A METHOD TO PREDICT PARTIALLY DRAINED DEFORMATIONS FOR CONDITIONS IN BRACED EXCAVATIONS by Theodore B.S. von Rosenvinge Eng. Northeastern IV University (1978) Submitted in part ial of the requirements fulfillment for the degree of Master of Science at Massachusetts the Institute of Technology (August 1980) Q Theodore von Rosenvinge IV Signature of Author Department Certified of Civil Engineering, August 14, 1980 by Thesis Supervisor Accepted by Chairman, Departmental Students of Committee on Graduate the Department of MASSACHUSETTS INSTIIUT: OF TECH ,VOG, OC T 9 1980 Civil Engineering. 2 A METHOD TO PREDICT DEFORMATONS FOR PARTIALLY DRAINED CONDITIONS IN BRACED EXCAVATIONS by Theodore von Rosenvinge IV Submitted to the Department of Civil Engineering on August 14, 1980 in partial fulfillment of the requirements for the degree of Master of Science in Civil Engineering ABSTRACT The purpose of this thesis is to develop a method to predict deformations in braced excavations, which includes The time the effects of excess pore pressure dissipation. variables considered are time for construction compared with time required for pore pressure equilization due to altered The method will apply the Stress flow conditions and shear. Path Method to determine appropriate soil parameters to use in the existing finite element program, BRACE III in a way that accounts for time effects. The method will be applied to an actual case to demonstrate its applicability and illustrate its use. Thesis Supervisor: Title: Dr. William Allen Research Associate Marr 3 To M.E. and Marta 4 ACKNOWLEDGMENTS The his author interest author is and also providing is grateful to Dr. guidance during grateful William Allen Marr the to Professor information and soil work on T.W. specimens this for thesis. The Lambe for his support, tested for the case study. The author also wishes and discussion provided ern University Special Marta for hours on during thanks humor was tion while her and of thanks father to my encouragement to stages my wife, during my processor are sustaining note Walter E. early due their patience the word acknowledge by Dr. the is to during the this M.E., education. gratefully was working on his family last for generous Jaworski of supplied by Marta's entire the of advice Northeast- thesis. and young M.E.'s daughter, tireless acknowledged. often welcome "thethiss". their continued several years. The distracAnd a support 5 TABLE OF CONTENTS Page TITLE PAGE 1 ABSTRACT 2 DEDICATION 3 ACKNOWLEDGEMENTS 4 TABLE OF 5 CONTENTS 9 LIST OF TABLES LIST OF FIGURES CHAPTER ONE 10 INTRODUCTION 1.0 INTRODUCTION 14 1.1 THESIS OBJECTIVE 19 1.2 THESIS SCOPE 19 CHAPTER TWO THE ROLE OF TIME 2.0 INTRODUCTION 21 2.1 STRESS PATHS 21 2.1.1 Undrained 2.1.2 Dissipation of 21 Shear Pore Pressure Following Shear 2.1.3 2.2 THE Stress 22 Paths PERFORMANCE OF - 25 Summary VS. TIME 25 Cohesionless Sand 25 BRACED EXCAVATIONS 2.2.1 Braced Excavations 2.2.2 Piping, Suffosion 2.2.3 Effects 2.2.4 Braced of Frost 26 Action Excavations Consolidated Clay in In 26 Normally 27 6 Page 2.2.5 Braced Excavations in Overconsolidated Clay 30 2.2.6 Braced Excavation in Stiff Fissured Clay 32 2.2.7 Braced Excavation in Silt 35 36 2.3 METHODS OF ANALYSIS AND DESIGN 37 Empirical Methods 2.3.1 Semi - 2.3.2 Finite Element Analysis 2.3.3 The Stress 41 45 Path Method 46 2.4 CONCLUSIONS CHAP TER THREE PROPOSED IN THE PRECEDURE PREDICTION FOR INCORPORATING TIME OF THE PERFORMANCE OF A BRACED EXCAVATION 3.0 INTRODUCTION 75 3.1 OUTLINE OF THE PROPOSED METHOD 76 CHAP TER FOUR CASE STUDY - PREDICTION OF THE PERFORMANCE OF A BRACED EXCAVATION 4.0 INTRODUCTION 84 4.1 TYPE OF PREDICTION 85 4.2 PROJECT DESCRIPTION 85 4.3 4.4 4.2.1 General 85 4.2.2 Construction Schedule 86 SUBSURFACE CONDITIONS 86 4.3.1 Soil 86 4.3.2 Groundwater Conditions 87 NAKAGAWA PREDICTION 4.4.1 Initial Model of Field 87 Situation 87 7 Page 4.4.2 Stress Paths III from Initial BRACE 87 Analysis 4.4.3 Laboratory Tests and Revised Soil 89 Profile 4.4.4 A. Soil Classification 89 B. Stress Path Tests 90 C. Coefficient of Consolidation 91 D. Revised Soil E. Contours of Equal Vertical Revised BRACE 91 Profile III Analysis Strain for Partially 95 Drained Conditions 95 A. General B. Computation of Partially Drained 96 Moduli Undrained 2. Consolidation Strains Dissipation of Excess 3. 96 Shear Strains 1. Within 95 Due to Pore Pressure 97 the Excavation Consolidation Strains Due to Dissipation of Excess Pore Pressure Behind C. 98 the Excavation 100 of Moduli 4. Contours 5. Ko 102 6. Anisotropy 102 Predicted Loads, Stab i 1ity Deformations and 103 8 Page 1. General 103 2. Deformations 103 3. Loads 106 4. Stability 107 SUMMARY AND CONCLUSIONS CHAPTER FIVE 5.0 GENERAL 152 5.1 LIMITATIONS 153 5.2 SUGGESTIONSFORFURTHERRESEARCH 154 5.3 CONCLUSIONS 156 LIST OF SYMBOLS 161 REFERENCES 163 APPENDIX A GRAINSIZE PLOTS AND SQUARE ROOT CONSOLIDATION PLOTS - OF TIME NAKAGAWA SOIL 167 SPECIMENS APPENDIX B VERTICAL NAKAGAWA EFFECTIVE STRESS VERSUS DEPTH- 182 9 LIST OF TABLES Table No. Page Title 81 3.1 GEOTECHNICAL 3.2 STRESS 4.1 SOIL INDEX PROPERTIES, 4.2 SUMMARY OF COEFFICIENT OF CONSOLIDATION DATA FROM STRESS PATH TESTS PATH PERFORMANCE 82 METHOD AND CLASSIFICATION 4.3 SUMMARY 4.4 SUMMARY OF DETERMINATION OF PARTIALLY DRAINED STRESS STRAIN MODULI 4.5 OF SHEAR STRENGTH DATA SUMMARY OF STRENGTHS FOR AVERAGE IN STABILITY ANALYSIS 115 121 124 129 ELEMENTS 151 10 LIST OF FIGURES 1.1 Page Title Figure No. EFFECT OF FORCED DELAY ON A CRITICAL CONSTRUCTION EVENT 48 BRACED EXCAVATION GEOMETRY 2.1.1 EXAMPLE 2.1.2 STRESS PATHS FOR UNDRAINED UNLOADING NORMALLY AND OVER CONSOLIDATED SOIL ELEMENTS 2.1.3a 2.1.3b 2.1.3c 2.1.3d 2.1.4 2.1.5 2.2.1 2.2.2 2.2.3 20 OF 49 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR NORMALLY CONSOLIDATED SOIL-NO DEWATERING 50 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR NORMALLY CONSOLIDATED SOIL-WITH DEWATERING 51 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR OVER CONSOLIDATED SOIL-NO DEWATERING 52 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR OVERCONSOLIDATED SOIL-WITH DEWATERING 53 DETERMINATION OF TOTAL HEAD SUBJECT TO EXCAVATION AND/OR DEWATERING 54 STRESS PATHS FOR ACTIVE AND PASSIVE CONDITIONS FOR NORMALLY AND OVERCONSOLIDATED SOIL 55 STRESS PATHS FOR EXCAVATION IN COHESIONLESS SAND 56 PIPING/SUFFOSION MECHANISMS 57 INCREASE STRUT LOAD VS. IN TIME FOR A BRACED CUT IN STIFF FISSURED CLAY COEFFICIENT OF CONSOLIDATION 2.2.4 VARIATION IN 2.2.5 SOIL PROFILE, EXCAVATION, AND INSTRUMENTATION DETAILS WALL IN SOFT CLAY, OSLO 2.2.6 SUMMARY OF SOFT CLAY, 58 FOR A BRACED OBSERVATIONS FOR BRACED OSLO 59 SLURRY 60 CUT IN 61 11 Page 2.2.7 2.2.8 2.2.9 2.2.10 2.2.11 2.2.12 2.2.13 2.2.14 STRESS DATA FOR PIEZOMETER P-i, CAES FOUNDATION EXCAVATION BELOW THE 62 SOUTH COVE SUBWAY EXCAVATION TEST SECTION PIEZOMETER P-4 63 STRUT LOAD AND PORE WATER PRESSURE