united states department of the interior … report 85-518 1 woods ... static triaxial test results...
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UNITED STATES DEPARTMENT OF THE INTERIOR
GEOLOGICAL SURVEY
STATIC AND CYCLIC STRENGTH
PROPERTIES OF MOUNT ST. HELENS
DEBRIS AVALANCHE AND ASH CLOUD MATERIALS
by
William J. Winters 1
and
Robert E. Kayen2
Open-File Report
85-518
1 Woods Hole, Massachusetts 02543
2 Menlo Park, California 94025
August 1985
This report is preliminary and has not been reviewed for conformity with U.S. Geological Survey editorial standards and stratigraphic nomenclature. Any use of trade names is for descriptive purposes only and does not imply endorsement by the USGS.
TABLE OF CONTENTS
Page
Introduction............................................................ 1Sample preparation and testing methodology.............................. 1
Sampling............................................................. 1Laboratory testing methodology....................................... 2
Results................................................................. 3Static triaxial tests................................................ 3Cyclic triaxial tests................................................ 3
Discussion.............................................................. 4Modeling field behavior in the laboratory with small-scale specimens. 4Static triaxial test results......................................... 4Sample preparation................................................... 5Anisotropic field stress state and reconstitution method............. 5Correction factors applied to cyclic triaxial test results........... 6
1. Membrane compliance............................................ 62. Isotropic consolidation........................................ 7
Normalized shear stress curves for use with the simplified method todetermine liquefaction potential.................................. 8
Liquefaction susceptibility assessment.................................. 8Conclusions............................................................. 9Acknowledgements........................................................ 10References.............................................................. 11Nomenclature and symbols ................................................ 14Tables.................................................................. 16Figures................................................................. 22Appendices A. Static triaxial test results............................. 43
B. Cyclic triaxial test results............................. 83
ii
INTRODUCTION:
On May 18, 1980 the northern flank of Mount St. Helens turned into an enormous debris avalanche that traveled up to 23 km in a period of approximately ten minutes and buried an area of about 60 km^ to an average depth of 45 m (Voight and others, 1983). The mass movement dammed a number of streams, created a blockage in front of Spirit Lake, and deposited approximately 0.4 km0 of material into Spirit Lake raising the water level 60 m (Glicken and others, in preparation). New impoundments were formed when natural drainage routes were blocked (Fig. 1). South Fork Castle Creek was dammed by the debris avalanche and formed a lake with a volume ofJ qapproximately 0.02 km0 . That lake level has been presently stabilized by the construction of a spillway. The mass flow consists of poorly sorted mixtures of material ranging from large boulders to clay size with a sand and gravel matrix (Meyer and others, 1985). Layers of volcanic ash cloud deposits are present in many locations, typically near the ground surface.
The physical properties, and static and dynamic strength of material obtained from the Spirit Lake and Castle Creek blockages are presented in this report. Two samples were obtained from each of those blockages (Table 1, Fig. 1). Surface grab samples were seived, reconstituted, and reconsolidated in the laboratory. Also, samples of the ash cloud deposit were obtained near the surface of the Spirit Lake blockage. The samples were subjected to static (in order to assess pre- or post-earthquake stability) and cyclic triaxial tests (to evaluate the effects of cyclic loading on material behavior). Sample consolidation stresses, overconsolidation ratios, dry densities, and grain sizes were varied to determine their effect on sample behavior.
The results of the test program can be used to assess the liquefaction susceptibility of the material. The liquefaction potential can then be determined by comparing the susceptibility of the material to anticipated earthquake loadings at Mount St. Helens.
Liquefaction of a significant amount of the debris flow material could lead to failure or overtopping of the recently formed dams by the impoundments during or immediately after an earthquake. Flooding and mud flows could then threaten both lives and property downstream. Many small and moderate earthquakes have occurred in the Mount St. Helens region both before and after the 1980 eruption (Voight and others, 1983).
SAMPLE PREPARATION AND TESTING METHODOLOGY
Sampling:
In August of 1982 and March of 1983 surface grab samples were collected on the north side of Mount St. Helens at the Spirit Lake (SL) and South Fork Castle Creek (CC) localities (Table 1). The debris flow material was bagged and allowed to dry. Particles greater than 64 mm in diameter were removed from the grab samples. The finer-grained ash cloud deposit (SL1) from Spirit Lake was sampled by vertically pushing a 48 mm inside-diameter thin-walled tube into a horizontal bench cut into the deposit.
Laboratory testing methodology:
Two subsamples were taken from each of the Spirit Lake and South Fork Castle Creek grab samples. The first subsample contained only particles finer than 5.6 mm in diameter, while the second contained particles finer than 3.3 mm in diameter. These grain sizes represent one-sixth and one-tenth of the reconstituted triaxial specimen diameter (36 mm) respectively. The grain size distributions from the grab sample and subsample with particles less than 5.6 mm in diameter were obtained by dry sieving in. a mechanical sieve shaker in accordance with the American Society for Testing and Materials (ASTM), Test for Particle-Size Analysis of Soils (D 422) (Fig. 2). Ash cloud material (SL1) was tested intact, without remolding or seiving. Intact samples were trimmed on a standard soil lathe to the appropriate dimensions.
Triaxial samples were prepared within a 0.3 mm thick commercial geotechnical membrane stretched inside a hollow cylindrical mold. Two procedures were employed to reconstitute the material within the confines of the membrane:
1) Material was pluviated through deaired water (i.e., the particles were allowed to fall through approximately 20 mm of standing water) until a 90 mm tall cylindrical sample was formed. The top soil was removed until a 70 mm high specimen remained.
2) Material was pluviated in 10 mm high layers through deaired water and tamped up to 25 times per layer with a 9 mm diameter rod. The initial 90 mm high sample was trimmed to a height of 70 mm.
Tamping was used to densify the material and to remove entrapped air bubbles. Once the sample was prepared, it was placed in a triaxial cell with deaired water as a confining fluid. Water was slowly flushed through the sample to expel interstitial air, until the sample was nearly saturated. The cell and sample water pressure were then raised similtaneously to 345 kPa in order to dissolve any remaining gas bubbles and fully saturate the sample. Skempton's B-coefficient values typically were greater than 0.95, indicating a nearly saturated condition existed (Skempton, 1954).
Upon completion of saturation (typically overnight), the material was consolidated by increasing the cell pressure and allowing pore water to drain. After consolidation was complete, the drainage valve was closed and the sample was tested by increasing the axial load on the cylindrical sample. Static triaxial shear tests were performed on 38 reconstituted samples. The water content and dry density of the sample were determined after each test was finished. Material from sample SL4 had the highest water content and lowest dry densities, followed by material from CC1 and CC2 (Fig. 3).
Fifty cyclic triaxial tests were performed using an electropneumatic cyclic loading system similar to the equipment discussed by Chan (1981). Uniform sinusoidal cyclic deviator stresses with almost full stress reversals were applied at a rate of 0.1 Hz. Pore water pressure, axial deformation and axial load were continually monitored and automatically recorded during the static and cyclic triaxial tests.
RESULTS:
Static triaxial tests:
Samples were isotropically and anisotropically consolidated to either 100 or 300 kPa (representative of field overburden stresses) and subsequently were sheared undrained with pore pressure measurements until 20 percent axial strain was reached. A few specimens were rebounded to a lower consolidation stress prior to shear in order to produce an overconsolidated sample. Failure occurred at the point of maximum shear stress, q, (Table 2).
Peak friction angles, <j> f , were determined at points of maximum obliquity, a'-j_/a ! 3> assuming no cohesion intercept. The peak friction angles ranged from 35.4 to 51.1 degrees for the reconstituted material (Table 2, Figs. 4-6). The intact (non-reconstituted) ash deposit from Spirit Lake (SL1) had the lowest peak friction angle, 34.1 degrees.
A quasi-residual friction angle, <j>' r> was determined from each test at the point of lowest obliquity after peak deviator stress was reached. The residual strength of material is typically determined from direct shear tests (Lambe and Whitman, 1969, p. 302; Huang, 1983, p. 31). In addition, residual strength can also be determined from consolidated-undrained triaxial tests (Bowles, 1979, p. 368). However, when the triaxial test is performed to high strain levels, in the order of 20 percent, the sample looses its right circular cylindrical shape, producing a variable cross-sectional area. Therefore, the validity of calculated stresses is lowered. Although many triaxial test stress paths have an approximate straight-line failure envelope, most of the Mt. St. Helens tests produced a backward flip at higher stains (Appendix A) and in this region the residual friction angle was often determined. The validity of comparing the calculated quasi-residual friction angles to residual friction angles determined from direct shear tests or consolidated-drained triaxial tests is questionable.
Results from four static triaxial tests are plotted on Figs. 7-9 showing the effect of dry density on the stress path, stress-strain, and pore-water pressure-strain response of the samples. Individual test results, including stress paths, shear stress versus strain, and pore-water pressure response versus strain, are plotted in Appendix A.
Cyclic triaxial tests:
Isotropically consolidated undrained cyclic triaxial tests were performed on reconstituted material from samples CC1, CC2, and SL4 (Table 3). The ash cloud deposit from sample SL1 was trimmed intact from material extruded from the sampling tube.
The cyclic stress ratio, T/a' c , where T is the maximum average peak cyclic shear stress and a' c is the consolidation stress, is plotted versus the number of cycles to reach two percent single-amplitude strain or 80 percent pore pressure equalization (values after which necking of the sample in tension became more common) for various dry densities (determined at the end of the tests) (Figs 10-17). Lines of approximately equal densities have been drawn on the figures. The maximum, minimum, and mid-point stress ratios at
ten loading cycles (approximately equal to a magnitude 6.75 earthquake, Seed and others, 1983) is shown in each figure and in Table 4. A stress ratio for SL1 material was not determined because of a lack of data. Minimum stress ratios are approximately equal for the material from CC1, CC2, and SL4.
Wide scatter exists in the data with respect to dry densities and effect of grain size and consolidation stress. The larger grain size material from CC1 and CC2 appears to be more susceptible to cyclic loading (Figs. 10 and 11), possibly because a looser structure (lower dry density) was formed during reconstitution. Individual test results are shown in Appendix B.
DISCUSSION:
Modeling field behavior in the laboratory with small-scale specimens:
Inherently, problems exist when trying to model the in-situ behavior of extremely coarse-grained material containing gravel and boulders by small- scale laboratory tests. A case can be made that the large-grained material exists within a matrix of finer-grained material and that it is the finer material that determines the overall behavior of the material; the boulders just "float" in the matrix.
The largest grain size tested from Mount St. Helens was 5.6 mm in diameter. That is one-sixth of the triaxial specimen diameter. According to the ASTM Test for Unconsolidated Undrained Compressive Strength of Cohesive Soils in Triaxial Compression (D2850-82), only particles one-tenth of the sample diameter, for specimens less than 71 mm, should be present. However, the larger grain sizes probably do not invalidate the test results; additionally, the larger particles indicate the trend of results as grain sizes increase. That may allow extrapolation of laboratory based results to field conditions.
The use of a maximum cut-off sieve size creates another problem when testing small samples. The gradation of the sample material differs from the parent material (Fig. 2). Alternatively, parallel grading, i.e., selectively removing certain grain sizes from the sieved sample to achieve a sieved grain- size curve that is parallel to the field curve, has been used by Banerjee and others (1979) to model cyclic behavior of coarse-grained material in the laboratory. However, that technique markedly changes the median grain size, D5Q, of the tested material. Townsend (1978) showed that the technique was not valid for cyclic testing. Also, parallel grading may not be applicable if a large difference exists between field and laboratory grain sizes.
The debris blockages consist of heterogeneous materials. Samples from the surface of the dams may not adequately represent the material at depth.
Static triaxial test results:
Peak friction angles, <f>', typically increased as the dry density of the tested material increased (Figs. 4-6). The quasi-residual frictionangles, <f>' r , exhibiting a more random distribution, were affected to a lesser degree by the dry density (Figs. 4-6).
At a dry density of 1.82 g/cm-% the debris avalanche material (for all test types) from sample CC1 had peak and quasi-residual friction angles of about 43 and 36 degrees, respectively. This is in very close agreement with peak and residual friction angles of 42.5 and 36.5 degrees, respectively, determined from direct shear tests performed on debris avalanche material finer than 2 mm in diameter reported by Youd and others (1981). Voight and others (1983) reported obtaining friction angles from 40 to 44 degrees from direct shear tests performed on material smaller than 4.75 mm. Youd and others (1981) determined a range of dry densities from 1.71 to 1.94 g/cm-* at eleven locations on the debris avalanche. Peak friction angles were within the typical range of coarse sand to fine gravel (Lambe and Whitman, 1969, p. 149; Bowles, 1979, p. 382). Quasi-residual friction angles were typically within, or somewhat higher than, the range reported for coarse sand to fine gravel reported by Lambe and Whitman (1969, p.149).
The results plotted in Figs. 7-9 show the effect of density on the static behavior of material from sample CC1. At the lowest density the material exhibited, upon shear, a contractive behavior (Fig. 7), low strength (Fig. 8), and positive pore pressure response. As the dry density increased, the material progressively increased in dilative behavior, possessed higher strength, and generated greater negative pore pressure response.
Sample preparation:
The method used to reconstitute the laboratory sample has an important effect on the cyclic behavior of material. Mulilis and others (1977) found that pluviating Monterey No. 0 sand through a water-filled mold and then vibrating the sample to the required density produced the second greatest liquefaction susceptibility out of 11 different compaction procedures. That method is similar to the techniques used in this study, except that rodding of the Mount St. Helens material was performed instead of vibrating the sample. This indicates that the results of this study imply a greater susceptibility to liquefaction than would have been obtained had another preparation method been used.
Anisotropic field stress state and reconstitution method;
Most parts of the Mt. St. Helens debris blockages probably exist with an anisotropic state of stress. Therefore, initial shear stresses are present on horizontal surfaces in the dams. Seed (1979) stated that the presence of initial shear stresses typically reduces the rate of pore pressure generation and that a critical condition exists when no initial shear stresses are present, i.e., under level ground. We have assumed that intial shear stresses on horizontal surfaces were negligible because of the isotropic consolidation condition of the triaxial samples. Therefore, the test results present conservative estimates of shear stress ratios, t/a ! t that would induce liquefaction.
Correction factors applied to cyclic triaxial test results:
1. Membrane compliance;
Ideally, cyclic triaxial tests are performed undrained with constant specimen volume. However, even with all drainage lines closed, a small amount of drainage occurs around the periphery of the sample because penetration of the rubber membrane into the voids between coarse particles decreases with a reduction in the effective confining stress (Raju and Sadasivan, 1974). In contractive soil, as pore pressure increases, the membrane flexes outward, away from the sample, (accompanied by a volume loss within the grain structure) thereby relieving some of the excess pore water pressure (Kiekbusch and Schuppener, 1977). Therefore, pore pressure builds to a lower level than it would in a truly undrained test. Because of the reduction in pressure response, test results are unconservative (i.e., without membrane compliance the sample would fail quicker, either from a lower number of loading cycles or from a lower stress ratio) .
Membrane compliance effects are a function of mean particle diameter, void ratio, effective confining stress, the change in pore pressure during shear, and the amount of surface area of the sample (Lade and Hernandez, 1977). As the grain size increases, more initial penetration of the membrane into the voids between grains occurs, thereby causing subsequent compliance errors to increase. A well graded (poorly sorted) soil, like the Mt St. Helens debris avalanche material, is affected less than a poorly graded soil because the void space between surface grains is reduced.
