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Tacoma, Washington (Dickenson and Brown 1997b). Additional data has been<br />

gleaned from laboratory testing of reconstituted specimens at <strong>Oregon</strong> <strong>State</strong><br />

University (Brown, in preparation). The geotechnical characterization for these<br />

sites included mud rotary borings, thin-wall tube samples in the low- to highplasticity<br />

silts, penetration resistances provided by SPT and CPT, as well as<br />

limited shear wave velocity and pore pressure data (excess pore pressures during<br />

cone advance and pore pressure dissipation in the fine sands and silts).<br />

Conventional cyclic triaxial and simple shear equipment was employed and<br />

modified with Bender elements for obtaining the shear wave velocity of the<br />

triaxial specimens, and with enhanced volume change instrumentation.<br />

It is well known that the results of cyclic triaxial data are not strictly<br />

representative of field behavior due to testing limitations, such as boundary<br />

conditions, stress paths, and uniform uni-directional loading. Additionally, the<br />

low to non-plastic nature of these soils makes undisturbed sampling very difficult.<br />

Any technique short of controlled ground freezing and coring would be expected<br />

to disturb the soil fabric and densify the material, thereby altering its behavior and<br />

its tendency to generate pore pressure. Determining the magnitude of such<br />

alterations is arduous. However, the qualitative nature of the effect is more<br />

predictable. For loose, saturated deposits with very low to no cohesion, the effects<br />

of sample disturbance densifies the samples and increases their liquefaction<br />

resistance during laboratory testing. For this reason, laboratory tests would likely<br />

overestimate the liquefaction resistance of the in situ soil to some degree. The<br />

cyclic testing does, however, yield useful data on the liquefaction resistance of<br />

predominantly silty soils relative to sandy soils tested using the same equipment.<br />

This data is considered particularly useful for demonstrating how the liquefaction<br />

behavior of the silts varies from that of sand, for which current empirical<br />

procedures for assessing liquefaction hazards are well established.<br />

The results of cyclic triaxial tests on silty soils from various sites in the Pacific<br />

Northwest are presented in Figure 3.11. Cyclic triaxial tests conducted on soils<br />

from the Puyallup River near Tacoma, Columbia River near Portland, and Fern<br />

Hill, <strong>Oregon</strong> are presented to demonstrate the cyclic resistance curves as a<br />

function of OCR. The data in Figure 3.11 clearly demonstrates the influence of<br />

stress history on the soil’s liquefaction resistance. This effect should be accounted<br />

for in hazard analyses involving overconsolidated soils. The geotechnical<br />

properties of the samples are provided in Table 3.8. The data for relatively<br />

undisturbed specimens of silt soils from the Pacific Northwest provided in Table<br />

3.8 are augmented with test results for reconstituted specimens, as well as the<br />

results of similar testing performed on other low plasticity silts (i.e., Bonnie silt<br />

and a silt from France). This data highlights the range in cyclic resistance<br />

obtained for the various silts using cyclic triaxial equipment. The data provided in<br />

Table 3.8 also demonstrates the influence of sample preparation on the measured<br />

behavior of the specimens. For example, the cyclic resistance of he Tacoma silt<br />

represent tests performed on high quality specimens from the field and on<br />

specimens reconstituted from a slurry and consolidated to stresses equivalent to<br />

those in the field. Although the specimens were consolidated to the same stresses<br />

67

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