VS. -SOUTH COVE TEST SECTION 64 TIME MEASURED AND PREDICTED STEADY STATE PORE PRESSURES-SOUTH COVE TEST SECTION 65 TIME DEPENDENT BEHAVIOR OF TEST CUT IN STIFF FISSURED CLAY 66 EFFECT OF VARIATION OF TIME TO FAILURE ON STRENGTH IN UNDRAINED TRIAXIAL TESTS 67 EXCAVATION PENETRATING SILT: SECTIONS A & B 68 MBTA TEST MEASURED AND PREDICTED PORE PRESSURE MBTA TEST SECTIONS A AND B 69 2.3.la TERZAGHI & PECK DESIGN ENVELOPES 70 2.3.1b TERZAGHI & PECK DESIGN ENVELOPES 71 2.3.2 CONSOLIDATION AT THE END OF ONE-DIMENSIONAL 72 EXCAVATION 2.3.3a CONTOURS OF NEGATIVE EXCESS PORE PRESSURE FOR TWO-DIMENSIONAL EXCAVATION 73 CONTOURS OF NEGATIVE EXCESS PORE FOR TWO-DIMENSIONAL EXCAVATION 74 2.3.3b PRESSURE CONTOURS OF EQUAL VERTICAL 4.2.1 PLAN VIEW AND PROFILE OF NAKAGAWA SEWAGE TREATMENT PLANT EXCAVATION - SITE B 110 4.2.2 SITE B CONSTRUCTION SCHEDULE 111 4.4.1 INITIAL PROFILE AND FINITE ELEMENT MESH 112 4.4.2 DETAIL OF FINITE ELEMENT MESH IN ZONE OF EXCAVATION 113 4.4.3 STRAIN 83 3.1 TYPICAL TOTAL STRESS PATHS INITIAL BRACE III 114 ANALYSIS LINEARLY ELASTIC MODULUS 12 Page 116 4.4.4 PLASTICITY CHART 4.4. 5a STRESS 4.4. 5b STRESS PATH 4.4. 5c STRESS PATH TEST TE-1 119 4.4. 5d STRESS PATH TEST TE-2 120 4.4.6 REVISED 122 4.4.7 UNDRAINED STRENGTH TRIAXIAL TEST RESULTS VERSUS SAMPLE DEPTH 4.4. 8a PATH TEST 117 TC-1 TEST TC-2 118 SOIL PROFILE 123 ESTIMATED CONTOURS OF EQUAL STRAIN 125 COMPRESSION 4.4 .8b 4.4. 8c ESTIMATED CONTOURS COMPRESSION OF EQUAL ESTIMATED CONTOURS EXTENSION OF EQUAL 126 127 SIXTH 4.4.10 SUPERPOSITION OF TOTAL STRESS CONTOUR PLOT OF EQUAL STRAIN STAGE 4.4.11 DEPTH OF EXCAVATION 4.4. 12a TIME FACTOR VS. - STRAIN 4.4.9 EXCAVATION - STRAIN SIMPLIFIED VS. AVERAGE PROFILE PATHS ON 131 TIME DEGREE 128 132 OF CONSOLIDATION 133 4.4. 12b NORMALIZED 4.4.13 NORMALIZED DEPTH VS. CONSOLIDATION RATIO FOR TRIANGULAR INITIAL EXCESS PORE PRESSURE 134 4.4. 14a VOLUMETRIC PRESSURE 4.4. 14b 4.4.15 4.4.16 4.4.17 DEPDTH VS. STRAIN VS DISSIPATION OF 133 PORE 135 VOLUMETRIC STRAIN VS. OF PORE PRESSURE CONTOURS OF MODULI REVISED RUN B - CONTOURS OF MODULI FINAL RUN C - DEFORMED FINITE CONSOLIDATION RATIO LOGARITHMIC DISSIPATION 1 36 BRACE III ANALYSIS - 137 BRACE ELEMENT III ANALYSIS - 138 MESH 139 13 Page 140 4.4.18 SELECTED LINES OF LATERAL DISPLACEMENT 4.4.19 SELECTED LINES OF VERTICAL HEAVE 141 4.4.20 CONTOURS OF SHEAR STRESS 142 4.4.21 CONTOURS OF TOTAL SIGMA Z 143 4.4.22 CONTOURS OF TOTAL SIGMA X 144 4.4.23 CONTOURS SHOWING TRENDS OF NEGATIVE EXCESS PORE PRESSURE 4.4.24 4.4.25 COMPARISON BEHIND THE 145 OF PECK'S CHART WITH NAKAGAWA EXCAVATION ESTIMATED TOTAL STRESS THE STEEL PILE WALL SETTLEMENT DISTRIBUTION TERZAGHI 4.4.27 SIXTH EXCAVATION ANALYSIS STAGE 4.4.28 STRESS STABILITY ANALYSIS 5.1 LINEAR VS. NON 5.2 HYPERBOLIC STRESS A. 1-A. 6 COMBINED A.7-A. 14 SQUARE B.1 PATHS FOR ANALYSIS - 148 STABILITY 149 LINEAR STRESS STRAIN STRAIN CURVES GRAINSIZE ANALYSIS PLOTS ROOT OF TIME CONSOLIDATION PLOTS VERTICAL EFFECTIVE NAKAGAWA BEHIND 147 4.4.26 BASAL HEAVE 146 STRESS VS. 150 159 160 168 174 DEPTH, 183 14 CHAPTER ONE INTRODUCTION INTRODUCTION 1.0 and in dissipation, to highly influenced by the Presently or excavation "drained" pressure pore or constructing "deep" safety, adjacent effect the usual the and on major potential response the for can be facilities time of approach practice "unloading" to is use parameters of engineers and case excavations For conditions. deformation the excess time of role of mass. soil common and excavation the damage the and designing Design economy, excavations. the of the role specifically the consider carefully should engineer An "undrained" in "undrained" or the most clay and strength This design. for assume idealize to is approach assumes following: (1) Construction occurs (2) No dissipation excess of during construction The (3) soil rapidly. is strength pore pressure occurs no drainage occurs). (i.e., the in-situ shear undrained strength. The assumptions "instantaneous" soils are not above are applicable excavation. "instantaneous" Actual and only for excavations are partially in an cohesive drained. 15 Although for some situations (i.e. excavation in soil with a very undrained assumption is rapid temporary low permeability) the nearly valid at least for design purposes, many major braced excavations are open for months or even years. Significant pore pressure dissipation following shear stressing of the soil or altered may facilitate rapid drainage. and significant increases occur as well a consequence unpredicted in soil strength may in the stress/strain the soil with time. Although relatively few studies of excavations have been made the As or decreases as variation characteristics of of pervious soil Undetected layers conditions may occur. flow to observe performance of braced cuts, some instrumented the effect of time on significant To briefly summarize several observations have been made. cases: (1) Bjerrum & DiBiagio experimental 4 meter clay instrumented influence of the average struts for deep trench in stiff-fissured the purpose of studying the They observed force per meter as measured in increase from 2.3 Measurements reported on an time on earth pressure. tons/meter over (2) (1956) tons/meter several months to 7.17 (Sept. from a braced slurry wall Boston Blue Clay reported by Jaworski indicate a gradual and significant the to Dec.). in stiff (1973) increase in 16 earth pressure after excavation to the design depth. (3) DiBiagio & Roti (1972) reported earth and pore for a braced slurry wall pressure measurements Significant decreases and excavation in soft clay. in earth and increases after pore pressures during and completion of excavation to the final depth were observed. (4) Lambe reported piezometer (1968) excavation 22 data for an feet deep penetrating an overconsolidated medium Boston Blue Clay. Negative excess pore pressures in the clay at the bottom of the excavation decreased during the 24 day This period the cut was open. decrease in the strength of the indicated an overall soil as well as a safety with time. decreasing factor of The above observations reflect fact the that time is an important variable to be recognized by the engineer. Recently Clough & Osaimi (1979) investigated pore for excavations, pressure dissipation including braced excavations using a finite element model to determine how long the undrained case was applicable. From the results the authors concluded excavation in clay is that pore pressure dissipation likely to occur than previously believed and that should be used with care. to a greater for degree the undrained assumption 17 Determining pressure occurs difficult to other The several (1) the for a task. For phenomena engineer rate design sands such of The to (3) to system can be a be a complex factor with transport (piping). to the assess and respect importance of and is total to be