Soils with a mean particle diameter, D5Q} ies s than 0.1 mm generate negligible membrane compliance errors (Lade and Hernandez, 1977; Martin and others, 1978). However, because the material tested from Mt. St. Helens possessed 050 values larger than 0.1 mm corrections were applied to account for membrane compliance.
Most of the static triaxial tests generated negative pore pressures during shear. Those tests, therefore, were conservative with respect to membrane penetration. That is, the negative pore pressures would have become even more negative without membrane penetration. Cyclic tests, however, generate positive pore pressures and would, if not corrected for membrane compliance, lead to unconservative results. Ramana and Raju (1981) found little change in <f> f determined from static triaxial tests even with significant changes in pore pressure response. Therefore, we are correcting cyclic tests for membrane compliance but not static tests.
The profession is not consistent on how to correct tests for membrane penetration. Raju and Sadasivan (1974) improved a technique, first suggested by Roscoe and others (1963), of using brass rods surrounded by sample material to determine effects of membrane compliance. However, Vaid and Negussey (1984) indicated that those techniques were incorrect and proposed alternate methods. Kiekbusch and Schuppener (1977) indicated that undrained tests could not be simply corrected for membrane compliance, the way that drained tests could be. Instead, they suggested using liquid rubber that would harden around the periphery of the sample thereby reducing the amount of change in the membrane penetration as the test progressed.
Seed (1979) determined that a correction factor to the stress ratio of about 25 percent was required to account for membrane compliance of Monterey No. 0 uniform medium sand (D5Q equals 0.4 mm) (Mulilis and others, 1977) used in simple shear tests. However, Seed (1979) also stated that the need for such correction factors has not been widely recognized.
The Mount St. Helens samples were corrected for membrane compliance using the data of Martin and others (1978). The errors (defined as the percentage of the corrected stress ratio) in the cyclic stress ratios varied with the mean grain size, DCQ. The mean particle size of material from CC1 passing the 5.6 mm sieve is 0.8 mm, CC2 is 0.4 mm, and SL4 is about 1.0 mm (Fig. 2). According to Martin and others (1978) the error in cyclic stress ratios for 36 mm diameter samples of uniform grading with the mean grain sizes of the Mt. St. Helens samples are approximately 75 percent, 55 percent, and 80 percent respectively. Those values are inexact, however, and in-depth studies on actual Mt. St. Helens samples would be needed to better quantify the effect of system compliance.
The compliance correction values reported by Martin and others (1978) were arbitrarily reduced by 25 percent because the Mount St. Helens samples are well graded. Therefore, the error in stress ratios for the Mt. St. Helens samples were 0.55, 0.40, and 0.60 for CC1, CC2, and SL4, respectively. The corrected stress ratio equals the stress ratio determined from testing minus the estimated error. The error values reported by Martin and others (1978) of 0.55, 0.40, and 0.60 based on final (corrected) stress ratios correspond to membrane compliance coefficients 0.65, 0.71, and 0.63 based on initial test stress ratios. The initial cyclic stress ratios (Table 4) were multiplied by those coefficiants to account for membrane penetration (Table 5) .
2. Isotropic consolidation;
One of the largest variations between field and laboratory conditionsresults from using a coefficient of earth pressure at rest, Ko » equal to 1.0 in the laboratory (i.e., the horizontal and vertical effective stresses are equal prior to cyclic loading). Field conditions, however, typically have values of KQ iess than 1.0 for normally consolidated material. Seed (1979) suggested a correction factor of 0.57 for a KQ value of about 0.4. Seed's factor, that is applied to the cyclic stress ratio, corrects isotropically consolidated triaxial test results to agree with anisotropic simple shear behavior that is more representative of field conditions. The factor also accounts for multidirectional earthquake shaking in the field. A factor of about 0.6 was used with coarser-grained material by Banerjee and others (1979). Therefore, the cyclic stress ratios presented in Table 5 were multiplied by 0.57 to correct for field conditions (Table 6).
Test results (Tables 4-6, Figs. 10-17) show that similar results are derived from both failure criteria (2 percent strain or 80 percent pore pressure equalization). Additionally, the minimum stress ratios required to cause failure are very similar between CC1, CC2, and SL4. A greater difference between stress ratios is present for denser states.
Normalized shear stress curves for use with the simplified method to determine liquefaction potential:
The simplified method to determine liquefaction potential (Seed and Idriss, 1971; Seed, 1979; Seed and others, 1983) enables irregular field earthquake loadings to be modeled in the laboratory by uniform sinusoidally loaded cyclic triaxial tests. That method requires the use of a normalized shear stress versus number of cycles to reach failure plot (Fig. 18) in order to determine the cyclic stress ratio necessary to induce liquefaction in the field for different magnitude earthquakes.
The plot used by Seed and others (1983) (Fig. 19) is for sands and is not directly applicable to the Mt. St. Helens area. Therefore, using results from the cyclic triaxial tests, normalized curves were plotted for differentmaterials (Fig. 18). The normalized factor T/TJ_, where -q is tne estimated shear stress required to cause failure (two percent strain) in one cycle, is a representation of the slope of the stress ratio-cycle to failure plots (Figs. 10-13). Because of the lack of data in some areas the extrapolated value of T]_ is inexact. The family of curves (with the exception of the ash cloud deposit, SL1) shows a tight grouping up to 10 cycles. After 10 cycles, more divergence is apparent.
An average curve for the Mt. St. Helens material is shown in Fig. 19, weighted towards the tests from CC2 and SL4 because more data exists for those locations. The curves were also corrected for membrane compliance and isotropic consolidation as previously discussed, however those corrections were typically normalized out of the plot and had little effect on the curves. Results for the ash cloud deposit, SLl, are located well below the other materials and are more consistent with the data of Seed and others (1983) for sands. However, limited data were used to determine the curve for SLl, and the failure criterion used by Seed and others (1983) (pore water pressure equalization and ±5 percent strain) was different than the criterion used in this report.
The simplified method to determine liquefaction potential for the Mount St. Helens blockages, using the normalized shear stress curve (Fig. 19), is explained in more detail in a different publication (Chen and others, in press).
LIQUEFACTION SUSCEPTIBILITY ASSESSMENT:
The uncorrected midpoint cyclic stress ratios required to cause failure at 10 loading cycles for the Mt. St. Helens samples (Table 4) are approximately equal to or greater than the stress ratios (approximately 0.35) determined for Monterey sands No. 0 and No. 1 at a relative density of 60 percent (prepared by the wet tamping procedure) (Silver and others, 1976). The uncorrected minimum stress ratios (Table 4) for the Mt. St. Helens samples are somewhat lower than for the Monterey sand and the corrected minimum stress ratios (approximately 0.1) are substantially lower (Table 6). The corrected Mt. St. Helens stress ratios are also substantially lower than the stress ratios required to fail northern Bering Sea sediment in 10 loading cycles (Hampton and Winters, 1983).
Qualitatively, the loosest reconstituted Mt. St. Helens samples are defininely susceptible to liquefaction from moderately sized earthquakes. However, field conditions differ markedly from the laboratory setting. The Mt. St. Helens material grain sizes (Fig. 2) are substantially coarser than those reported to be the most easily liquefied (Finn, 1972) (Fig. 20). Townsend (1978) reported that the most liquefaction prone samples possessed aD^Q of approximately 0.1 mm with susceptibility decreasing as the mean grain size increased or decreased from that value.
With few exceptions, most of the static triaxial tests from CC1 and CC2 produced negative pore pressures upon substantial strain (Appendix A). Therfore, even if movement started to occur due to earthquake induced shaking, the material at those locations in all but the loosest condition would dilate after strain, reduce the excess positive pore pressures, and thereby stabilize itself. Tests performed on SL4 samples showed a greater tendency to produce positive pore pressures.
Drainage of pore water and subsequent reduction of excess pore pressures was not considered in this study. Due to the large grain sizes of the field material, some drainage may occur, thereby reducing the liquefaction potential.
Erosion at some locations will produce an overconsolidated stress history (thereby reducing the liquefaction susceptibility) in the remaining material, however that may be offset by the increased potential for creating an unstable geometry in the blockages. As time passes, the material's strength will probably increase due to aging effects (Mitchell and Solymar, 1984).
CONCLUSIONS:
Corrected results of cyclic triaxial tests performed on loose reconstituted, seived Mt. St. Helens debris avalanche material and on an intact ash cloud deposit indicate that low resistance to cyclic loading is present. However, major reductions in the cyclic strength were due to inexact membrane compliance correction factors that were used from another study. Membrane compliance correction factors for the actual Mt. St. Helens samples may not be as severe.
The laboratory samples possessed grain size distributions significantly different from those of the field material. Increased coarseness of field material will probably reduce the liquefaction susceptibility.
If failure does occur in any of the blockages, dilation of dense material will tend to stabilize the movement. Dilation will not occur in debris material present in a loose condition.
As time passes after the formation of the debris avalanche in 1980, the stability of the blockages will increase due to aging effects. However, that may be locally offset by the undercutting of individual slopes by erosion.
Future laboratory studies should utilize larger sample dimensions in order to better represent field conditions. Larger specimen sizes will also
reduce the effects of membrane penetration. Liquid rubber applied to the test membrane may be used to reduce the effect of membrane compliance.
In-situ density measurements, borings, seismic exploration, standard penetration tests, and cone penetration tests (if possible) would enable additional liquefaction susceptibility analyses to be made.
ACKNOWLEDGEMENTS:
The authors wish to thank the reviewer of this report, H. J. Lee, for his helpful comments. T. L. Youd, A. T. F. Chen, and R. L. Schuster provided suggestions and assistance. D. J. Bright performed much of the laboratory testing.
The cover photograph of Mount St. Helens was taken in April 1981 looking south across Spirit Lake. Lyn Topinka is thanked for giving permission to use the photograph.
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REFERENCES
Banerjee, N.G., Seed, H.B., and Chan, C.K., 1979, Cyclic behavior of dense coarse-grained materials in relation to the seismic stability of dams. Earthquake Engineering Research Center Report 79/13, University of California, Berkeley, 252 p.
Bowles, J.E., 1979, Physical and Geotechnical Properties of Soils. New York, McGraw-Hill Book Company, 478 p.
Chan, C.K., 1981, An electropneumatic cyclic loading system. Geotechnical Testing Journal, ASTM, Vol. 4, No. 4, December, p. 183-187.
Chen, A. T. F., Youd, T. L. , Winters, W. J. , and Bennett, M. J., in preparation, Liquefaction resistance of debris dams. In: Schuster, R. L. and Meyers, W. (eds.), U.S. Geological Survey Professional Paper.
Finn, W.D., 1972, Soil dynamics liquefaction of sands. Proceedings International Conference on Microzonation for Safer Construction Research and Application, Vol. 1, Seattle, p. 87-111.
Glicken, H., Meyer, W., and Sabol, M., in preparation, Geohydrology of Spirit Lake blockage with reference to lake impoundment. U.S. Geological Survey Open-File Report.
Hampton, M.A. and Winters, W.J., 1983, Geotechnical framework study of the northern Bering Sea, Alaska. U.S. Geological Survey Open-File Report 83-404, 382 p.
Huang, Y.H., 1983, Stability Analysis of Earth Slopes. New York, Van Nostrand Reinhold Company, 305 p.
Kishida, H., 1969, A note on the liquefaction of hydraulic fill during theTokachi-Oki earthquake. Second Seminar on Soil Behavior and GroundResponse During Earthquakes, University of California, Berkeley, Aug.
Kiekbusch, Manfred and Schuppener, Bernd, 1977, Membrane penetration and itseffect on pore pressures. Journal of the Geotechnical EngineeringDivision, Vol. 103, No. GT11, Nov., p. 1267-1279.
Lambe, T.W. and Whitman, R.V., 1969, Soil Mechanics. New York, John Wiley & Sons, 553 p.
Lade, P.V. and Hernandez, S.B., 1977, Membrane penetration effects in undrained tests. Journal of the geotechnical Engineering Division, ASCE, Vol.103, No. GT 2, Feb., p. 109-125.
Lee, K.L. and Fitton, J.A., 1969, Factors affecting the cyclic loading strength of soil. In: Vibration Effects of Earthquakes on Soils and Foundations, ASTM Special Technical Publication 450, p. 71-95.
Martin, G.R., Finn, W.D.L., and Seed, H.B., 1978, Effects of system compliance on liquefaction tests. Journal of the Geotechnical Engineering Division, ASCE, Vol. 104, No. GT 4, April, p. 463-479.
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Meyer, W., Sabol, M.A., Glicken, H.X., and Voight, B., 1985, The effects of ground water, slope stability and seismic hazard on the stability of the South Fork Castle Creek blockage in the Mount St. Helens area, Washington. U.S. Geological Survey Professional Paper 1345.
Mitchell, J.K. and Solymar, Z.V., 1984, Time-dependent strength gain infreshly deposited or densified sand. Journal of GeotechnicalEngineering, ASCE, Vol. 110, No. 11, November, p. 1559-1576.
Mulilis, J.P., Seed, H.B., Chan, C.K., Mitchell, J.K., and Arulanandan, K. , 1977, Effects of sample preparation on sand liquefaction. Journal of the Geotechnical Engineering Division, ASCE, Vol. 103, No. GT2, Feb., p. 91-108.
Ramana, K.V. and Raju, V.S., 1981, Constant-volume triaxial tests to study the effects of membrane penetration. Geotechnical Testing Journal, ASTM, Vol. 4, No. 3, Sept., p. 117-122.
Raju, V.S. and Sadasivan, S.K., 1974, Membrane penetration in triaxial tests on sands. Journal of the Geotechnical Engineering Division, ASCE, Vol. 100, No. GT4, April, p. 482-489.
Roscoe, K.H., Schofield, A.M., and Thurairajah, A., 1963, An evaluation of test data for selecting a yield criterion for soils. Laboratory Shear Testing of Soils, ASTM, Special Technical Publication 361, p. 111-128.
Seed, H.B., 1979, Soil liquefaction and cyclic mobility evaluation for level ground during earthquakes. Journal of the Geotechnical Engineering Division, ASCE, Vol. 105, No. GT 2, Feb., p. 201-255.
Seed, H.B. and Idriss, I.M., 1971, Simplified procedure for evaluating soil liquefaction potential. Journal of the Soil Mechanics and Foundations Division, Vol. 97, No. SM9, Sept., p. 1249-1273.
Seed, H.B., Idriss, I.M., and Arango, I., 1983, Evaluation of liquefaction potential using field performance data. Journal of Geotechnical Engineering, ASCE, Vol. 109, No. 3, March, p. 458-482.
Silver, M.L., Chan, C.K., Ladd, R.S., Lee, K.L., Tiedemann, D.A., Townsend, F.C., Valera, J.E., and Wilson, J.H., 1976, Cyclic triaxial strength of standard test sand. Journal of the Geotechnical Engineering Division, ASCE, Vol. 102, No. GT5, May, p. 511-523.
Skempton, A. W. , 1954, The pore-pressure coefficient A and B. Geotechnique, Vol. 4, p. 143-147.
Townsend, F.C., 1978, A review of factors affecting cyclic triaxial tests. In: Dynamic Geotechnical Testing, ASTM, Special Technical Publication 654, p. 356-383.
Vaid, Y.P. and Negussey, Dawit, 1984, A critical assessment of membrane penetration in the triaxial test. Geotechnical Testing Journal, ASTM, Vol. 7, No. 2, p. 70-76.
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Voight, B., Janda, R.J., Glicken, H. and Douglass, P.M., 1983, Nature andmechanics of the Mount St Helens rockslide-avalanche of 18 May 1980.Geotechnique, Vol. 33, No. 3, Sept., p. 243-273.
