. The vessels are all interchangeable within
the load frame, and all allow measurement of permeability during deformation,
but differ slightly in their construction. The low-pressure vessel is
constructed from plexiglass, and is designed for
use with water or oil as a confining fluid. It has 4 ports for fluid or
electrical lines to pass into the vessel. These are typically used for
confining pressure and pore pressure, which can be
controlled separately at the sample base and top. The high pressure vessel is
constructed of 3-16 stainless steel, and is designed for use with oil as a
confining fluid. It has 8 ports for fluid or electrical lines, which allow
the use of additional measurement elements, including an internal load cell
for measurement of the axial stress without interference from the seal
friction (although this can be calibrated and is typically small) and a
radial strain gauge. The high pressure core holder is modified from a
commercial vendor; axial pressure is typically applied hydraulically, but can
also be applied mechanically (using a load frame). In our
experiments, samples are typically jacketed in latex with o-ring seals at the
top and base of the sample, and silicon oil is used as a confining fluid. Any
desired stress path within the apparatus maximum pressure and stress capability
can be achieved under (1) stress feedback control (controlled mean and
differential stress, resulting strain is monitored), (2) strain control
(controlled shortening rate and/or rate of volume change, resulting stresses
are monitored), or (3) manual control.
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We routinely measure permeability of marine sediments, fault gouge,
and wall rock as part of our studies. We obtain permeability data from
flow-through experiments (constant head or constant flow), and also through
constant rate of strain (CRS) tests. In the latter, a sample undergoes
uniaxial consolidation at a constant displacement rate, and we monitor the
pore pressure within the sample. The displacement rate is chosen such that
excess pore pressures are a small fraction (typically 2-5 %) of the effective
stress. The example below shows permeability for a suite of marine mudstones
sampled on the incoming oceanic plate outboard of the Nankai Trench during
ODP Leg 190. Small dots are data from CRS tests; filled colored symbols are from
flow-through tests, and gray circles are from Gamage
& Screaton (2006), shown for comparison.
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We also measure deformation behavior as part of
our research, in order to define sediment, fault gouge, and country rock rheology. As one example, we conduct consolidation
experiments on marine sediments in order to define compression properties.
Clay-rich sediments are especially interesting because they retain a
“memory” of their maximum past burial stress. Upon reloading to
effective stresses below the maximum past burial stress (known as preconsolidation stress or Pc’), samples follow a
primarily elastic recompression trajectory (below). At stresses beyond Pc’, the stress-strain behavior
changes and deformation is dominantly plastic. If specimens are handled
carefully enough during sampling and test preparation in the lab, these data
can be used to estimate in situ effective stress and pore
pressure. The plot below shows data for two samples from the Nankai Trough,
illustrating Pc’, recompression behavior, and plastic compression
behavior (described by the compression index Cc).
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SOME OF OUR ONGOING PROJECTS IN THE LAB
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Our
ongoing lab studies of permeability, deformation, and frictional behavior
include studies of subduction zone sediment and fault materials, in order to
understand the rock properties that govern the strength and sliding stability
of subduction megathrusts. For this project, our approach is to study a
unique suite of natural samples that span P-T conditions from seafloor
conditions up to depths of ~12 km and temperatures of 250 C (schematic above). These samples include
material from ODP boreholes offshore Costa Rica (CR) and at the Nankai Trough
(NT), in addition to outcrop samples from exhumed accretionary complexes and
strike-slip faults. We also
use permeability and consolidation measurements as a key component of our
research on pore pressure in subduction zones.
We use the laboratory permeability data to constrain numerical models of
fluid flow, and consolidation and triaxial tests to provide estimates of in
situ pore pressure. We
are also conducting measurements on core samples and cuttings from the SAFOD
borehole and on outcrop samples representing lithologic
units within the 3-D crustal volume containing the
San Andreas Fault and SAFOD hole. This work is described here. Photos to
right are from field outcrop sampling, showing serpentinite
from New Idria (top right), and en echelon
cracks in a road that crosses the creeping portion of the San Andreas Fault
North of Paso Robles, CA (bottom right).
Our
laboratory studies also include a range of studies that investigate the
effects of stress state on permeability, the role of deformation bands in
reducing the permeability of sandstone reservoirs and aquifers, the
relationships between mudrock porosity and stress
in complex stress settings (meaning non-uniaxial deformation), and most
recently, we are ramping a collaboration to study the permeability of coal
and the effects of flooding with water and CO2. |
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