time in for which service (i.e. the permanent). of altered imposition groundwater of new groundwater control. The in changes cut pore design: excavation character the soil attempt support dissipation of time may as prior temporary or (2) to which given braced should variables The degree total boundary stress conditions conditions distribution due and due to excavation. (4) The on (5) effect the The for such Critical such a and after delays. final phase and and strikes excavation delay-(i.e. hence may stage for and parameters. labor etc). estimated conditions unforseen extend performance. as placing can be (1977) (just prior slab) at a major strikes accurately unexpectably such & Davidson caps be influence events dissipation deformation contractor of construction pile pressure time may an excavation Clough and forced excavation backfilling foundation of labor time pore strength weather as construction bracing excess construction reasonable events soil effect Although of most report to the office support or influenced one case casting bottom of a building, was by where 18 adversely affected by an unexpected delay. be used to support raker bracing for the sheet pile wall. carpenter strike delayed pile cap formwork during which the excavation stayed The slab was to open and for six days the walls inward. After 20 centimeters remedial support was applied by pile cap excavation to retard further movement. over 30 centimeters crack versus time and Corbet, excavation workers strike of concern benefit and Langford Although the for authors apparent this excavation. reported on a braced a national building specific results of state that to the author the this delay are the delay was a cause that the profession would time. The behavior of penetrating intermediate soils types such as are of particular engineer 1.1 shows movement for (1974) large from additional research and measurements of excavations etc. Figure A the stability of the excavation. excavation performance vs. and sand occurred. Eventually led to delay of a critical period in not reported, the is the wall. in stiff London Clay where excavation. It temporary filling of the the pertinent events Davies crept of movement had occurred some of wall movement appeared behind A silts, clayey silts interest. between the clay and clayey sands The demand for the to design with economy and safety warrant understanding of the role of soil subject a better time and drainage on behavior of to excavation unloading. 19 1.1 THESIS OBJECTIVE The apply objective of time several simple over time discussed. will to predict be the to formulate effects deformations discussion of cases, for the Several discussed. of of A and pore pressure an excavation. method will in the lab braced and to predict for a excavations design and type include stress the excavation. A path role of of time for of measurements will be analysis Stress Path Method study. element analysis, effect significance current applied This the several braced outlined and deep the is THESIS SCOPE Following made thesis a method which includes change with 1.2 this approaches approach will prediction of a a composite of finite testing time of in the soil be case specimens study of a Strike 30- Elevation Om 25: 5 1_3 . 3 2 0. w 202 Li 0 DAY 6 Poured Pile Caps0 Pile Caps Partially Filled With Soil -J 10 Elevation Om o East Sheetpile Wall 3 West Sheetpile Wall 5. 5Excavation of Pile Caps(-Ilm) DAY.3 0- Excavation to Subgrade (-9.5m) 0' ' ' ' 5 ' ' ' ' 'O ' ' ' '2 ' ' ' ' ' ELAPSED TIME SINCE START OF EXCAVATION (DAYS) EFFECT OF FORCED DELAY 115 DAY 7-14 FrOM CLOt&-CL" ON -A CRITICAL CONSTRUCTION E VENT j CA'IDSON (9-17) FIG. 1.1 21 CHAPTER TWO THE ROLE OF TIME INTRODUCTION 2.0 this chapter the effect In outline the importance of excess pore pressure dissipation Related observations and excavations. for braced of pressure and time measurements be simple examples will be discussed to several deformation for of time on strength and discussed. from the Various current methods of analysis and design will be reviewed on the basis incorporate time for of how the methods Limitations and assumptions made effects. each method are discussed. 2.1 STRESS PATHS Use of stress 1967, paths and Lambe & Marr 1979) within which for literature will the Stress Path Method (Lambe provides an organized framework Stress paths the field problem can be studied. field situations can be modeled using standard tests, laboratory such as the three dimensional triaxial test. 2.1.1 Undrained Shear At this and 2.1.2 point convenient to refer constructed by the writer. are an example of effective stress clay soil it is to Figures Shown in the braced excavation geometry and paths 2.1.1 figures total and for normally and overconsolidated elements adjacent to the excavation. 22 The total between 2A and 2B represent the experienced by soil elements stress the wall stress type of unloading typically 1 and 2. change for element 2 at excavation is 1A and 1B and stress paths between points The mode of total the center extension unloading. line of the Soil element 1 behind experiences compression unloading or an "active" condition. Typical effective can be stress paths for 1A and 1C and points 2A and 2C traced between points on each p-q plot. The horizontal at any given value of q is the undrained shear width of the shaded area the value of excess pore pressure generated by shear. The which shaded region also represents the effective stress conditions. effective a material drained 2.1.2 There for partially drained in silt this region. Rapid excavation in for example, may exhibit partially behavior. Dissipation Of Pore Strength and Pressure Following stress-strain modulus of the dependent on the pore lie are an infinite number of possible stress paths such as paths the region within effective stress path. are soil parameters Figure important in the soil are Since changes pressure directly affect the effective these changes Shear in stress path, field and when estimating for design. 2.1.3a-d shows geometry of Figure 2.1.1 stress for paths for the example typical overconsolidated and 23 The plots normally consolidated clays. exhibit in the figure type of pore a range of situations bracketing the to occur during and after pressure behavior likely to the design depth. excavation made in order shear due to plots; undrained to draw these occurs excavation A simplifying assumption is first and then is followed by dissipation of excess pore pressure. pore pressure results Excess release due to excavation and/or from decrease in pore pressure due to altered flow conditions (i.e. dewatering). With respect to dissipation pressures following qualitative after the construction of 2.1.3a--This strength of excess Clay soil will (i.e. move towards the failure envelope) pore pressure positive excess result in occurs at element the to dissipation of pore pressure caused by dewatering settlement. The soil will experience an increase in strength with consolidation. vertical to Consolidation heave will occur. 