Youd, T.L., Wilson, R.C., and Schuster, R.L., 1981, Stability of blockage in North Fork Toutle River. In: Lipman, P.W. and Mullineaux, D.R., (eds.), The 1980 Eruptions of Mount St. Helens, Washington, U.S. Geological Survey Professional Paper 1250, p. 821-828.
13
NOMENCLATURE AND SYMBOLS:
A Coeff. - Pore pressure parameter at failure (maximum q), equal to the change in pore pressure divided by the deviator stress.
ASTM - American Society for Testing and Materials.
DCJQ - Mean grain size.
DELTA u - The change in excess pore water pressure from the beginning of a shear test.
Dev Stress - The deviator stress or difference between the major and minor principal effective stresses, (0'^ - 0*3)
KQ - Coefficient of earth pressure at rest, (a'^/a^)
OCR - Overconsolidation ratio, (c^'vm^'vo^ *
p' - The normal effective stress acting on a plane inclined at 45 degrees from the horizontal in a triaxial test, (a' + v'
q - The shear stress acting on a plane inclined at 45 degrees from the horizontal in a triaxial test, (0' - a'
qmax - Maximum value of q reached during a static triaxial test, equal to Su .
SIG l c ' - The major (or vertical) principal stress applied to a triaxial test sample prior to shear.
SIG 3C T - The minor (or horizontal) principal stress applied to a triaxial test sample prior to shear.
TE - Prefix for a static triaxial test number.
w - Water content (weight of water/weight of solids).
a 'l - The major principal effective stress applied to a triaxial test sample.
a'^/a'o - obliquity factor; it is a maximum at the point of the largest friction angle during a triaxial test.
a '2 ~ The minor principal effective stress applied to a triaxial test sample.
o' c - The isotropic consolidation stress imposed on a triaxial test sample prior to shear.
= 0 T VO - The in-situ vertical effective stress exerted by the weight of overburden.
T - Shear stress.
14
^ - Estimated shear stress required to cause failure in one cycle during a cyclic triaxial test.
' - The peak friction angle expressed in terms of effective stresses.
' - The quasi-residual friction angle expressed in terms of effective stresses.
15
Table 1.
Sample in
form
atio
n.
Sample
Alternate
Location
Date
Field
Grain
Sample
Material
I.D.
I.D.
Obtained
Density
Specific
Type
Type
(g/c
m3
) Gravity
_____________________________________________________________(g/cm3)_______________
CC1
- S.F. Castle Creek
3-8-
83
- 2.75
Grab
Debris
Avalanche
CC2
JM-82-826-2
S.F.
Castle Creek
8-26-82
1.59
2.
76
Grab
Debris
Avalanche
SL1
- Spirit La
ke
3-8-83
- -
Tube
Ash
Cloud
Deposit
SL4
JM-82-825-7
Spirit Lake
8-25-82
1.79
2.65
Grab
Debris
Avalanche
Tabl
e 2.
Static triaxial teat results
Sa
mp
le
CC
1
CC
2
SL1
SL4
Tte
st
No
.
123
124
127
12
81
30
13
1132
133
13
41
36
125
12
61
35
176
17
8
137
13
81
39
14
01
43
14
41
55
164
147
148
14
9
15
0151
15
2179
18
3
12
9
170
173
175
17
71
84
18
5
Pa
ssin
g
Sie
ve
Siz
e (
mm
)
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
5.6
5.6
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
5.6
5.6 -
3.3
3.3
3.3
3.3
5.6
5.6
Con s
ol.
Str
ess
(kP
a)
101
103
10
0100
99
99
98 98
96
20
4/9
93
00
300
49
87
101 99
100
98
99
100
97
100
97
299
295
29
9
29
62
67
/10
745
97
97
101
97
103
298
29
69
69
9
Wa
ter
Conte
nt
Aft
er
Sh
ea
r
(%)
18.6
17.7
21.8
19
.01
7.0
17.6
18.9
17.9
17.7
18
.61
9.8
?18.1
18
.519.7
15
.0
15.9
15
.014.5
14.2
15
.41
6.6
17.2
16.4
14.0
13
.615.3
15.1
14.9
14.7
15.7
15.9
31.4
24.5
22.2
24.1
23.0
27
.02
0.7
A
Coef f.
-0.0
2-0
.19
0.4
1-0
.16
-0.1
8-0
.15
-0.2
4-0
.19
-0.2
1-0
.19
0.0
1-0
.05
-0.2
3-0
.03
0.1
3
-0.2
6-0
.24
-0.2
0-0
.17
-0.2
0-0
.21
-0.2
0-0
.17
-0.0
9-0
.1 2
-0.1
0
-0.1
1-0
.22
-0.2
5-0
.01
0.1
9
0.0
6
-0.1
2
-0.2
40
.09
0.3
41
.21
0.2
3
Str
ain
at
Failure
(%)
16.3
7.9
19
.61
9.2
7.5
5.7
17
.0
7.0
7.0
9.4
7.7
8.5
9.8
6.0
5.3
11 .
87
.89
.98
.49
.16
.5
8.7
8.3
5.3
7.9
6.2
7.0
6.5
7.2
9.3
7.5
13
.8
14
.51
1.2
12
.08
.011.3
10.2
OC
R
1.0
1.0
1 .0
1 .0
1 .0
1 .0
1.0
1 .0
1.0
1.0
1 .0
1 .0
6.1
1.0
1 .0
1 .0
1 .0
1.0
1 .0
1 .0
1 .0
1 .0
1 .0
1.0
1 .0
1 .0
1.0
1 .0
6.7
1 .0
1 .0
1 .0
1.0
1.0
1 .0
1 .0
1 .0
1 .0
qF
ailure
(k
Pa
)
168
63
96
4266
60
34
97
724
84
46
69
451
46
56
55
500
17
11
07
5
551
66
3909
11
85
927
471
514
30
61
25
01
45
61
26
2745
717
645
146
107
96
20
67
39
378
210
16
3583
P1
Fa
ilu
re
(kP
a)
275
980
110
452
914
74
01168
12
66
10
45
721
75
61
02
4780
26
71
46
0
932
1078
13
72
1697
13
95
761
81
65
06
1762
20
93
18
15
12
10
11
34
99
6244
164
185
35
31201
609
364
281
952
*'
Peak
(deg.)
38
.445.6
35.9
38.1
45
.04
6.2
43
.7
45
.44
3.6
43.9
42.0
42
.74
4.0
40.1
51 .
1
41
.74
2.6
44.6
46
.44
5.5
42.9
42.1
40.5
46.4
45
.345.1
41
.841.9
42
.536.9
41
.7
34
.1
39
.34
3.4
39
.53
5.4
37.3
42.4
*'
Re
s .
(de
g.)
36.6
34
.73
5.2
35.6
37.2
36.7
37.7
35
.3
34
.33
5.7
35.2
34.7
36.3
38.3
38.2
33.8
33
.73
9.0
40.2
36.9
35.2
36.6
34.5
35.5
39
.0
34
.331
.5
36
.33
5.5
34
.338.5
30.2
35
.03
2.2
35.4
29
.73
2.6
30
.9
Dry
D
ensity
(g/c
m3
)
1 .8
21.8
5
1 .7
21
.81
1.8
71
.85
1 .8
21
.84
1.8
5
1 .8
21.7
8?
1 .8
31
.82
1.7
81
.94
1 .9
21
.95
1 .9
7
1 .9
81
.94
1 .8
91
.87
1 .9
01
.99
2.0
11
.94
1 .9
51
.95
1 .9
61
.92
1 .9
2
1.3
4
1 .6
11.6
71
.62
1.6
51.5
41.7
1
Tab
le
3.
Cycl
ic
tnax
ial
test
resu
lts
00
Sample
CC1
CC2
SL1
SL4
Test
No.
130
131
132
133
134
135
136
197
198
137
138
139
140
141
142
143
144
145
161
162
146
147
148
149
179
180
181
182
183
184
195
185
186
187
188
155
156
163
164
165
166
169
170
189
190
191
192
196
193
194
Passing
Siev
e Size (mm)
3.3
3.3
3.3
3.3
3.3
3.3
3.3
5.6
5.6
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
3.3
5.6
5.6
5.6
5.6
5.6
5.6
5.6
5.6
5.6
5.6
5.6 - - 3.3
3.3
3.3
3.3
3.3
3.3
5.6
5.6
5.6
5.6
5.6
5.6
5.6
Consolidation
Stress
(kPa
)
100 97 98 100
98 100
98 95 96 100 98 99 98 99 98 99 98 98 94 72
299
297
297
297 96 101
109 94 98 100 96
295
297
293
297 99 98 93 96 88 87 100 97 97 98 97 99 97
275
275
. .
Water Content
After Shear
_____ U) _____
17.2
20.8
19.0
16.6
16.5
18.9
18.0
19.8
18.1
17.0
14.8
14.7
14.8
13.4
13.8
13.9
14.2
14.4
15.9
17.6
13.9
13.0
13.6
14.5
18.8
16.2
22.4
16.7
17.0
17. J
16.3
16.3
15.8
15.7
14.2
30.8
28.0
25.8
26.3
23.8
22.4
24.7
17.3
21 .8
20.3
26.4
25.6
14.6
20.1
25.0
OCR
1.0
1 .0
1.0
1 .0
1.0
1 .0
1 .0
1.0
1 .0
1.0
1.0
1.0
1.0
1.0
1 .0
1.0
1.0
1.0
1 .0
1.0
1 .0
1.0
1 .0
1 .0
1 .0
1.0
1.0
1.0
1.0
1 .0
1 .0
1 .0
1 .0
1.0
1.0
1 .0
1.0
1.0
1.0
1.0
1 .0
1 .0
1 .0
1.0
1.0
1.0
1.0
1 .0
1 .0
1 .0
T°'c
(%) 97 57 33 24 50 48 60 40 27 33 41 31 48 29 48 23 35 51 37 55 33 40 35 45 53 27 36 46 43 22 44 39 31 34 27 80 48 41 22 29 28 38 50 29 42 32 40 34 48 32
Cycles to
2% Strain
-
7 - 1212
1 257 2 1
19 18 22 19 6 55 4344 237 141
13 8 222 1
34 3 2 4 33 3 3 6 550
1 3 713
1 16103 _
14 49 19 14 9 9 5 6
Cycles
70% 3 2 6 78 6 5 2 2 17 14 15 11 3403
309 124 7 - 9 4 12 _ _ 31 _ 2 3 28 2 4 5 3
38
2 3 51 14 11 958 7 42 14 14 9 6 5 6
" - - -
to Pore Pressure
80%
-
5 2 8 87 8 6 - _ 18 16 18 12 4 433
319 13 5 8 - 11 5 15 _ - 32 _ 3 4 30 3 5 6 4
42
2 3 7121 14 99 11 9 46 16 17 12 7 _ 7
Equalization
90%
.
- 10 95 11 - - _ 20 18 23 14 546 4
327 15 6 11 - - 7
22- - 34 _ 4 6 31 - _ 7 5
47
2 4 812
7 16102 18 _50 _ 20 - 9 _ -
Dry
Density
(g/cm3
)
1 .8
71.
751 .80
1 .89
1 .89
1.81
1.84
1.79
1.84
1.88
1 .9
61.
961 .9
62.
022.00
1 .9
91 .98
1 .97
1 .9
21 .8
61 .9
92.
032.01
1 .9
71.
821.
911.71
1 .89
1 .90
1.89
1 .90
1 .9
21 .9
21.
931 .9
8
.42
.56
.57
.59
.62
.66
.60
.82
.68
.72
.56
.58
.91
.75
.61
Tabl
e 4.
Cycl
ic stress ra
tios
, T/a
1 ,
at 10 lo
adin
g cycles de
term
ined
from Fi
gs.
10-1
7.
Samp
le
T/a
'c at
2
% strain
T/a'c
at ®®
^° Po
re pr
essu
re equalization
max.
midp
oint
rain.
max.
midp
oint
min.
CC1
0.76
0.50
0.24
0.
82
0.55
0.28
CC2
0.48
0.
37
0.26
0.46
0.36
0.26
SL1
0.3
- 0.
2 (?
) 0.3
- 0.
1 (?
)
SL4
0.54
0.
41
0.28
0.
48
0.38
0.28
Table
5.
Cycl
ic stre
ss ra
tios
, T/a
1 , at
10
loading
cycl
es determined from Fi
gs.
10-1
7 co
rrec
ted
for
membrane co
mpli
ance
.
Samp
le
T/a
'c at 2
% strain
T/a
'c at
**
0 %
pore pressure eq
uali
zati
on
__________max._________midpoint______mi n._________max.
midp
oint
min.
CC1
0.49
0.
33
0.16
0.
53
0.36
0.
18
CC2
0.34
0.
26
0.19
0.33
0.26
0.19
SL1
0.3
- 0.
2 (?)
0.3
- 0.1
(?)
SL4
0.34
0.
26
0.18
0.30
0.24
0.18
Tabl
e 6.
Cyclic stress ratios,
T/O'
C> at 10 lo
adin
g cy
cles
determined from Fi
gs.
10-1
7 co
rrec
ted
for
memb
rane
compliance an
d multiplied by 0.57 to si
mula
te fi
eld
conditions.
Samp
le
T/a'c
at 2
% st
rain
T/°'
c at
^
pore pr
essu
re equalization
max.
midpoint
rain.
max.
mi
dpoi
nt
rain.
CC1
0.28
0.
19
0.09
0.30
0.21
0.10
CC2
0.19
0.15
0.11
0.19
0.15
0.11
SL1
0.2
- 0.1
(?)
0.2
- 0.05 (?)
SL4
0.19
0.15
0.10
0.17
0.14
0.10
LIST OF FIGURES
Fig. 1. Sample location map.
Fig. 2. Grain size distribution curves.
Fig. 3. Water content versus dry density for seived triaxial samples after testing.
Fig. 4. Static triaxial test results for site CC1.
Fig. 5. Static triaxial test results for site CC2.
Fig. 6. Static triaxial test results for site SL4 .
Fig. 7. Stress paths for CC1 material (<3.3 mm) showing effect of dry density on static triaxial test behavior.
Fig. 8. Deviator stress versus strain for CC1 material (<3.3 mm) showing effect of dry density on static triaxial test behavior.
Fig. 9. Change in pore water pressure versus strain for CC1 material (<3.3 mm) showing effect of dry density on static triaxial test behavior.
Fig. 10. Cyclic stress ratio, T/a' c , versus cycles to 2 percent single-amplitude strain for site CC1.
Fig. 11. Cyclic stress ratio, T/a' c , versus cycles to 2 percent single-amplitude strain for site CC2.
Fig. 12. Cyclic stress ratio, t/a' c , versus cycles to 2 percent single- amplitude strain for site SL1 .
Fig. 13. Cyclic stress ratio, T/a' c , versus cycles to 2 percent single- amplitude strain for site SL4 .
Fig. 14. Cyclic stress ratio, T/a' c , versus cycles to 80 percent pore pressure equalization for site CC1 .
Fig. 15. Cyclic stress ratio, T /a ' c , versus cycles to 80 percent pore pressure equalization for site CC2.
Fig. 16. Cyclic stress ratio, T /^' c , versus cycles to 80 percent pore pressure equalization for site SL1 .
Fig. 17. Cyclic stress ratio, T /^' c , versus cycles to 80 percent pore pressure equalization for site SL4.
Fig. 18. T/T^ versus cycles to 2 percent single amplitude strain for Mt . St. Helens cyclic triaxial test samples.