2.1.3b-- Consolidation due will This the bottom of the excavation and behind excavation wall. in undergo a minor decrease the original pore water pressure. (2) pore conclusions can be made following dissipation of excess both construction the Figure 2.1.3 plots: Normally Consolidated (1) total stress from the strain will Net be higher with dewatering for 1 due to additional compressive strains at 24 constant shear stress. strain for element However the net vertical 2 will be less associated with no dewatering. steady state If two strain dimensional flow conditions are attained steady-state pore pressure the can be determined from a flow net. Although steady state flow conditions will be reached, this condition represents (3) than the 2.1.3c--For to an outside bound. an increasing over consolidation ratio the effective stress due it may be unlikely that full path will shift to the right the generation of large negative excess pore pressures. result Subsequent consolidation will in a substantial decrease in strength and a consolidation heave. (4) 2.1.3d--If the absolute value of change pressure due to to or altered in pore flow conditions is greater than the absolute value of pore pressure due increase. to shear, Otherwise the equal the excess the strength will strength will decrease with time. For a given excavation with excess pore generated by shear pressures and dewatering the net excess pore pressure can be estimated by super-imposing or adding two. this. Lambe (1968) discusses schematically illustrates the field situation. the Figure 2.1.4 procedure for simplifying the 2.1.3 Stress The use 25 Paths---Summary of stress paths to illustrate the various possibilities assists the engineer in his judgement. Qualitatively the pore pressure-strength-strain relation clarified stress in one's mind. paths pressures to (1970) illustrate active and passive for excavation overconsolidated clays. plots Similarily Henkel earth For comparison, several paths. recognizes the utility in type applying this of Henkel's a slightly different graphical portrayal of stress Henkel of approach may behave. THE PERFORMANCE OF BRACED EXCAVATIONS VS. Cohesive soils TIME are assigned low permeabilities compared to cohesionless soils which have high permeabilities. general for projects changes as the engineer in his understanding of how a given excavation 2.2 uses in normally and highly are reproduced in Figure 2.1.5 showing an aid to is the time associated involving in with most construction loading or unloading of the flow conditions, in cohesive soils. some degree For sands In soil or of drainage occurs the condition of full drainage is achieved rapidly. 2.2.1 Braced Excavations For excavations In Cohesionless in sand deposits steady-state seepage conditions are achieved rapidly. paths illustrating Sand Figure 2.2.1 shows stress this behavior. Since sand has a relatively high permeability pore pressure dissipation is virtually instantaneous. The total stress path equals the 26 stress path and the effective Therefore time does not play a be obtained from a flow net. Although the following two sections are significant role. not to 2.2.2 particles via high seepage gradients into Figure 2.2.2 graphically for excavation. Peck (1969) resulting from migration of sand into the ineffective. and render them anticipated by field montoring of of the excavation Also at presence of suspended The mechanics of this (1942) and D'Appolonia Effects of (pump the bottom of the excavation piping were elucidated by Terzaghi 2.2.3 flow into and out for the failure by heave may occur. (1967) through cracks or conditions can be Serious a sheet pile wall. & Peck cut. time migration of silt size particles can Particles can also be piped soil particles. points control may lead to damaging clog construction dewatering wells effluent) the the mechanisms illustrates suffosion and/or piping. Over a period of holes in time piping or suffosion. to as inadequate groundwater settlements are present, to migration or erosion of soil is referred This migration responsible time plays in the cohesive soil). (vs. gravels, silts and sands or a role with respect out that soil they serve Suffosion Piping, Where plays the different type of role in cohesionless excavation objective, thesis the specifically bound to illustrate steady state pore pressure can phenomena and discussed by Terzaghi (1971). Frost Action Field observations have shown the effect of frost action 27 to be substantial. struts may increase Several cases show the several fold. monitored performance 1 Pappas & Sevsmith of a deep braced cofferdam in sensitive Leda clay. Abnormally load were detected loads in the large increases in strut during December excavation. heating of the adjacent soil resulted in rapid reduction, the problem was concluded Since load to be one of frost act ion. DiBiagio & Bjerrum within in and at load in lower observed after the surface of an excavation the upermost struts, and severe bracing struts. (1956) levels buckling some trench, decreases increases in the of the walers and Although reliable deformation measurements were not available, visual observations led to the conclusion upward expansion of the soil during freezing unusual shows ground freezing changes the caused the in distribution of pressure. dramatic time vs. Terzaghi & Peck (1967) that an Figure 2.2.3 strut load behavior. report that braced cuts in Oslo & Chicago were subjected to below freezing weather. They observed earth greater pressures climb to magnitudes several than those prior Ground freezing as to freezing. these cases unpredictable and radical behavior. frost lenses is times time dependent, the illustrate Since the can result in formation of potential for damage can be anticipated by monitoring the wall movements and strut loads. IRefer ------------------------------------------------------------to Clough and Davidson (1977) 2.2.4 28 In Normally Consolidated Clay Braced Excavations For clays one expects a soft normally consolidated clay to have a lower coefficient of consolidation than an overconsolidated clay since this value be higher shown in recompression than in Figure 2.2.4 rate. At least generally found to in primary consolidation as for a varved clay. expect soft clay to dissipate excess slower is We would therefore pore pressures at a one braced excavation case illustrates that normally consolidated clay the ideal undrained condition is not sustained over the course of time excavation. DiBiagio and Roti for a temporary (1972) measured the magnitude of total earth pressure, deformations of a braced slurry-trench wall in Oslo. Below the clay the wall was bedrock. Measurements were made before,during and after excavation. Figure 2.2.5 geometry of the excavation layout. pore pressure and shows the as well a soft the profile and instrumentation pressure two piezometers. The measurements during the excavation stages Figure 2.2.6 indicate only minor decreases in occured until groundwater shown in pore pressure the excavation approached bedrock and control was facilitated Consequently, the pore pressure at was through this layer. the bottom of the clay significantly reduced, accompanied by a marked in total clay keyed into a pervious soil as in Instrumentation included fifteen earth cells and for earth pressure on the wall. remained open to reduction The excavation this depth for approximately 200 days. A 29 downward gradient in the settlements during this period before excavation bottom with pore earth the course of total its increasing in pore pressures. For the fact location of the that the upward towards the center concludes that this specific zone correct as decrease Coupled with the force moved layer with time, central point of the this soft clay As a practical matter, the undrained assumption may looking at the careful study, center of the clay resultant earth of the behaved partially drained. not total a small decrease in pore the time of construction. is the initial value. pressure over However, The the construction of this excavation piezometer PZ-9 shows writer slab. earth pressure varied dramatically due primarily to changes layer, towards of the from this point on the rate of settlement and pressure back Over the "sealing" the construction of a base pressure built up steadily decreasing the clay contributed to consolidation clay mass as this be reasonable. a whole piezometer PZ-8 clearly in the assumption shows. the writer concludes that because After the in pore pressure in PZ-9 occurred before dewatering and remained relatively constant, dewatering did not significantly affect the center of the clay and the negative increment of pore pressure was due solely to changes total stress. layer shows changes in Conversely the lower portion of the the effect of both changes flow conditions. in total in clay stress and 30 is Although admittedly this that illustrates pore pressure dissipation can be a factor even for impervious walls Dissipation of soft clay. in positive excess pore pressures resulting large pressure decreases against lead to construction. from dewatering can the wall during More rapid dissipation of excess can be expected pressures it only one case, pore for sheet pile and other non-slurry-trench walls which are characteristically more permeable. 2.2.5 Braced Excavation In Overconsolidated Clay interesting conclusions Some undrained from field data suggest the assumption to be seriously in error for the overconsolidated clay. Referring now to Figure piezometer readings 2.2.7, Lambe Very litle the after excavation. a value Thereafter of negative excess path towards follows The P-1 are reproduced the pore pressure increased less than u. porewater pressure). pore pressure moves failure and results as Lambe concludes 24 days. in the pore pressure immediately greater than u. but still pre-excavation static It is for in this excavation. for a point at piezometer Note that u. , figure. the CAES building The excavation was open dewatering was attempted stress paths observed from the medium clay layer at the bottom of a temporary braced excavation for foundation at MIT. (1968) (the The dissipation the effective stress in a consolidation heave. that there is to a progressive decrease in strength leading to a decreasing factor of 31 time. safety with is Therefore the end of the unloading period the most critical the unloading period replaced in is defined just before as Hence, the excavation. The end of this excavation. time for load is the the most critical condition occurs some time after completion of the excavation. Observations slurry-trench and sheet Figure pore deformations and strut 2.2.9 shows a redrawn pressure versus slurry wall. in stiff clay pile walls subway excavation in Boston (see pressures, for braced and measurements were made Observations loads were measured. compilation of strut load and section at of piezometers behind the wall feet decreasing to 82 the wall after in the feet measured loads strut pressure measured figure. total (less increased Following mud steadily as did in the piezometer than 1 inch) resulting from construction. joints was observed. measured pore pressure vs. predictions 106 in piezometer P-4 behind P-4 as the change water pressure can be associated with altered wall panel of shown Since measurements showed very little outward wall movement conditions in water head the final cut had been made. slab placement, axial pore water from an initial the indicate excavation was accompanied by steady decreases pressure Pore Figure 2.2.8). for a test cross time for a in pore flow Seepage through Figure 2.2.10 shows depth. Steady state seepage compared well with end of construction pore pressure measurements. Hence, it can be argued that the 32 drained parameters,C and are more applicable for this "end of construction" case. In constrast to Oslo, the slurry wall pore pressures significantly. throughout case in the soft the stiff clay drop Imposition of new boundary water pressure conditions are met with a relatively quick drainage. the strut reflect over loads at the strut the life structure. in strut DiBiagio (1956) loads for trench studied. gradual during excavation in Figure 2.2.11 load shows a section of profile and (Sept. test data. to mid Nov.) show a winter load (see to the also Figure 2.2.3). total intense period of rainfall is followed by pressure observed for Autumn Pore pressures pore pressure versus plotted in Figure 2.2.11 time over this clay facilitate access Autumn earth pressure show increases following periods of rainfall. value of pore the type of soil frost action and previously section 2.2.3 rainfall data compared most this and marked increase followed by enormous discussed in figure in stiff marine clay Bjerrum & the Autumn increases attributed to sharp in the Stiff Fissured Clay the excavation, corresponding soil Strut trend are seen in adjacent struts. interesting case the experimental The load by a factor of approximately Braced Excavation In One is loads which the bracing will experience Similar trends 2.2.6 Also the end of excavation do not accurately of the shows an increase 1.5. clay in the maximum in mid November. show the measured period. of water to The The fissures in the clay mass. Total 33 release from excavation in fissured and weathered stress clays lead to can further opening of the permeability. increases in conditions leads such Prolonged construction under progressive weakening or softening, increases in the as as well to fissures