Fig. 19. Weighted average T/T^ curve for Mt . St. Helens samples; Seed and others (1983) used a failure criterion of 100 percent pore pressure equalization and ±5 percent strain.
Fig. 20. Zones of grain size distrbution curves of liquefaction prone materials .
22
U>
South
C
old
wate
r C
ree
k
La
nd
slid
e-D
eb
ris F
low
S.F
. C
astle C
ree
k
Mt.
St. H
ele
ns
Fig
. 1
. S
ampl
e lo
cati
on
map
I
O10
0
GR
AV
EL
SA
ND
SIL
T
CD OC LU *-
at80
Q LU O
60
H-
CL
<
0. o z I K~ CC
LU
"Z.
40 20
n
cc
100
LU
Q.
10
1
PA
RT
ICLE
D
IAM
ET
ER
, IN
M
ILL
IME
TE
RS
0.1
0.01
Fig. 2.
Grai
n size distribution cu
rves
.
WATER CONTENT, IN PERCENT
09
OJ-
coC 03
CL
CL ft)
l-h rr fD
cc
O)
D 33-<
D mZ r* to -j
l-hO>-!
CO DH-<(D CL
rr»-!
T)m330 -C o>CD
0
Om
mII woo
TOO * no -i,
EFFECTIVE FRICTION ANGLE, IN DEGREES
H-00
-O
CO rr
rt H-O
rt:riaxic
Mrt n>COrtr-t
CO
rtCO
O i-j
COH**rtft
OI-1
ro co co 4* -p*. en o en o en
-vl
O
"^
OmCOH
boZ
O DD
CO-g
m
OC^ _,.0 b
omzH
mHmDO
rob
i i i i
O CO0 > * x o _,
q Q O. c^ ex ^ *"~*o"o"o"o"o IJ^ « » « £ 0
_ O O CD O O 1o o o o 3Dy- ^ ^ ^. ^ ^
"0 "D Q) "0 "D ,_,Q) 0) Q) 0) -^
o 5^^ O , x ° xZ 3 r~00 » __,
- Pi. mCO , .
c; __j0 ^ >. ^ X e *»
A g m x *
? r c - 1* . ' q f- ' £ wCO * *
3 3
_
o -no^D CII >
£3 S^ i
C/5
CT5 ^~
mF
en o
i
-g
m^TI
o-H0
>
CDr~m
LZ
EFFECTIVE FRICTION ANGLE, IN DEGREES
*3 H-
OQ
Ui
COrt03rtH*"o
rti-<LJ. "*
03XL^II "
03M
rt ft03rt
i-jfteocMrt03
i-h0 ^
03H-rt 0>
nnN5
r c
DDD _, < boDmz0>
H-<
Z
ODO>sO) r"
CO TJmDO
0cCD
0
omzH
^ ro^om3D
O CO CO 4^ 4^ O1 Ji O Ol O Ol O
1 1 1 1 1
0 » » X . g "
ro >>q Q Q c^ c^ -^
o o o o o o R « » » » S O
- -i. ro ^ co ^ ' o -J 01 o o ® Ho o ^ o o ^ 33?r ?r T3 ?r ^ °? >T3 T3 Q) T3 T3 ^ r.Q) Q) 0) Q) C" S**
> R ^ > ^ O ^ r-
± 3 '00 «s \O
G) ' m en ' ''
_ C/5o , 0
A Z ^^ co m . .s ? ^^ - O) r^ / 3 ; «,., , ^3 H
w ,CO o ~ CO
3 K t> _
»
«
t
X X
x x
TIO 13 ^D d m0 > >£4 C£ ^
o ' "n Z ^D 33m o -»^ /-^ * ;
CDr~ m
CDr- m
EFFECTIVE FRICTION ANGLE, IN DEGREES
nH-
OQ
<^
C/3 rt to rtP-nrri~1H-to XH-tot >
rrft)cnrr
i-lft)cnC MrrCD
HI O i-S
cnH-rr ft)
C/ir" j>>
ro co co 4*. en o en o
en '
O IDX
DmzCOH __,. -< .- 0
zo3J>^CO-D
m3J
OC ^ CD - lO
OmzH
m-Hm3J
OD
1 I 1
O O
«
X X
- x x
Ofl
-no -n ES S 0 ?^ >-H S2 ^o ' "n z ^ ^
m ^> CO I}
og o r ^ "7>
^ >m r~ > z.
0r~m
-f^ en en o
i i
ODO) H
o x r~ > * 3Q ci C^ ^_, Q
o" o " o ^8 » « '3D_L CO -^ CO 0 0 0 N) > 0 0 0 ^ ><
PT ?r x- ro >-rj -rj -D Cn r-03 Q) W ^j H
-^ m_____ OD
A A 335" P mO) CO OD33 c3 3 -
OD
800
TEST 12? TEST 12&-- -TEST 130 TEST
1 3
rd
Q_
300
200
100
0
SAMPLE CC1
( 3
- D
ry D
ensi
ty.
g/c
m3
C1.8
73
XC1.85)
C1.81)
0100
300
400
500
600
700
800
900
1000
aFi
g. 7.
Stress paths for
CC1
material (<3.3 mm) showing effect of
dry density on static triaxial test
behavior.
TEST 12? TEST 128---TEST 138--TEST 13
+--
U) o
C.
U k
D k
j
22
50
^2
00
0
CL _x:
1?50
1500
00 W
12
50
(D
L_
s 1
00
0i
>
*
^ f
X f V
«/
_j /
cn750
> OJ 500
Q
25
0
0e
__
__
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SA
MP
LE C
C1
t
C )
- D
ry D
ensi
ty,
g/c
m 3
_
I
__
^; E-
/-
-~
.-C
1.8
7)
|
/
^^___
I
/
- .(
1.8
5)
/
.. .--------- C
1.8
1)
- /
...-
----"""""
^ 1 ....
1 ....
1 __
__
__
__
_ I1
"'23
, ,
. ' ' ' I I I I I LI
I I
5 1
0
15
20
2
/o S
tra
inFi
g. 8.
Deviator stress versus strain fo
r CC
1 material (<3.3
mm)
showing
effect of
dr
y density on
static tr
iaxi
al te
st be
havi
or.
101
75
50
25
TE
ST
12Z
..T
ES
T
128-
.TE
ST
130 -
TE
ST
131--
.
rd
Q_ 0 50
-100
rd12
5
Q-1
75
-200
-22
5
-25
0I
i i
0
SA
MP
LE
CC
1C
) -
Dry
Den
sity
, g
/cm
3
(1.7
2)
(1.8
1)
1015
20
t r
a i n
25
Fig
. 9
.Change in
po
re water pressure versus strain fo
r CC1
material (<
3.3
mm)
showing effect of
dry
density on static triaxial test behavior.
u> N3
1.0
o o h- DC CO
CO
LJJ
DC
I
CO g
O
O
0.8
0.6
0.4
0.2
0.0
I.
87
1.8
4
01
.79
CY
CL
IC
TR
IAX
IAL
TE
ST
R
ES
ULT
S
CC
1 tf
'c
»100
kPa
<3.3
mm
o
<TC
«1
00
kP
a
<5.6
mm
Nu
mb
ers
re
pres
ent
dry
de
nsi
ty,
in g/c
m^
RA
NG
E
OF
T/0
'c
AT
10
C
YC
LE
S
0.7
6
- M
AX
IMU
M
0.5
0
- A
VE
RA
GE
0
.24
-
MIN
IMU
M
__
__
__
__
__
__
__
__
I__
__
__
__
__
I.89
These
re
sults
do
not
incl
ude
corr
ect
ions
for
me
mb
ran
e
com
plia
nce
or
iso
tro
pic
conso
lidatio
n.
0.1
1 10
CY
CL
ES
T
O
2 P
ER
CE
NT
S
TR
AIN
100
1000
Fig
.10.
Cycli
c
str
ess ra
tio,
T/a
'c>
vers
us
cycle
s to
2
perc
ent
single
-am
pli
tude str
ain
fo
rsit
e
CC
1
u>
u>
1.0
O0.
8
o i
0-6
CO
CO
UJ
CE
h-
CO g
0.4
O
o
0.2
0.0 0
.1
RA
NG
E
OF
T/<
J'c
AT
10
C
YC
LE
S
0.4
8
- M
AX
IMU
M
0.3
7
- A
VE
RA
GE
0
.26
-
MIN
IMU
M
1.86
,
1.82
*
CY
CLIC
T
RIA
XIA
L
TE
ST
R
ES
ULT
S
CC
2
0"c
»100
kPa
x of
'c «
300
kPa
o cT
c «
10
0
kPa
* O
'c »
300 k
Pa
<3.3
mm
<5.6
mm
Num
bers
re
pres
ent
dry
de
nsi
ty,
in
g/c
m^
97
1.
96
.2.0
2k
1.98
1.9
91.8
9
Th
ese
re
sults
do
no
t in
clu
de
corr
ections fo
r m
em
bra
ne
co
mp
lian
ce or
iso
tro
pic
co
nso
lidatio
n.
10
CY
CL
ES
T
O
2 P
ER
CE
NT
S
TR
AIN
100
1000
Fig.11.
Cyclic stress ra
tio,
T/a'
c, versus cycles to
2
perc
ent
single-amplitude strain fo
r si
te CC2
1.0
o0.8
0.6
o h- DC CO
CO
LJ
J DC
h-
CO g
0.4
_J o
o
0.2
0.0
1.4
2
1
.56
CY
CL
IC
TR
IAX
IAL
TE
ST
R
ES
ULT
S
SL1
(AS
H)
-
0"c
»100
kPa
Num
bers
re
pre
sent
dry
densi
ty,
in
g/c
m^
Th
ese
re
sults
do
no
t in
clu
de
co
rre
ctio
ns fo
r m
em
bra
ne
com
plia
nce
o
r is
otr
opic
co
nso
lida
tion
.
0.1
10
CY
CLE
S
TO
2
PE
RC
EN
T
ST
RA
IN
100
1000
Fig
.12
. C
ycli
c str
ess ra
tio
, T
/a'
vers
us
cy
cle
s to
2
perc
en
t si
ng
le-a
mp
litu
de str
ain
fo
r sit
e
SL
1.
1.0
0.8
0.6
o O h-
<
oc V) (f) LU
QC g
0.4
_j
O
>-
o
0.2 0.0
RA
NG
E
OF
r/C
f'c
AT
10
C
YC
LE
S
0.5
4
- M
AX
IMU
M
0.4
1
- A
VE
RA
GE
0
.28
-
MIN
IMU
M
l.6 l
CY
CL
IC
TR
IAX
IAL
T
ES
T
RE
SU
LT
S
SL
4 0"
c »100
kPa
<
3.3
mm
o
tf'r
»
10
0
kPa
r'c
«300 k
Pa
< 5
.6m
m
Num
bers
re
pre
sent
dry
de
nsi
ty,
in
g/c
m^
O 1
.68
1.6
6
1.5
9
Th
ese
re
sults
do n
ot
incl
ud
e
corr
ections fo
r m
em
bra
ne
com
plia
nce
or
iso
tro
pic
co
nso
lidatio
n.
0.1
10
CY
CLE
S
TO
2
PE
RC
EN
T
ST
RA
IN
100
1000
Fig
.13
. C
ycli
c str
ess ra
tio,
T/O
' ,
vers
us
cycle
s to
2
perc
en
t si
ng
le-a
mp
litu
de str
ain
fo
r sit
e
SL
4.
O O
1.0
-
0.8
0.6
DC CO
CO
LLJ
DC
h-
CO O
0.4
O
O
0.2 0.0
1.8
7
I.
75
RA
NG
E
OF
r/c
r'c
AT
10
C
YC
LE
S
0.8
2
- M
AX
IMU
M
0.5
5
- A
VE
RA
GE
0
.28
-
MIN
IMU
M
CY
CLIC
T
RIA
XIA
L
TE
ST
R
ES
ULT
S
CC
1 tf
'c
»1
00
kP
a
<3
.3m
m
o cT
c «100
kPa
<
5.6
mm
Numbers re
pres
ent dry
density,
in g/cm^ l.8
9
Th
ese
re
sults do
no
t in
clu
de
co
rre
ctio
ns fo
r m
em
bra
ne
com
plia
nce
or
isotr
opic
consolid
ation.
0.1
1 10
100
CY
CLE
S
TO
80
PE
RC
EN
T
PO
RE
P
RE
SS
UR
E
EQ
UA
LIZ
AT
ION
1000
Fig.14.
Cyclic stress ra
tio,
T/a
1 ,
versus cycles to 80 pe
rcen
t pore pressure equalization for
site
CC
1.
1.0
o o
0.8
0.6
DC 00 00 LLJ
DC I-
00 g
0.4
o
o
0.2
0.0
2.0
0
1.8
9°
1.9
0 1.9
31.9
7.
1.9
6
01
.90 X2.0
3
1.92
A
.1-
92
|.98»x 2
.01
1.881.9
6
2.0
0 \
CY
CU
C
TR
IAX
IAL
TE
ST
R
ES
ULT
S
CC
2
tf'c
~
10
0
kPa
x
or'c
»300
kPa
o (T
c «100
kPa
* 0~
'c »
300
kPa
<3.3
mm
< 5.6
mm
Nu
mb
ers
re
pre
sent
dry
de
nsi
ty,
in
RA
NG
E
OF
r/C
f'c
AT
10
C
YC
LE
S
0.4
6
- M
AX
IMU
M
0.3
6
- A
VE
RA
GE
0.2
6
- M
INIM
UM
________________I
__
1.9
9
Th
ese
re
sults
d
o n
ot
incl
ude
corr
ections fo
r m
em
bra
ne
co
mp
lian
ce o
r is
otr
op
ic
conso
lidatio
n.
0.1
1 10
10
0 C
YC
LE
S
TO
80
PE
RC
EN
T
PO
RE
P
RE
SS
UR
E
EQ
UA
LIZ
AT
ION
1000
Fig.15.
Cyclic stress ra
tio,
T/a'
( CC
2.versus cycles to 80 percent po
re pressure equalization fo
r si
te
oo
1.0
o
So0.
8
0.6
QC LLJ
QC
I
CO g 0.4
O
O
0.2
0.0 0.
1
1
.42 1
.56
CY
CLIC
T
RIA
XIA
L
TE
ST
R
ES
ULT
S
SL1
C
AS
H)
rf
'c
»100
kPa
Nu
mb
ers
re
pre
sent
dry
densi
ty,
in
g/c
m3
Th
ese
re
sults
do
no
t in
clu
de
co
rre
ctio
ns fo
r m
em
bra
ne
co
mp
lian
ce
or
isotr
opic
co
nso
lidatio
n.
1 10
10
0
CY
CL
ES
T
O
80
PE
RC
EN
T
PO
RE
P
RE
SS
UR
E
EQ
UA
LIZ
AT
ION
1000
Fig.
16.
Cyclic stress ra
tio,
T/^
'c
, ve
rsus
cycles to
80
percent
pore pressure equalization for
site
SL
1.
1.0
o o H
<
DC (7)
CO
LLJ
DC I
C/D g
_i
o >
o
0.8
0.6
0.4 0.2 0.0
RA
NG
E
OF
r/a
'c
AT
10
C
YC
LE
S
0.4
8
- M
AX
IMU
M
0.3
8
- A
VE
RA
GE
0
.28
-
MIN
IMU
M
CY
CL
IC
TR
IAX
IAL
TE
ST
R
ES
UL
TS
S
L4
0"c
»100
kPa
<
3.3
mm
o
CT'C
«100
kPa
- A
cr'c
»300
kPa
< 5
.6m
m
Nu
mb
ers
re
pre
sent
dry
densi
ty,
in
g/c
m3
o i.6
8.6
6
1.