and in pore pressure. rapid changes dramatically The effect of fissuring on stability is illustrated by the short term slip failure of an unsupported excavation in London Clay reported by Skempton and LaRochelle (1965). The results The strengths measured of the average tests. from triaxial triaxial tests and the actual pressure migration within the It was fissuring. the for Conventional tests to in failure to intact clay, tests, and run at a pore (2) time to strength decreased. failure of 15 minutes time to the strain rate due of strain rate on strength strength versus tests (1) strain rates much higher than and pressure migration. triaxial The authors shown that by increasing the triaxial unrepresentative of influence undrained the difference between the measured strengths attributed correspond the estimated mobilized shear strength in approximately 55% clay mass was failure fissured clay as in stiff slip occurred shortly after excavation had been The completed. the lend of this study understanding to braced excavation well. to soil succeptibility of the Figure time to 2.2.12 failure performed to to excavation. is attributed shows to pore the results for a series This of of undrained study this behavior. Secondly, 34 the authors the fissuring can weaken the clay during excavation. Several conclude that at of the least five important factors are, along fissures leading to increases factors related to absorption of water in water (softening), reduction of strength to zero as content fissures open, and progressive failure. Quantifying the effect of fissures and the rate of softening on stability and deformation to predict is difficult. performance Corbet et al (1974), observations made for and Cole and Burland both reported a raker braced diaphragm wall meter deep excavation for a basement London Clay. In view of in in a 20 stiff fissured the uncertainties cited in the previous paragraph, detailed construction performance monitoring was undertaken. were monitored. Several of Wall movement and verticality Earth pressure however, was not monitored. the conclusions drawn by the authors after observing the construction performance are reiterated below. (1) Wall movements showed a clear (2) Early internal time dependence. support placement is essential to minimize movements. (3) Performance monitoring control is important for and is of research value for construction future exca- vat ions. (4) Inward wall movement progressive of the clay. is associated with a softening and reduction in The greatest stiffness reduction in stiff- 35 ness was found to be near the wall. This is attributed fissures due to lateral In summary, one significant factor excavation to the opening of stress can clearly see release. that time fissured clay. and measurements Although conclusions of practical value at undrained assumption is not applicable stiff fissured clay which remain open and minimizing construction time Lambe two ic et al, 2.2.13. and MIT (1972) monitored underlain by glacial till The test for sections, with silts No time was measured. the studies was that the pore pected to is desireable. literature. reported on a study of in fill overlying as Section A and Section B were significant strut against load variation However, one conclusion reached for braced excavation pressure behind be less organ- seen in Figure stresses and deformation and compared predicted behavior. in information on excavation instrumented Boston subway cuts silt, The important and is in silt has been reported in the (1969), time. in Silt Very little well documented performance can make for several months, recommended, Excavation are needed to excavations performance monitoring is Braced additional this construction 2.2.7 a very of field situations to advance our understanding of this case we several is for load and deformation behavior of in stiff observations the ground surface behind in sands and the excavation can be ex- than static due to construction. agreement between the final measured pore pressures Some and in 36 steady state pore pressures predicted by analysis (FEDAR, Taylor and Brown pressure in indicates the pore two test sections the upper fill and stiff Therefore general conclusions by soil representative of the lower strata. the writer regarding However the cases be made. in silt cannot penetrate several penetrate silt, truly representative of an excavation in conditions are not to 2.2.14. See Figure these Although excavation element the silt was probably in a transient state near steady state. silt due 1967) finite do fact that many excavations soil types and cannot be are easily categorized. studies are valuable case histories. These illustrate the They type of construction monitoring data which predictions of construction performance can be evaluated from. As a result, our understanding of braced excavations The reader extended. additional details. like BRACE is referred Use of finite to the references can be for computer programs element and FEDAR to model braced excavation and flow respectively showed encouraging predictive capabilities. 2.3 METHODS OF ANALYSIS AND DESIGN The following currently used methods design will be discussed as of time of analysis and they relate to effects. (1) Semi-empirical Methods (2) Numerical Analysis Methods (3) The Stress Path Method the incorporation 37 Semi-empirical Methods 2.3.1 Several well known semi-empirical design methods are Terzaghi and Peck Method (2) Tschebotarioff Method (1973) (3) DM-7 are similar and are strut loads. Peck presented the original apparent envelopes published version. derived from classical earth method is of strut referred reliably measuring the apparent loads to as (1974) is pressure theory and actual Hence in excavations. semiempirical. stresses against stress distribution the Difficulty in sheeting required The envelopes intended to give maximum values of strut experienced and are not load to be truly representative of the adjustments have been made to accomodate newer envelopes of the 2.3.la and for sand is based for braced excavations actual and observations 2.3.1b show the Terzaghi and Peck Method for The pressure envelope load measurements are Over the years modifications and experience. Figures the to be inferred or backfigured from the strut loads. stress distribution. the most The design envelopes were recent measurements in sand or for braced excavations in 1948 Peck, Hansen & Thornburn in clay. will this design approach. discussed to illustrate pressure (1967) Only the Terzaghi and Peck Method Terzaghi and in commonly used to estimate maximum lateral They are intended practice. 