59
Th
ese
re
sults
do
no
t in
clude
corr
ections fo
r m
em
bra
ne
com
plia
nce
o
r is
otr
op
ic
conso
lidatio
n.
0.1
1 10
100
CY
CLE
S
TO
80
PE
RC
EN
T
PO
RE
P
RE
SS
UR
E
EQ
UA
LIZ
AT
ION
10
00
Fig
.17.
Cycli
c
str
ess
rati
o,
SL
4.vers
us
cy
cle
s to
80
perc
ent
po
re
pre
ssu
re
eq
uali
zati
on
fo
r sit
e
1.0
0.8
-
0.6
-
0.4
-
0.2
-
0.0
SL4 --------
c -
Cor
rect
ed f
or m
embr
ane
com
plia
nce
and
isot
ropi
cco
nsol
idat
ion.
10
100
CYCLES TO 2
PERCENT STR
AIN
1000
Fig.18.
T/TI versus cy
cles
to
2
perc
ent
single amplitude strain fo
r Mt.
St.
Helens cyclic tr
iaxi
al
test samples.
Wei
ghte
d av
erag
e of
C
C1,
CC
2, a
nd S
L4F
or s
and,
fro
m S
eed
and
othe
rs (
1983)
CYCLES TO
CAUSE
100
LIQ
UE
FA
CT
ION
1000
Fig.
19.
Weighted average
T/T-
, cu
rve
for
Mt.
St.
Helens sa
mple
s,
Seed
an
d others (1
983)
failure criterion of 10
0 percent
pore
pressure equalization an
d ±5
pe
rcen
t st
rain
.used a
0
M -
8
CC
-12
LJ
Q.-1
6 40
13
Z M
CL20 10
4
6C
YC
LE *
CRUISE ST HELENS
CORE NO.
SL4
200]
/ % 0 a. * w
13
0
LJ a u 0.
10
0
90
N) a. u1E
+01
IE-0
110 INCREMENT (cm)
TEST NO.
CYCLE #
REMOLDED SURF
D194
SIGlc'(kPa)
275.2
STRTIC qf (kPa)
280.0
SIG3c'CkPa)
275.2
RVG MflX q
(kPa
) 89.2 (31.9^)
INDUCED OCR
1.0
RVG MIN q
(kPa
) -78.1 <27.9*>
Q_
j*
w
20
0
150
100
50
100
20
0p'
(kP
a)
300
400
80
ST
RflIN
(3
O
CR
UIS
E
ST
H
ELE
NS
IN
CR
EM
EN
T
(cm
) C
OR
E
NO
. C
flST
LE
C
RT
ES
T
NO
.R
EM
OLD
ED
-SU
RF
T
E123
SIG
lc'(kP
a)
10
0.8
SIG
3c'(kP
a)
10
0.8
IND
UC
ED
O
CR
1.0
800
600
40
0
200 0
200
400
600
800
p'
(kP
a)
10
0
-200
CL
^-3
00
U
Q
-400
I I I I I I I I I I I k I I 4 I I I
ST
RR
IN
(5O
CRUISE ST HELENS
INCREMENT (c
m)
REMOLDED-SURF
CORE NO.
CflS
TLE CRTEST NO.
TE124
SIGlc'(kPa)
103.
1SIG3c'(kPa)
103.
1INDUCED OCR
1.0
Q.
60 40
50
100
(kP
a)
150
10
15
ST
Rfl
IN20
25
CR
UIS
E
ST
H
ELE
NS
IN
CR
EM
EN
T
(cm
) C
OR
E
NO
. C
flST
LE
C
RT
ES
T
NO
.R
EM
OLD
ED
-SU
RF
T
E127
SIG
lc'C
kP
a)
99
.9S
IG3c'(
kP
a)
99
.9IN
DU
CED
O
CR
1.0
00
400
a 30
0 Q.
200
100 0
100
200
300
400
40
p' (kPa)
20
0
-20
3 jE-«
U
0-60
-80
-
STR
flIN
(J
i
CRUISE ST HELENS
INCREMENT (c
m)
REMOLDED-SURF
CORE NO.
CflS
TLE CRTEST NO.
TE128
SIGlc'(kPa)
99.8
SIG3c'(kPa)
99.8
INDUCED OCR
1.0
800
600
400
200
200
400
p'
600
800
-50
3-1
00
(C gJ-
158
P
-200
10
15
20
ST
RflIN
CRUISE ST HELENS
CORE NO.
CC1
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
TE130
SIGlc'(kPa)
98.6
SIG3c'CkPa)
98.6
INDUCED OCR
1.0
cr
400
300
200
100
200
Ln o
400
600
p'
Ck
Pa)
800
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C1
SIGlc'(kPa)
98.9
SIG3c'(kPa)
98.9
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
TE131
800
800
400
200
500
1000
(k
Pa)
1500
3-2
00
<r
-40
0
ST
RflIN
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C1
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LD
ED
-SU
RF
T
E1
32
SIG
lc'(
kP
a)
98
.1S
IG3
c'C
kP
a)
98
.1IN
DU
CED
O
CR
1
.0
000
800
400
200
500
1000
(k
Pa)
1300
ST
RflIN
(%
CRUISE ST HELENS
CORE NO.
CC1
INCREMENT (cm)
REMOLDED-SURF
TEST NO.
TE133
SIGlc'CkPa)
98.2
SIG3c'(kPa)
98.2
INDUCED OCR
1.0
or
800
600
400
200
Ln
U>
300
10
00
p'
(kP
a)
1500
10
Q.
-20
0
J3-3
00
U a-4
00
ST
RflI
N
CRUISE ST HELENS
CORE NO.
CC1
INCREMENT (c
m)
TEST NO.
SIGlc'CkPa)
96.0
SIG3c'<kPa)
96.0
INDUCED OCR
1.0
REMOLDED-SURF
TE134
Q.
^
w
400
300
200
100
800
400
600
p'
(kP
a)
800
0
-100
[3-1
50
Id a-8
00
2!
ST
Rfl
IN
(JO
CRUISE ST
HELENS
CORE NO
. CC1
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
TE136
SIGlc'CkPa)
204.3
SIG3c'<kPa)
98.9
INDUCED OCR
1.0
40
0
a 3
00
0.
20
0
100
Ln
Ln
200
400
60
0
p'
(kP
a)
800
ST
Rfl
IN
(JO
CRUISE ST HELENS
INCREMENT <cm)
CORE NO.
CflS
TLE CRTEST NO.
REMOLDED-SURF
TE125
SIGlc'(kPa)
299.9
SIG3c
x(kPa)
299.9
INDUCED OCR
1.0
800
a 60
0 0.
40
0
20
0
Ln
50
010
00
p'
CkP
a)
1S00
3 0
£-50
_J U-J00
-150
-200
I I
I I
I I
I
I I
I I
\
10
1520
21
ST
RR
IN
CRUISE ST HELENS
INCREMENT (cm)
CORE NO.
CfiSTLE CRTEST NO.
SIGlc'(kPa)
300.0
SIG3c
x(kPa)
300.0
INDUCED OCR
1.0
REMOLDED-SURF
TE126
80
0
400
300
20
0
40
0
80
0
80
0
p'
(kP
a)
ST
Rfl
IN
CRUISE ST HELENS
CORE NO.
CC1
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
TE13
5
SIGlc'(kPa)
48.9
SIG3c'(kPa)
48.9
INDUCED OCR
6.0
39
0
23
8
200
a-
1913
90
oo
200
300
400
900
p'
Ck
Pa
)60
070
0 8
/ N 0.
0
W-4
3 or-e
ui P-1
2
-16
10
13
20
,___|
ST
RA
IN
C3O
ST HELENS
CORE NO.
CC1 87.0
SIG
3is
'(kP
a)
8?
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IND
UC
ED
O
CR
N
/fl
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
TE
17
&
1601
}
a 12
0i)
0. cr800
400
400
800
1200
1600
p'
(kP
a)
a) a.-1
00
-20
0
(L J
U
-400
CRUISE ST HELENS
CORE NO.
CC1
SIGlc'(kPa)
100.7
SIG3c'(kPa)
100.7
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO
.REMOLDED SURF
TE178
800
* 60
0 Q
.
400
200 0
200
400
600
60
0
px
(kP
a)
0
*
Q.
-20
03
(C U
Q
-40
0
ST
RR
IN
<*)
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C2
SIG
lc'(
kP
a)
98.9
SIG
3c'
Ck
Pa)
98.9
IND
UC
ED
OCR
1.0
INC
RE
ME
NT
(c
m)
RE
MO
LDE
D-S
UR
F
TE
ST
N
O.
TE
137
600
600
400
200
50
01
00
0
(kP
a)15
00
STR
flIN
(J
O
CR
UIS
E
ST
H
EL
EN
S
CO
RE
N
O.
CC
2
SIG
lc'(
kP
a)
99.6
SIG
3c'
CkP
a>
99.6
IND
UC
ED
O
CR
1.0
INC
RE
ME
NT
(c
m)
RE
MO
LD
ED
-SU
RF
T
ES
T
NO
. T
E1
38
800
800
40
0
200
300
1000
p
' (k
Pa)
1500
Al
Q_ o: ^-3
00
u
n-4
00
ST
RR
IN
(JO
CRUISE ST HELENS
CORE NO.
CC2
SIG
lc'(kP
a)
97
.8S
IG3c'(kP
a)
97.8
IND
UC
ED
O
CR
1
.0
INC
RE
ME
NT
(c
m)
RE
MO
LDE
D-S
UR
F
TE
ST
N
O.
TE
139
500
1000
15
00
2000
p
' (k
Pa)
^-1
00
«t tL
^ W-2
00
3 CC ^-3
00
U n-4
00
ST
RR
IN
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'(kPa)
98.5
SIG3c
x(kPa)
98.5
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
TE140
800
600
40
0
200
500
10
00
p'
(kP
a)19
00
id
Q.
-20
03 o: ui
p
-40
0
ST
RR
IN
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C2
SIG
lc'(
kP
a)
10
0.2
SIG
3c'(
kP
a)
10
0.2
IND
UC
ED
OC
R
1.0
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LD
ED
-SU
RF
T
E143
40
0
30
0
20
0
100
30
04
00
60
0 p
' (k
Pa)
80
0
CR
UIS
E
ST
H
ELE
NS
C
OR
E J
NO
L
_C
C2
SIG
lcx(k
Pa)
97.0
SIG
3c'(
kP
a)
97
.0IN
DU
CE
D
OC
R
1.0
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LD
ED
-SU
RF
T
E1
44
STRf
lIN
(SO
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
100.1
SIG3c'(kP<O
100.1
INDUCED OCR
1.0
INCREMENT (c
m)
TEST NO
.REMOLDED-SURF
TE155
400
a 30
0 a.
200
100
200
400
600
p'
CkP
a)80
0
3-1
00
<r J
Q
-20
0
ST
RR
IN
CRUISE ST HELENS
CORE NO.
CC2
INCREMENT (c
m)
TEST NO.
SIGlc'(kPa)
97.4
SIG3c'(kPa)
97.4
INDUCED OCR
1.0
REMOLDED-SURF
TE164
OO
2001
>
150
>
300 0
S00
1000
15
00
p'
CkP
a)20
00
ST
RflIN
CRUISE ST HELENS
CORE NO.
CC3
SIGlc'(kPa)
299.1
SIG3c
x(kPa)
299.1
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO.
RE
MO
LDE
D-S
UR
F
TE
H?
200i
>
150)
300
90
0
1000
13
00
30
00
2
00
p'
(kP
a)
100
-10
0
fE-2
00
U
0-3
00
-400
» <
-) -
t »
-«-»
-j-
t i
I <
|' »
i
^--
f-
ST
RR
IN
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
294.7
SIG3c'(kPa>
294.7
INDUCED OCR
1.0
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
TE148
200i >
150! >
100i
>
500-
CRUISE ST HELENS
CORE NO.
CCS
INCREMENT (c
m)
TEST NO.
SIGlc'(kPa)
299.3
SIG3c'(kPa)
299.3
INDUCED OCR
1.0
REMOLDED-SURF
TE149
10
19
20
ST
RR
IN
C5O
CRUISE ST HELENS
INCREMENT (c
m)
REMOLDED-SURF
CORE NO.
CC2
TEST NO.
TE150
SIGlc'(kPa)
SIG3c'<kPa>
INDUCED OCR
295.9
295.9
1.0
800
600
400
200
500
10
00
p'
(kP
a)
1500
-100
a Q.
-30
0
Ld
Q-4
00
ST
RR
IN
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C2
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LD
ED
-SU
RF
T
E151
SIG
lc'(
kP
a)
26
7.1
SIG
3c'(
kP
a)
106.8
IND
UC
ED
O
CR
1.0
000
40
0
800
1 ' '
d'I
I I
I I
I M
I
I I
I I
I I
I M
I
I I
I I
200
400
600
000
p' CkPa)
10
-10
0
tt (L-2
00
-300
-J
LJ Q-4
00
15
20
ST
RflI
N
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'(kPa)
44.8
SIG3c'(kPa>
44.8
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
TE15
2
I I
I j
I I
I I
| i
I I-H-
STRRIN <5O
CRUISE ST
HELENS
CORE NO
. CC
SINCREMENT (c
m)
TEST NO.
REMOLDED SURF
TE179
SIGlc'CkPa)
97.0
SIG3c
x(kP
a)
97.0
INDUCED OCR
1.0
CRUISE ST HELENS
CORE NO.
CC2 _
SIGlc'(kPa)
96.8
SIG3c'(kPa)
96.8
INDUCED OCR
1.0
INCREMENT (c
m)
TEST NO.
8 12
S
TR
flIN
RE
MO
LDE
D
SU
RF
T
E183
16
10
15
STRRIN
20
CRUISE ST
HELENS
CORE NO.
SL1
INCREMENT
TEST NO.
(cm)
flSH (TUBE)
TE129
SIGlc'(kPa)
100.8
SIG3c'(kPa)
100.8
INDUCED OCR
1.0
20
0
a 15
0 O. or
100
50
100
200
300
p'
(kP
a)
40
0
ST
RR
IN
(5i
CRUISE ST HELENS
CORE NO.
SL4
SIGlc'CkPa)
97.4
SIG3c'(kPa)
97.4
INDUCED OCR
1.0
INCREMENT (cm)
TEST NO
.REMOLDED-SURF
TE170
600
^
600
Q.
.* w
400
200
400
00
600
1200
p
' (k
Pa)
1600
ST
RflI
N
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. S
L4
SIG
lc'C
kP
a)
10
2.9
SIG
3c'(
kP
a)
10
2.9
IND
UC
ED
OC
R
1.0
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LDE
D
SU
RF
T
E1
73
400
300
200
100
20
04
00
(kP
a)
60
08
00
10
15
ST
RflIN
2025
CRUISE ST HELENS
CORE NO
. SL4
INCREMENT
TEST NO
.(cm)
REMOLDED SURF
TE175
SIGlc'(kPa)
298.3
SIG3c'(kPa)
298.3
INDUCED OCR
1.0
00 o
10
15
STRflIN
(JO
CRUISE ST HELENS
CORE NO.
SL4
INCREMENT (cm)
TEST NO.
REMOLDED SURF
TE177
SIGlc'(kPa)
296.0
SIG3c'(kPa)
296.0
INDUCED OCR
1.0
330;
3001
238
w
0. o- 1
30
30 0
tea
200
300
400
300
800
oo
700
ST
H
ELE
NS
C
OR
E
NO
. S
L4 9
6.2
96.2
IN
DU
CED
O
CR
N
/fl
INC
RE
HE
NT
(c
m)
TE
ST
N
O.