1967) (Navdocks) Method (1971) These methods be (1948, (1) the: design sand and clay. in part on strut in New York, 38 An equivalent uniform earth Munich, and Berlin. was fit through the apparent pressures in pressure the excavation. Several qualifications attend the application of this method for sand. The authors emphasize (1) that the diagram has been developed from a limited number of excavations varying in depth The diagram is (2) from 28' to 40'. distribution for a pressure estimating the maximum values of strut expected bottom of the cut. opinion), seepage or assumed to be below the (in Consequently, points for out is (water level Application of the Terzaghi and Peck sands must accompany an awareness of can be should the writer's opinion be added especially since substantial. the incorporated into such the groundwater pressures which may be experienced over the structure below cut) the bottom of problem cannot simply be conditions. Also, in soil behind time related effects have been piping and piping heave at This (1973) seriously in error. to be any pressure envelope. for assumption detrimental associated with excavation. this Ries impervious diaphram type walls typically retard drainage of the likely For sands that the writer's pressures should static water pressure distribution. the wall, method is be added to the which to be for similar cuts. groundwater level The (3) loads life of the these pressures 39 Several relevant the facts one should be aware of when using of the Terzaghi and Peck method are clay envelopes summarized below. (1) Cuts are or undrained condition is assumed Average undrained strength side (2) The)=0 condition assumed to be temporary. is the cut Chicago) from which (Oslo and test cuts from the the data the envelopes evolved included in strut load increases measurements showing large these during cold weather, for formulation of measurements were not used the freezing Therefore the effects of envelopes. the the clay along of used. Although due to freezing to prevail. should be considered separately. (3) The authors (1967) available data on cuts in clays, and clayey sands yet to be worked out. (1969) reports that the However more recently, Peck trapezoidal five cuts in stiff clay could be used that limited drained behavior and appropriate drained strength input clay envelope into an equation for earth pressure stiff the parameters equation for Ka. as a data for at deep cut in dense clayey sand and sandy clay shows sandy design envelopes have etc., conservatively and therefore least one clays, stiff intact fit the measured values of guideline. Peck suggests little due to admit that can be Presumably, the for excavation in sand 40 is then modified (4) Use of to discussed by Peck 1969) in dependent behavior. for stiff the authors (Terzaghi and Peck (1957) This which suggested that maximum design pressure, showed time case has been discussed the writer in earlier sections The authors fissured light of the measurements made by DiBiagio and Bjerrum by expression. the trapezoidal envelope clay is 1967, include this the of this paper. lower value .2WH be used for if movements of the sheeting are minimal and construction time is short. If these conditions of the higher pressure value .4VH is recommended. in an indirect way have assigned some to time In summary, methods provide loads. although of Hence Terzaghi and Peck, fissured strut do not apply, use it importance for stiff clay. is the writer's a useful opinion that these guideline for estimating maximum The method has been to extend effects tempered with experience the scope of the Terzaghi and Peck method more experience for a large variety of cuts The of the method should be realized and may be limitations understood by studying the evolution of its Major braced cuts designed on open for extended periods the basis of this method alone. is required. formulation. should not be The engineer's understanding of the excavation problem may benefit by using other more fundamental techniques. 41 2.3.2 Finite Element Analysis Over recent years the advent of the high speed digital computer has enabled numerical analysis and viable technique for problems . The sets of use equations of sets of equations solving complex engineering the electronic by matrix mathemat icaly model be c omputer algebra problems could in set al lows detail * up Appl ication and theory documented Zienkiew icz 1967, analys is . in the the programs the the engineer to such solution was too Element Method is (Desai and Abel literature over solve 1arge hand. Fini te Bathe and Wilson Subsequently, elem ent computer of to Previously the but complica ted to achieve practically by now well to become a popular 197 6) 1972, for engineering decade several last finite to model construction of braced e xca vations have been developed and used by several inve stigators including Wong (1971), Jaworski (1973) and Clou gh and Duncan (1971). Advantages of using this (1) Complex soil and technique include: structure geometries and properties can be modeled. (2) Construction sequence and details (3) Detailed information on stress can be changes simulat ed. and deformations can be obtained. (4) Parameter studies can reveal of (5) the relative input data (strengths, moduli, and penetration etc.) Critical stages of excavation import ance sheeting stiff ness for a given excavation. can be predicted. 42 limitation lies Nevertheless, even soil in modeling the in the difficulty sheeting interface). soil interaction (i.e., structure One such to be overcome. limitations have yet Some stage of in the relatively young development for finite element modeling of excavation, encouraging results and in practice, and Kenney (1970), and others have demonstrated the powerful the method. applicability of The finite element program developed at MIT for analysis called of excavation is and Jaworski (1971) The program in its present form will model behavior of the The program does modulus. strength, modulus, pressure which include the the effects strain elastic of time on If necessary, dissipation). effect of time Conventional such a program is the undrained undrained modulus analysis) or case not model or deformations. loads stress effects must be indirectly considered by inputing parameters for the or bi-linearly a linear soil via for details. (1973) theses by Wong to is referred reader The BRACE. the these Duncan and Chang (1974), Clough and Tsui Palmer (1972), Cole and Burland MIT (1972), (1972), Indeed, insights have been gained. to model soil parameter the undrained drained parameters, C pore (e.g., soil strength and case input and (total for stress the drained (effective stress analysis). Pore Pressure Dissipation Recently, new insight into the evaluation of the validity of the undrained assumption and total soil stress 43 for excavation has been presented by Clough and analysis to model technique TIME-CONSTRUCT and at authors (Clough 1980) interest are of discussed this the study was for not available documentation its since is computer program this writing is