RB
IOLD
Er)
S
UR
F
TE
184
00 ro
800
* 600
0.
400
200 0
200
400
600
800
p' (kPa)
CRUISE ST HELENS
CORE NO.
SL4
SIGlc'CkPa)
98.6
SIG3c'(kPa)
98.6
INDUCED OCR
1.0
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
TE185
S50-
I I I I I I I
100 150 200 2*
-50 -
-100
p' (kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) TEST NO.
REMOLDED-SURF D130
SIGlc'CkPa) 33.7SIGSc'CkPa) 33.7INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q CkPa) 36.3 (36.3*)RVG MIN q CkPa) -71.3 (71.3*)
84
oo Ln
0
S-5
w Z £-u
(0 (L
U
Q.-20
- r
a: a
4 e
CYCLE
#
CRUISE ST HELENS
CORE NO.
CC1
SIGic'CkPa)
99.7
SIG3c'(kPa)
99.7
INDUCED OCR
1.0
£
80 60 20
3 e
U
P-2
0
-80
U
1E-K
K I-
1C
-01
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I i
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I >
I |
i i
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| I
I i
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t
i i
104
6 C
YC
LE *
INCREMENT (c
m)
TEST NO.
RE
MO
LDE
D-S
UR
F
D130
ST
flT
IC
q-f
(k
Pa
) 1
00
.0R
VG
M
flX
q
CkP
a)
96.3
(9
6.3
^)
flVG
M
IN
q
(kP
a)
-71.3
(7
1.3
*)
10
-ese
£L
p' (kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) TEST NO.
REMOLDED-SURF D131
SIGlc'(kPa) 37.4SIG3c'(kPa) 37.4INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q (kPa) 46.4 (46.4*)RVG MIN q (kPa) -35.0 (35.0*)
86
oo
20 15 10
2
-20 80
w
60
r
«*cr Q
20
2 3
CY
CL
E
#
a (L
80 60
ID U
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P
40
<E Q!
20
1E
-01
2 3
CY
CL
E
#
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C1
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LDE
D-S
UR
F
D13
1
SIG
lc'(kP
a)
97.4
SIG
3c'(kP
a)
97
.4IN
DU
CE
D
OC
R
1.0
ST
flT
IC qf
(kP
a)
100.0
RV
G
MflX
q
(kP
a)
46.4
(4
6.4
*)R
VG
M
IN
q (k
Pa
) -3
5.0
(3
5.0
*)
100 T
rd CL
-10 -
-20 -
x CkPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) TEST NO.
REMOLDED-SURF D132
SIGlc'CkPa) 98.2SIG3c'CkPa) 98.2INDUCED OCR 1.0
STRTIC q-f (kPa) 100.0RVG MflX q (kPa) 32.3 (32.3*)RVG MIN q (kPa) -21.1 (21. U)
00
w
2 *"2 o: u-e
Q.-8
20 13
a:
a
10
15
CY
CL
E
#2
0
80
60
U 0
40
20
!E+
03g
-
lE+02g-
1E+0
1
1E-0
125
10
13
CY
CL
E
#
CRUISE ST HELENS
CORE NO.
CC1
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D132
SIGlc'CkPa)
98.2
SIG3c'(kPa)
98.2
INDUCED OCR
1.0
STfl
TIC
q-f
(kPa)
100.0
flVG
Mf
lX q
(kPa)
32.3 (32.3?O
MIN q
(kPa)
-21.1 (21.U)
tee-
-20 -
(kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) TEST NO.
REMOLDED-SURF D133
SIGlc'CkPa) 39.5SIG3c'CkPa) 33.5INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 23.6 (23.65ORVG MIN q (kPa) -23.1 (23.
90
o: £ tn u 0.-8
iv* Z M r
a:
a
40
30 10
010
020
0 30
0 C
YC
LE
#
400
CRUISE ST
HELENS
CORE NO.
CC1
SIGlc'(kPa)
99.5
SIG3c'(kPa)
99.5
INDUCED OCR
1.0
200
r\ at
Q
.w
19
0
a
100
(E
U
Q-
90
1E
+0
!
1E
+0
1
1E
+00 y
-
1E
-01
»»! »*
90
01
00
200
300
CY
CLE
#
400
50
0
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D133
STRTIC qf (k
Pa)
100.0
RVG MRX q
(kPa
) 23.6 (2
3.6*
)RVG MIN q
(kPa
) -2
3.1
(23.U)
ida.
-20
-40 -
p' CkPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) TEST NO.
REMOLDED-SURF D134
SIGlc'(kPa) 97.5SIG3c'(kPa) 97.5INDUCED OCR 1.0
STRTIC qf CkPa) 100.0RVG MRX q (kPa) 48.8 (48.8^)RVG MIN q (kPa) -38.0 (38.0^)
92
z £-10
<n
-20
o:
n
40
30
20 10
20
40
80
CY
CL
E
#80
10
0IE
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20
40
60
CY
CL
E
#80
100
CRUISE ST HELENS
CORE NO.
CC1
SIGlc'(kPa)
97.5
SIG3c'(kPa)
97.5
INDUCED OCR
1.0
INCREMENT
TEST NO.
STfl
TIC
qffl
VG Mf
lX q
flVG
MIN q
(cm)
(kPa)
(kPa)
(kPa)
REMOLDED-SURF
D134
100.0
48.8 (48.85O
-38.0 (38.05O
-S58-
288 --
Q. 158 --
U)en u a:h- cn
u QH I I I | I I I I | »
188
-48 -
-28
STRRIN (JO
p' (kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) REMOLDED-SURF TEST NO. D135
SIGlc'CkPa) 99.5SIG3c'CkPa> 99.5INDUCED OCR 1.0
STflTIC qf CkPa) 100.0RVG MflX q (kPa) 47.4 (47.4*)RVG MIN q (kPa) -36.4 (36.455)
94
-5
M-1
0
-13
K-2
0 15 »g
10
19
CY
CL
E
#20
CRUISE ST
HELENS
CORE NO.
CC1
/-s (0
Q.
Ul o:
ui
80 60 40 28
Ul
1E+0
1
1C-0
129
10
19
CY
CL
E
#20
INCREMENT (cm)
TEST NO
.REMOLDED-SURF
D135
SIGlc'<kPa>
99.5
SIG3c'<kPa)
99.5
INDUCED OCR
1.0
STfl
TIC
q-f
<kPa>
100.0
RVG Mf
lX q
<kPa>
47.4
(4
7.45
Ofl
VG MIN q
(kPa)
-36.
4 (3
6.45
O
23
250-
rd Q_
-20 -
-40 -
x (kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) REMOLDED-SURF TEST NO. D136
SIGlc'(kPa) 97.8SIG3c'CkPa) 97.8INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q (kPa) 61.9RVG MIN q (kPa) -41.5 C41.5*)
96
-15
-20
80 60
- r a: a
20
2 3
CYCLE
#
CRUISE ST
HELENS
CORE NO.
CC1
SIGlc'CkPa)
97.8
SIG3c'(kPa>
97.8
INDUCED OC
R 1.0
* a.
80 60
D U
40
Q k!20
0
1E+03 |-
lE4-
02«-
1E+01
1E+00S-
IE-0
12
3 C
YC
LE
*
INCREMENT (c
m)
TEST NO
.REMOLDED-SURF
D136
STflTIC
qf (kPa)
100.0
RVG
MflX q
(kPa
) 61
.9 (61.95i)
RVG MI
N q
(kPa
) -4
1.5
(41.
55O
a a.
en u a:h- cn
u a
ieo -*-- STRRIN
p' (kPa)
CRUISE ST HELENS CORE NO. CC1
INCREMENT (cm) REMOLDED SURF TEST NO. D137
SIGic'(kFa) 35.3SISSc'CkPa) 3i5.3INDUCED OCR 1.0
STflTIC qf (kPa) 108.0BVG HRX q (kPa) 33.4 (33.fiVG HIN q (kPa) -32.8
98
CY
CLE
*
CY
CLE
#
CRUISE
1 CORE NO
SIGlc'(
ST HELENS
. kf»*>
SIG3o'CkP*>
INDUCED
OCR
CCl 93 95 i.
. . 0
3 3
INCREMENT
TEST MO
STHTIC
RVG MRX
RVG MIN
. q* q q
(cm)
CkP*)
(kP&)
CkPsi)
REMOLDED
D1S?
iae.
£33.4
-32.11 C3
8.) (32
SURF
45O
.8^)
tee-
p' (kPa)
CRUISE ST HELENS CORE NO. CCi
SIGlc'(kPa) 98.3SIG3c x (kPa) 96.3INDUCED OCR 1.0
INCREMENT (cm) REMOLDED SURF TEST NO. D138
STRTIC qf (kPa) 138.8RVG MflX q (kPa) 27.3 (27.3%)flVG MIN q (kPa) -2S.7 (26.7*)
100
0
o
M-8
a: (0 a:
u
a.-1
6
"Z.
M a:
o
30
20
10
is
CY
CLE
*
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C1
SIG
lc'(kP
a)
SIG
3c'(kP
a)
IND
UC
ED
O
CR
96.3
96
.31
.0
1E-0
110
13
C
YC
LE
#
20
INCREMENT (cm)
TEST NO.
REMOLDED SURF
D198
STfl
TIC
qf (kPa)
108.0
RVG MRX q
(kPa
) 27.3
RVG MIN q
(kPa
) -^6.7
100-
rtf Q_
p" (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D137
SIGlc'(kPa) 99.8SIG3c'(kPa) 99.8INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q (kPa) 33.2 (33.2*)RVG MIN q (kPa) -28.9 (28.9*)
102
O
LO
z £-10
h- tn ec
u
o.-2
0 20 15
C3 z M a. r
a:
a
10
is
CY
CLE
#
20
CRUISE ST
HELENS
CORE NO
. CC
2
25
a* (L
80 60
ID
_J
U 0
40
a:
u20
1E+0
4
1E+0
2
1E+0
1
1E
-01
10
15
CY
CL
E
#20
25
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D137
SIGlc'(kPa)
99.8
SIG3c'(kPa)
99.8
INDUCED OCR
1.0
STRTIC qf (kPa)
100.0
RVG MRX q
(kPa)
33.2 (33.25O
RVG MIN q
(kPa)
-28.9 (28.95i)
fdCL
en en LJCK1-en
LJ
H I I f- I I h H I I \
Id CL
-28 -15
STRRIN (50
p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D138
SIGlc'CkPa) 97.6SIG3c'(kPa) 97.6INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q CkPa) 39.0 (39.0%)RVG MIN q (kPa) -39.9 (39.9%)
104
O
Ln
or Of H- 0)
-15
or
LJ
Q.-2
0 40
30
o:
Q
10
102
0
30
C
YC
LE
#
40
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'(kPa)
SIG3c'CkPa)
INDUCED OCR
97.6
97.6
1.0
80
-
60
-
at (L ZD d U
20
Q. lE
+0
4a-
1E
+033-
1E
+023-
1E+
01
1E-0
150
1020
30
CY
CLE
#
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D138
ST
flT
IC
q-f
(k
Pa)
10
0.0
flVG
M
RX
q
(kP
a)
39
.0
C3
9.0
5O
MIN
q
(kP
a)
-39.9
(3
9.9
*)
tee-
rdQ_
p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D139
SIGlc'(kPa) 98.8 STRTIC qf CkPa) 100.0SIG3c'CkPa) 98.8 RVG MRX q (kPa) 30.9 (30.9*)INDUCED OCR 1.0 RVG MIN q (kPa) -30.6 (30.6.*)
106
(T -
1QL I- (T LJ
-3
0.
-4
20 15
(T n
108
0
30
C
YC
LE
#
CRUISE ST HELENS
CORE NO
. CC2
SIG
lc'(kP
a)
98.6
SIG
3c'(kP
a)
98.6
IND
UC
ED
O
CR
1
.0
LJ
IE-0
1
50 INCREMENT (cm)
TEST NO.
10
20
3
0
CY
CLE
#
RE
MO
LD
ED
-SU
RF
D
13
9
40
50
STRTIC qf
(kPa)
100.0
RVG MRX q
(kPa)
30.9 (30.9*)
RVG MIN q
(kPa)
-30.6 (30.6?O
a.
en en LJ
cn
LJa
100
80 -
60 -
40 -
20 -
0
-20 -
-40
p' CkPa)
CRUISE ST HELENS INCREMENT (cm) REMOLDED-SURF CORE NO. CC2______TEST NO.________D140________
SIGlc'(kPa) 97.7 STRTIC qf CkPa) 100.0SIG3c'(kPa) 97.7 RVG MRX q CkPa) 46.3 (46.3*)INDUCED OCR 1.0 RVG MIN q CkPa) -46.8 (46.855)
108
10 5 0
M-5
a: te Sn-1
0
a: ,s
u
15Q
-
-20
(J
Z (T
P
40
30
30 10
1020
30
CY
CL
E
#4
0
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
97.7
SIG3c'(kPa)
97.7
INDUCED OCR
1.0
a Q-
80 60
ID _J U
40
Q (T U
20
CL
1E+
04
1E+
03
1E
+02
1E+
01
IE+
00
IE-0
1S
010
20
30
CY
CL
E
ft40
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D140
ST
RT
IC
q-f
(kP
a)
10
0.0
RV
G
MflX
q
(kP
a)
46.3
(4
6.3
*)
RV
G
MIN
q
(kP
a)
-46
.8
(46
.8*)
tea-
to tu o> in O
p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D141
SIGlc'(kPa) 98.5SIG3c x (kPa) 98.5INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 28.3 C28.35OflVG MIN q (kPa) -28.9 (28.9*)
110
100
130
CY
CL
E
#3
00
CRUISE ST HELENS
CORE NO.
CC2
SIG
lc"(
kP
a)
98
.5S
IG3c'(kP
a)
98
.5IN
DU
CE
D
OC
R
1.0
At
Q.
=3 ui Q (L
111
Q.
80
60
u
1E+
01
1E
-01
230
50
100
130
CY
CL
E
#200
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D141
STRTIC qf (kPa)
100.0
RVG MRX q
(kPa
) 28.3 (28.3*)
RVG MIN q
(kPa)
-28.9 (28.95O
rtJ Q_
-20
-40 -
p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT Com) REMOLDED-SURF TEST NO. D142
SIGic'(kPa) 98.0 STRTIC qf (kPa) 100.0SIG3c'CkPa) 98.0 RVG MRX q (kPa) 46.6 (46.6^)INDUCED OCR 1.0 RVG MIN q (kPa) -44.5 (44.5*)
112
,\*-
5
DC -
a:
\- 0) a:
u
a.-2
0 40 30
Q. o:
a
10
10
15C
YC
LE
#
CRUISE ST HELENS
CORE NO.
CC8
SIGlc'CkPa)
98.0
SIG3c'CkPa)
98.0
INDUCED OCR
1.0
25
a 0. _
Id a a: Id a.
80
60
40 20
/A
Of a. Id
1E
+04
!E+
03
g-
lE+
02
sj~
1E+
01
IE-0
1
jf-
INCREMENT Co
m)
TEST NO.
10
15
CY
CL
E
#20
25
REMOLDED-SURF
D142
STfl
TIC
qf (k
Pa)
100.0
RVG MRX q
(kPa
) 46.6 (46.65O
RVG MIN q
(kPa
) -44.5 (44.55O
rd Q.
(kPa)
CRUISE ST HELENS CORE NO. CC2
SIGlc'CkPa) 99.0 SIG3c'(kPa) 99.0 INDUCED OCR 1.0
INCREMENT TEST NO.
STRTIC qf RVG MRX q RVG MIN q
(cm)
(kPa) (kPa) (kPa)
REMOLDED-SURF D143
100.0 22.8 (22.8*) -23.2 (23.255)
114
4 2
~ 0
Z M or-2
a: UJ-6
-8
40
30
Z 1-1
Q.
21 a:
a
10
100
(0 a.
200
150
u a
100
a:
u
a.
50
/->> Q. w
U
1E+0
4
lE+
03
g-
1E+0
2
1E+0
1
20
0
30
0
CY
CL
E
#400
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. C
C2
500
INC
RE
ME
NT
T
ES
T
NO
.
100
20
0
30
0
CY
CL
E
#400
500
(cm
)REMOLDED-SURF
D143
SIGlc'CkPa)
99.0
SIG3c'CkPa)
99.0
INDUCED OCR
1.0
STRTIC qf (k
Pa)
100.0
RVG MRX q
(kPa
) 22.8 (22.8%)
RVG MIN q
(kPa)
-23.2 (23.2*)
-tee
p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D144
SIGlc'CkPa) 97.9SIGSc'CkPa) 97.9INDUCED OCR 1.8
STRTIC qf (kPa) 108.0RVG MRX q (kPa) 32.9 (32.9*)RVG MIN q (kPa) -34.5 (34.5*)
116
2 M o:
en <r
LJ0 -2 4
0
30
M
£ (E
O
10
20
40
6
0
CY
CL
E
#00
CRUISE ST HELENS
CORE NO.
CC2
SIG
lc'(kP
a)
SIG
3c'(kP
a)
IND
UC
ED
O
CR
00
a (L
60
LJ
O (E
LJ
40
20
0
-20
(0
lE+
03
g-
U
1E+
01
1E+C
IE-0
110
020
40
6
0
CY
CL
E
#
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D144
97.9
STfl
TIC
qf (kPa)
100.0
97
.9
RV
G
MflX
q
(kP
a)
32.9
(3
2.9
JO
1.0
R
VG
M
IN
q (k
Pa
) -3
4.5
(3
4.5
^)
100
-258-
-100p' CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D145
SIGlc'(kPa) 38.1SIG3c'(kPa> 98.1INDUCED OCR 1.0
STflTIC qf (kPa) 100.3RVG MflX q (kPa) 50.4 (50.45ORVG MIN q CkPa) -48.3 C48.35O
118
5
fc-1
0
H tn-
o:
u
Q.-2
0
I I
I I
f -4
I I
I <
I I
I I I »
o:
40
30
20 10
102
0
30
C
YC
LE
#
4050
at (L
60
60
_
U 0
40
o:
u20
lE+
04
g~
lE+
03s-
1E+
02
1E+0
1
1E-0
11
02
0
30
C
YC
LE
#
40
CRUISE ST HELENS
CORE NO.
CC2
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
D145
SIGlc'CkPa)
98.1
SIGSc'CkPa)
98.1
INDUCED OCR
1.0
STfl
TIC
qf (kPa)
100.0
flVG Mf
lX q
(kPa
) 50.4 (50.45i)
flVG
MIN q
(kPa
) -48.3
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) REMOLDED-SURF TEST NO. D161
SIGlc'CkPa) 94.3 STRTIC qf (kPa) 100.8SIGSc'CkPa) 94.3 RVG MRX q (kPa) 34.8 (34.8*)INDUCED OCR 1.0 RVG MIN q CkPa) -38.1 (30.
120
Cfl-1
5(E
LJ
Q
.-2
0
o:
Q
40
30 20 10
at
Q_
80 60
^
^«,
n
40
a:
a!
20
\ /
i I
| -i -ill
{ \-
\ i
< |
I-I
i \-
\-\-
-\
-\
1E+0
-4
1E
+033-
rt a. u1
E+
01
1E
-01
10
is
CY
CLE
#
2025
10
15
CY
CL
E
#
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
94.3
SIG3c'(kPa)
94.3
INDUCED OCR
1.0
INC
RE
ME
NT
(c
m)
TE
ST
^NO
^^
STRTIC qf (kPa)
RVG MRX q
(kPa)
RVG MIN q
(kPa
)
REMOLDED-SURF
D161____ __
100.0
34.8 (34.8*)
-30.1 (3
0. ISO
20
100
Q_
\-~i>
0)cn u
cn
uQ
STRRIN (SO
-50
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D162
SIGic'(kPa) 72.1SIG3c x (kPa) 72.1INDUCED OCR 1.0
STRTIC qf CkPa) 100.0RVG MflX q (kPa) 39.6 (39.6*)RVG MIN q (kPa) -27.4 (27.4*)
122
ho U)
-3
Si-
10
UJ
Q_-2
0 80
60
z M 0. a:
Q
20
23
CY
CL
E
#
CRUISE ST
HELENS
CORE NO.
CC2
SIG
lc'(
kP
a)
72
.1S
IG3c'(
kP
a)
72.
1IN
DU
CED
O
CR
1.0
80
a) tL
80
3
40
U
Q20
o: UJ
-20
lE+0
3=»-
lE+02=r~
0. v^ UJ
IE-0
1
INCREMENT (cm)
TEST NO.
23
CY
CL
E
#
REMOLDED-SURF
D162
STRTIC qf
(kPa)
100.0
RV
G
MR
X
q
(kP
a)
39
.6
(39.6
*)
RV
G
MIN
q
(k
Pa
) -2
7.4
(2
7.4
*)
p x CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D146
SIGlc'CkPa) 299.3 STRTIC qf CkPa) 300.0SIGSc'CkPa) 299.3 flVG MRX q (kPa) 98.1 (32.7%)INDUCED OCR 1.0 flVG MIN q (kPa) -90.5 (30.2*)
124
0
CC a
en-1
5
CC
LJ
Q.-2
0
(C
Q
40
30 20 10
0
r-r-
t-r-
T^
-v I
i
i i
10
13
CY
CL
E
#20
CRUISE ST HELENS
CORE NO.
CC2
tf Q.
400
300
ui Q
200
(E
UI10
0
0.
^ W
Ul
IE +
01
1E
-01
23 INC
RE
ME
NT
(c
m)
SIG
lc'(kP
a)
SIG
3c'(kP
a)
IND
UC
ED
O
CR
29
9.3
299.3
1.0
10
13
CY
CLE
#
RE
MO
LDE
D-S
UR
F
D146
ST
RT
IC q
f (k
Pa
) 3
00
.0R
VG
M
RX
q
(kP
a)
98
.1R
VG
M
IN
q (k
Pa
) -9
0.5
<
30
.2$
O
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDEB-SURF D147
SIGlc'(kPa) 297.0 STRTIC qf (kPa) 300.0SIG3c'(kPa) 297.0 RVG MRX q CkPa) 118.9 (39.65OINBUCEB OCR 1.0 RVG MIN q CkPa) -110.7 (36.3*)
126
x-s
v/ ft:
-15
u ft.-2
0 30
£ 20
o: a
10
10
13
CY
CL
E
#20
CRUISE ST HELENS
CORE NO.
CC2
_J
U
Q CC
U
Q.
40
0
300
200
100
1E+
0!
U1E
+02
g-
1E+
01
1E-0
123
10
13
CY
CL
E
#
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
D147
SIGlc'CkPa)
SIG3c'CkPa)
INDUCED OCR
297.0
STRTIC qf (kPa)
297.0
RVG MRX q
(kPa)
1.0
flVG
MIN q
(kPa)
300.0
118.9
(39.
65O
-110.7 (36.95i)
20
258-
Q_
Q- ;
cn en u
cn
u o
250
200-
-20 -15 -10
STRRIN C%esa-
x CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D148
SIGlc'CkPa) 297.4 STRTIC qf CkPa) 300.0SIG3c'(kPa) 297.4 RVG MRX q (kPa) 103.2 C34.45OINDUCED OCR 1.0 RVG MIN q CkPa) -104.9 (35.0*)
128
0
*\* w 5-i0
a: Of a:
w
a.-2
0
200
~ w
150
e> £
100
a: Q
30 0
U^1_JJJ^^I^
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| P"
1
-t
1 1
1
1 1
1 |
1 1
1 1
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10
20
30
40
9C
CY
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#
40
0
*
0.
w
30
0
P
200
CC
OL
100
0
1E
+03
lC-t
-04
^
1E
+03
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1E
+02
U
1E
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1E+0
C
IE-0
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1/f
t i
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i i i
i
i i
i i
i i
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^^---^_
^
r v
r r 5~ _ r
10
20
30
40
50
CY
CL
E
#
CR
UIS
E
ST
H
ELE
NS
IN
CR
EM
EN
T
(cm
) R
EM
OLD
ED
-SU
RF
CO
RE
N
O.
CC
2 T
ES
T
NO
. D
14
8
SIG
lc'(kP
a)
29
7.4
S
TflT
IC qf
(kP
a)
30
0.0
S
IG3
c'(kP
a)
29
7.4
R
VG
M
flX
q (k
Pa
) 103.2
(3
4.4
*O
IND
UC
ED
O
CR
1
.0
RV
G
MIN
q
(kP
a)
-104.9
(3
5.0
5O
rd CL
0)u Q:h- cn
LJ O
STRRIN (SOsee-
i i/ i i i i i i i i i i300 400 5t 0
x CkPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D149
SIGlc'(kPa) 297.3 STRTIC qf (kPa) 300.0SIG3c'(kPa) 297.3 RVG MRX q (kPa) 135.4 (45.1^)INDUCED OCR 1.0 RVG MIN q CkPa) -117.8 (39.3*)
130
a: 0) CC a -20 00 60
Si (E n
20
02
3 C
YC
LE
#
200
100
50
So
Q.
-50
1E
+04|-
lE+
02
ar
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01
1E
-01
II
I |
< I II
| I
1 I
I j
I *
I «
{-
4;4
--f-
-«
2 3
CY
CL
E
CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
SIGSc'CkPa)
INDUCED
OCR
297.3
297.3
1.0
INCREMENT
TEST NO.
STfl
TIC
qffl
VGfl
VGMf
lXMIN
q q
(cm)
CkPa)
(kPa)
(kPa)
REMOLDED-SURF
D149
300.0
135.
4_
<17
.8(45. (39
15i)
.3*)
-20 -
-40 -
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
SIGlc'CkPa) 95.5SIG3c'(kPa) 95.5INDUCED OCR 1.0
INCREMENT (cm) TEST NO.
REMOLDED-SURF D 179
STRTIC qf (kPa) 180.0RVG MRX q (kPa) 37.7RVG MIN q (kPa) -31.8
132
20 15 10
U OL-10
-15 80
60
2 M a.
20
I t
«II
I I
«
0.4
,8
1.2
C
YC
LE
*
1.6
80
£
60
w 3
40
UJ a
0
1E
+04
1E
+0
3
0
i
1E
+02
W LJ
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+01
1E+
0B
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cii
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^-"
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X
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,,,,,,.... M
y ..........
r
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^^
r
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1.3
C
YC
LE
*
CRUISE ST HELENS
CORE NO.
CC2
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
D 179
SIGlc'CkPa)
95.5
SIG3c'CkPa>
95.5
INDUCED OCR
1.0
STRTIC qf Ck
Pa)
100.0
RVG MRX q
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) 37.7 (3
7.RVG MIN q
CkPa
) -31.8 (3
1.8*
)
1.6
-tea
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D180
SIGlc'CkPa) 100.7 STRTIC qf (kPa) 100.0SIGSc'CkPa) 100.7 RVG MflX q (kPa) 27.7 (27.755)INDUCED OCR 1.0 RVG MIN q (kPa) -27.3 (27.3%)
134
16
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m)
TEST NO.
10
20
30
CYCLE *
REMOLDEB-SURF
0180
SIGlc'CkPa)
SIG3c'CkPa)
INDUCED OCR
100.
7 ST
flTI
C qf
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100.0
100.7
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27.7 (2
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50
40
30
20
10
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20 40 60 80 It
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ft1/i !
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CRUISE ST HELENS INCREMENT (cm) REMOLBEB-SURFCORE NO. CC2 TEST NO. B181
SIGlc'CkPa) -108.6 STRTIC qf (kPa) 100.0 SIGSc'CkPa) -108.6 RVG MRX q (kPa) 33.3 (33.3*) INDUCES OCR 1.0 RVG MIN q (kPa) -37.0 (37.0*)
136
ft:
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2 3
CYCL
E *
REMOLDED-SURF
D181
SIGlc'(kPa)
-108.6 STRTIC qf (k
Pa)
100.0
SIG3c'(kPa)
-108.6 RVG Mf
lX q
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) 39.3 (39.3*)
INDUCED OCR
1.0
flVG MIN q
(kPa
) -37.0 (37.0*)
en enLdai- cn
LJa
STRflIN (JO
p' CkPa)
CRUISE ST HELENS CORE NO. CCS
INCREMENT (cm) TEST NO.
REMOLBEB-SURF 0182
SIGic'CkPa) 93.9SIGSc'CkPa) 93.9INBUCEB OCR 1.8
STflTIC qf CkPa) 100.8RVG MRX q (kPa) 43.7 (43.752)RVG MIN q (kPa) -38.7 (38.7*)
138
« I -4
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4
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CRUISE ST HELENS
CORE NO.
CC2
SIGlc'CkPa)
93.9
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93.9
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1.0
80
a 0. ID U P
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TEST NO.
CY
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MO
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D
182
ST
flT
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(kP
a)
10
0.0
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q
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a)
43.7
(4
3.7
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RV
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MIN
q
(kP
a)
-38.7
(3
8.7
^)
tee-
p' (kPa)
CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED-SURF D183
SIGlc'(kPa) 95.8 STRTIC qf (kPa) 100.0SIG3c'CkPa) 95.8 RVG MRX q (kPa) 41.4 (41.4*)INDUCED OCR 1.0 RVG MIN q (kPa) -36.1 C36.U)
140
0
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30
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110
4 6
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CL
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INCREMENT (c
m)
TEST NO.
STRTIC qf (kPa)
flVG
Mf
lX q
(kPa)
RVG MIN q
(kPa
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MO
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ST HELENS INCREMENT (cm)CORE NO. CC2 TEST NO.
SIGlc'(kPa) 100.3 STRTIC q-f (kPa) SIG3c'(kPa) 100.3 RVG MRX q (kPa) INDUCED OCR N/fl RVG MIN q (kPa)
i | i j i i i i
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142
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ST
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CRUISE SI HELENS CORE NO. CC2
SIGie'CkPa) 95.!3IG3c'(kPa5 95.SINDUCED OCR 1.8
INCREMENT TEST NO.
REMOLBEB SURF B13S
3TRTIC qf CkPa)RVG MRX q CkPa) 42.8RVG HIN q CkPa) -42.3 C4S.83O
144
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REMOLDED SURF D185
SIGlc'(kPa) 284.3 STRTIC qf CkPa) 383.3SIG3c'CkPa) 234.3 RVG MRX q CkPa) 115.2 (38.4^)INDUCED OCR 1.3 RVG MIN q CkPa) -31.2 C30.43O
146
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2 (3
0.4^
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£50-
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CRUISE ST HELENS CORE NO. CC2
(kPa)
INCREMENT (cm) REMOLDED SURF TEST NO. D186
SIGlc'(kPa) 237.3 STRTIC qf CkPa) 300.0SIG3c'(kPa> 297.3 RVG MRX q (kPa) 92.1 (30.75i)INDUCED OCR 1.0 RVG MIN q (kPa) -79.7 (26.6*)
148
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30
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40
0
30
0
20
0
100
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m)
TEST NO.
REMOLDED SURF
D186
SIGlc'CkPa)
SIGSc'CkPa)
INDUCED OCR
297.3
297.3
1.0
STRTIC qf (k
Pa)
300.0
RVG MRX q
(kPa
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(3
0.7*
>RVG MIN q
CkPa)
-79.7 (26.6^)
-88 -
CRUISE ST HELENS CORE NO. CC2
CkPa)
INCREMENT (cm) REMOLDED SURF TEST NO. D187
SIGlc'CkPa) 293.2 STRTIC qf CkPa) 380.8SIG3c'CkPa> 293.2 RVG MRX q CkPa) 138.7 (33.6?OINDUCED OCR 1.8 RVG MIN q CkPa) -84.9 (28.3*)
150
4 »
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40
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200
100
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2
10 INCREMENT (cm)
TEST NO.
4 3
CYCLE *
REMOLDED SURF
D187
SIG3c'(kPa)
INDUCED OCR
293.2
293.2
1.0
STRTIC qf (kPa)
300.0
RVG
MRX q
(kPa)
100.7
(33.6*)
RVG
MIN q
(kPa
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4.9
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CRUISE ST HELENS CORE NO. CC2
INCREMENT (cm) TEST NO.
REMOLDED SURF D188
SIGlc'CkPa) 236.5 STRTIC qf CkPa) 300.0SIG3c'(kPa> 236.5 RVG MRX q (kPa) 68.0 (22.7^)INDUCED OCR 1.0 RVG MIN q (kPa) -80.4 (26.8^)
152
5-8
CC
Of
CC
Ld
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6
g« 20
020
40
6
0
CY
CL
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80
CRUISE ST
HELENS
CORE NO.
CC2
100
1E
-01
2040
6
0
CY
CL
E
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a
INCREMENT (cm)
TEST NO.
REMOLDED SURF
D188
SIGlc'(kPa)
296.S
STRTIC qf (kPa)
300.0
SIGSc'CkPa)
296.5
RVG Mf
lX q
(kPa)
68.0 (2
2.75
OINDUCED OCR
1.0
HVG MIN q
(kPa)
-80.4
(26.8?i)
CkPa)
CRUISE ST HELENS CORE NO. SL1
INCREMENT (cm) TEST NO.
RSH (TUBE) D155
SIGlc'(kPa) 38.7SIG3c'(kPa) 98.7INDUCED OCR 1.0
STRTIC qf (kPa) 36.4RVG MP.X q (kPa) 78.6 (81.5^)RVG MIN q (kPa) -63.2 (55.6*)
154
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80
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CYCLE *
INCREMENT (cm)
RSH (TUBE)
TEST NO.
D155
SIGlc'(kPa)
98.7
SIG3
c'(kP<*)
98.7
INDUCED OCR
1.0
STRTIC qf
(k
Pa)
96.4
RVG MRX q
(kPa
) 78
. G
(81.5*)
RVG MlN q
(kPa
) -63.2 (6
5.6*
)
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M I I 1 i I I I I I I j I I II
p' (kPa)
CRUISE ST HELENS CORE NO. SL1
INCREMENT (cm) TEST NO.
RSH (TUBE) D156
SIGlc'CkPa) 98.0SIGSc'CkPa) 98.0INDUCED OCR 1.0
STRTIC qf (kPa) 96.4RVG MRX q CkPa) 45.0 <46.7?ORVG MIN q (kPa) -46.3 <48.7*)
156
20
IS
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NO.
SL1
LJ
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100
20
INCREMENT (c
m)
TEST NO.
40
6
0
CY
CL
E
#
RS
H
(TU
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156
80
SIGlc'CkPa)
98.0
SIGSc^kPa)
98.0
INDUCED OCR
1.0
ST
flT
IC
q-f
(kP
a)
96
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VG
M
RX
q
(k
Pa
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6.7
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RV
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M1N
q
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a)
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(4
8.7
JC)
CkPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT Com) TEST NO.
REMOLDED-SURF D163
SIGlc'CkPa) 93.3SIGSc'(kPa) 93.3INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 38.2 (38.25i)RVG MIN q (kPa) -30.5 (30.5*)
158
20 15
2
10
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30 20 10
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CYCLE #
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SL4
10
Ui
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14
6 C
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LE
#
10
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D163
SIGlc'CkPa)
93.3
SIG3c'(kPa)
93.3
INDUCED OCR
1.0
STRTIC qf (kPa)
100.0
RVG Mnx q
(kPa)
38.2 (3
8.2*
)MIN q
(kPa)
-30.5 (3
0.5*
)
p' CkPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED-SURF D164
SIGle'(kPa) 96.0SIG3e'CkPa) 96.0INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 21.1 C21.15C)RVG MIN q (kPa) -18.3 C18.3JO
160
cr>
5 0
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030
100
130
CY
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0
CRUISE ST HELENS
CORE NO.
SL4
SIG
lc'(kP
a)
96.0
SIG
3c'(kP
a)
96.0
IND
UC
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1
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230
ft
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130
100
130
CY
CL
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230
INC
RE
ME
NT
(c
m)
TE
ST
N
O.
RE
MO
LDE
D-S
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F
D164
ST
flT
IC qf
(kP
a)
100.0
RV
G
MflX
q
(kP
a)
21
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q
(kP
a)
-18.3
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8.3
*)
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50
40 -
30 -
20 -
10 -
U"
-10 -
-20 -
p' CkPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED-SURF D165
SIGlc'(kPa) 87.8SIG3c'(kPa) 87.8INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MRX q (kPa) 25.2 (25.2^)RVG MIN q (kPa) -20.9 (20.9*)
162
5:~i
0 o: <r
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0
80
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60
CE
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10
15
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20
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OR
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NO
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SIG
lc'(kP
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87.8
SIG
3c'(kP
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87.8
IND
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id
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80
-
60
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40
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20
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1E
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2
lE+
01
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1E
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2510
15
CY
CLE
#
20
25
INCREMENT (cm)
TEST NO.
REMOLDED-SURF
D165
STRTIC qf (kPa)
100.0
RV
G
MR
X
q (k
Pa)
25.2
(2
5.2
5O
RV
G
MIN
q
(kP
a)
-20.9
(2
0.9
*)
-tee
p' (kPa)
CRUISE ST HELENS CORE NO. SL4
SIGic'(kPa) 86.6SIG3c'(kPa) 86.6INDUCED OCR 1.0
INCREMENT (cm) TEST NO.
REMOLDED-SURF D166
STRTIC qf (kPa) 100.0RVG MRX q (kPa) 23.9 (23.9*)RVG MIN q (kPa) -21.9 C21.95O
164
Ln
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or
Q
20 15 10 0 40
30 10
0
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40
60
12
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#
160
CRUISE ST HELENS
CORE NO.
SL4
SIGlc'CkPa)
86.6
SIG3c
x(kPa)
86.6
INDUCED OCR
1.0
200
IE-0
14
060
120
CY
CL
E
#16
3200
INCREMENT (c
m)
TEST NO.
REMOLDED-SURF
D166
STfl
TIC
qf (k
Pa)
100.0
RVG Mf
lX q
(kPa)
23.9 (2
3.9%
)RVG MIN q
(kPa)
-21.9 (2
1.9%
)
139-
p' CkPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED SURF D169
SIGlc'CkPa) 99.5SIGSc'CkPa) 99.5INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 37.9 (37.3*)RVG MIN q (kPa) -29.4 (29.4*)
166
£-2
I- ui ft
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40
38
ft. o: Q
10
1020
30
CY
CLE
#
40
CR
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ST
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ELE
NS
C
OR
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NO
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L4
SIG
lc'(
kP
a)
99
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IG3c'(
kP
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99
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DU
CED
O
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1.0
50
80
/^ at
(L
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60
ID
J
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40
£
20a. at (L U
lE+
02g-
1E+0
1
1E
-01
1020
30
CY
CL
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#40
INCREMENT (c
m)
TEST NO.
REMOLDED SURF
D169
STRTIC qf (kPa)
100.0
RVG MRX q
(kPa)
37.9 (37.9SO
RVG MIN q
(kPa)
-29.4 (29.45O
I «r-H I I I I
48 -
28 -
8
-28 -
-48 -
p' CkPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) SURF TEST NO. D170
SIGic'CkPa) 97.4SIGSc'(kPa) 97.4INDUCED OCR 1.0
STRTIC qf CkPa) 100.0RVG MRX q (kPa) 48.3 (48.3*)RVG MIN q CkPa) -48.6 (48.6*)
168
Z M in LJ
Q.-4
M r 20
a: Q
e 12
C
YC
LE *
ie
CRUISE ST HELENS
CORE NO.
SL4
SIGlc'(kPa)
97.4
SIG3c'(kPa>
97.4
INDUCED OCR
1.0
20
80* Q. w 00
U P 40
(C U
0-20
0
1E+
04 |-
lE+
03s-
1E+0
1 3-
IE-0
1
L I
I.J
I <
* I
I I
» f
INCREMENT
TEST NO.
(cm)
ST
RT
IC qf
(kP
a)
RV
G
MflX
q
(kP
a)
RV
G
MIN
q
(kP
a)
8 12
C
YC
LE
#
SU
RF
D17
0 _____
100.0
48
.3
(48.3
*)-4
8.6
(4
8.6
SO
16
a) « Momsana)CO CO CO
p x (kPa)
CRUISE ST HELENS CORE NO. SL4
SIGlc'(kPa) 36.8SIG3c'(kPa) 36.8INDUCED OCR 1.8
INCREMENT (cm) TEST NO.
REMOLDED SURF D189
STRTIC qf (kPa) 180.8RVG MRX q (kPa) 27.3 (27.RVG MIN q (kPa) -26.8 (26.85O
170
fi-i
h-
W *-
u CL
20
w
j3C3
Z »H ft-
id
r
l0a:
» «
« t-
i
20
40
60
CY
CL
E
#80
100
IE-0
1
CRUISE ST HELENS
CORE NO.
SL4
INCREMENT (c
m)
TEST NO.
20
40
60
CYCLE *
REMOLDED SURF
D189
SIGlc'CkPa)
96.8
SIG3c'(kPa)
96.8
INDUCED OCR
1.0
STRTIC qf (kPa)
100.0
RV
G
MflX
q
(kP
a)
27
.9
(27
.95
i)R
VG
M
IN
q (k
Pa
) -2
6.8
wa
(kPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED SURF D130
SIGic'(kPa) 38.1SIG3c'CkPa) 38.1INDUCED OCR 1.0
STRTIC qf (kPa) 100.0RVG MflX q (kPa) 41.6 (41.RVG MIN q (kPa) -38.1 (38.
172
(0 (T
U
Q_-8
U)
w
15
2 M i.
80
o. w
60
W
^«
n
40
x (T ol
20
1E+0
3 |-
10 0. Ul
1E+0
1
1E-0
110
15
CYCLE *
20
CRUISE ST
HELENS
CORE NO.
SL4
SIGlc'(kPa)
98.1
SIG3c'(kPa)
98.1
INDUCED OCR
1.0
25 INC
RE
ME
NT
(c
m)
JE
ST
JJ
O,,
STflTIC
qf (k
Pa)
MRX q
(kPa
)MIN q
(kPa
)
10
15
CY
CLE
*
REM
OLD
ED
SUR
F IH
9J3
10
0.0
41.6
(4
1.6
%)
-38.1
(3
8.
23
tea-
p' CkPa)
CRUISE SI HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED SURF D131
SIGlc'CkPa) 36.6 STRTIC qf CkPa) 100.0SIG3c'CkPa) 96.6 RVG MRX q CkPa) 31.3 (31.3*)INDUCED OCR 1.0 RVG MIN q (kPa) -28.S (28.6*)
174
Z £ ft:
-12
o: UJ
Q.-1
0 20 13
a: n
00
12
CYCLE #
16
CRUISE ST
HELENS
CORE NO
. SL
4
UJ
IE-01
20 INCREMENT (cm)
TEST NO.
8 12
C
YC
LE
#
RE
MO
LDE
D
SU
RF
D
19
1
SIGlc'(kPa)
96.6
STflTIC
qf (kPa)
100.0
SIG3c'<kPa)
96.6
RVG MRX q
(kPa
) 31.3 (31.35C)
INDUCED OCR
1.0
RVG MIN q
(kPa)
-28.6
(kPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) REMOLDED SURF TEST NO. D192
SIGlc'CkPa) 98.5SIG3c'(kPa) 98.5INDUCED OCR 1.0
STRTIC qf (kPa) 108.0 |RVG MRX q (kPa) 39.6 (39.6%)RVG MIN q (kPa) -38.0 (38.0%)
176
0
M-8
CE
-12
o:
ui
a.-is 88
M r CE a
20
I.JJI
I |T
T~
i t
| ill
I (
tf a. a:
u
a.
80
60
40 20
vs LJ
IE-0
1i
12
CY
CL
E *
1620
i 12
C
YC
LE
*
CRUISE ST HELENS
CORE NO.
SL4
INCREMENT (cm)
TEST NO.
REMOLDED SURF
D192
SIGlc'(kPa)
98.5
SIG3c'CkPa>
98.5
INDUCED OCR
1.0
STRTIC qf (k
Pa)
100.0
RVG MRX q
(kP»)
39.6 (39.65O
RVG MIN q
(kPa)
-38.0 (38.05O
16
x (kPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED SURF D196
SIGic'CkPa) 37.3SIG3c'CkPa) 97.3INDUCED OCR 1.8
STRTIC qf CkPa) 188.8RVG MRX q CkPa) 32.9 C32.9*)RVG MIN q CkPa) -31.8 C31.8SO
178
-4
5-8 I o:
u
a.-t
e 20
^
15
Z (T Q
LI a: u tL
80 60 40 20
CYCLE
iea
12
CY
CLE
*
16
CRUISE ST HELENS
CORE NO.
SL4
INCREMENT (c
m)
REMOLDED SURF
SIGlc'CkPa)
97.3
SIG3c'(kPa)
97.3
INDUCED OCR
1.0
STRTIC q-
f (kPa)
RVG MRX q
(kPa)
RVG MIN q
(kPa)
10
0.0
32
.9
(32.9
5O
-31
.8
(31
.8*/
O
see-
p' (kPa)
CRUISE ST HELENS CORE NO. SL4
INCREMENT (cm) TEST NO.
REMOLDED SIJRF D133
SIGlc'CkPa) 275.4 STRTIC qf (kPa) 288.0SIGSc'CkPa) 275.4 RVG MflX q CkPa) 132.S (47.4^)INDUCED OCR 1.0 RVG MIN q (kPa) -107.6 (38.45O
180
oo
0
ec
a 01-1
2a:
u a.
-16 16
0
/^ w
120
Z M r
a0oc a
40
I I
I I
I I
I I
I" I
I ->
»-4
l
l l
I |
I t
l
4 6
CY
CL
E *
CR
UIS
E
ST
H
ELE
NS
C
OR
E
NO
. S
L4
160
a. 12
0
u
a40 0 -40
1E+
04 g
-
IE-0
1
4-i
-l-f
-4-1
<
«
--I-
i
I I/
I I
I I
I I
10
4 6
CY
CL
E
#
INCREMENT (cm)
TEST NO.
REMOLDED SURF
D193
SIGic'(kPa)
275.4
SIG3c'(kPa>
275.4
INDUCED OCR
1.8
STfl
TIC
qf (kPa)
^80.0
jRVG MRX q
(kPa)
132.
6 (47.4%)
flVG
MIN q
(kPa
) -107.6 (38.45O