In any event, complete. purpose of The The name of excavation. distribution given rates of pressure dissipation occurs during and to show how pore after for excavation sequence (meters per day). excavation finite element the The authors used (1979). Osaimi is not the published results by the to the engineer and will be following paragraphs. in the Using TIME-CONSTRUCT Clough and Osaimi analyzed several cases. excavation are shown in Figure the one central protion of that decreasing drainage represent the bottom of the the excavation For wide excavation 2.3.2. unloading and dimensional dimensional of a one Results of the analysis cut. The figure to corresponds rate the shows an increase in the percentage of consolidation at the end of construction for the wide range of permeabilities analysed. Figures 2.3.3a two and b summarize the analysis dimensional excavation for cases of both nonlinear pressure soil behavior. excess pore the pore pressure response at the bottom of the excavation contours is essentially one Dissipation of the excess occur vertically. Of of negative linear and Contours of negative shown indicate that dimensional. results for general interest, excess pore pore pressures will in pressure Figure 2.3.3a for no wall in 44 are shown place in the magnitudes can conclude that Therefore we of negative excess somewhere between the two consolidation would occur for impermeable Note that this pressure would be at In any event more cases. the sheet pile wall of drainage due to dewatering which excavation construction. a result, As pressures due to produce an upward movement of consistently show settlement time, of the (1) we can conclude the shear alone will the soil mass behind the for many case Since measurements and observations studies than for analysis by Clough and Osaimi does not dissipation of excess pore wall. the type. the role accompanies with pore the for (sheetpile), of a more pervious wall realistic case consider inhibits of an impervious wall markedly consolidation. the As would be expected the linearly behaving soil. presence values for comparison with the supported excavation occurs behind the wall for such excavations one or more following: The dissipation of negative excess due to shear behind the wall or larger positive pore pressure is negated by equal excess pore pressures resulting from dewatering. (2) The heave movements are non-existent behind the wall due to greater settlement inward wall movement the bottom of resulting and/or loss from of ground towards the excavation with time. 45 including surcharging by traffic or Other factors (3) equipment as Clough & Osaimi One important conclusion was their study. as a result of occurs fact is probably based on the commonly generally field than predicted by Extrapolating test results in the lab undetected drainage thick likely to occur more rapidly. several times more rapidly specimens "end of further note that They that consolidation in the available methods. the field is latter conclusion accepted The undrained, low permeability clay. consolidation in the This drawn by Clough and Osaimi unlikely to occur even in construction" case is deposits of suggest. in analyses of the field layers may exist may using small situation where explain some of discrepancy. 2.3.3 Stress Path Method The Lambe's Path Method is Stress understanding and analyzing a given geotechnical Lambe problem. (1967) and Lambe for both a useful method and Marr (1979) engineering describe the fundamentals and applications of this method. By selecting and analyzing representative or "average" soil elements, one can attempt to estimate the stresses and strains that will occur in the phase of field for each construction. For a supported excavation one can subject representative stresses, soil specimens apply the to the total stress excavation and measure in-situ changes the strains, initial associated with pore pressures (and 46 and coefficients of hence, effective stresses), consolidation and lateral earth pressure, K.. Of course the method has Sample disturbance aware of. affects measured values of coefficient of consolidation, strength, determined tests path the initial in engineer. the evaluation of performance of present to run. to varying Many degrees geotechnical if the engineer is the the of the aware predicted versus measured geotechnical actual Stress and the applicability of this method The value limitations. 2.4 not of the method outweigh The advantages limitations, particularly lie in is K. in the field. available to the other methods the K, can be both expensive and difficult limitations however, are of these and modulus. initial stresses from reloading to the truly representative of should be one limitations some projects. CONCLUSIONS The measurements from the case histories literature show that time dissipation) are of excavation. For cohesive exist effects significant (pore pressure importance Recent numerical include in error and may be excavations. techniques allow analysis which may the effects of time, but most use stress-strain parameters. have non-linear conditions the undrained assumption is only a design simplification which is seriously in error in some in braced soils partially drained during construction and from the cited Other numerical parameter models, linear techniques which are expensive and 47 difficult Clough to use and and Osaimi don't have consider developed a time effects. computer program (TIME-CONSTRUCT), which considers non-linear strain behavior, their dependent only stress treated Nevertheless of area the actual studies looks date have to advance of an to forward performance time excavation. a significant is writer The versus Path parameters Finite numerical conjunction and appropriate soil excavation could approach. with technique the time include Method obtain with provides Method which Element excavation an their work Stress powerful the hypothetical and an in this evaluation actual of excavation TIME-CONSTRUCT. The soil simple, study. predicted using a Although the complex Stress Path parameter then be effects. Stress the can a rational be stress Method input. predicted to One may Path used way using The sequential distribution The combine Method. to model used select to in determine deformations this of fundamental r/wrP/Y I, / "St / /AX /7 I' 1/ I 1/ H H WAkER / / .EL12/AE4A/r / HH / / I / I / -I---- / I ~ 7l/ / :r AN /,> 7"^ I I liii I EXA G TE' DZ-Fo~'k~A77OMA ,ELEmcA/r 2 / I /150 400 $TRj~SS -5~0 0 73A1 EXAMPLE BRACED EXCAVATION GEOMETRY FIG. 2.1.1 49 + 0 28LA. Ivo R AIA LY COW50L / DATrE0 -I- is /c 22A :B i 0 ~= ~rv-i&)~ + IVJ STRESS OF PATHS NORMALLY AND P A FOR UNDRAINED UNLOADING OVER CONSOLIDATED SOIL ELEMENTS FIG. 2.1.2 50 - aue PAT' + AiNED SHEAR U ES~ ri 4. .-- S c ivo CON54 LuDATioN ' Y0 T., P, p ELEMZAr / K0 I L"o + I %0 / z 151 U14 PATh -Z U.NrZAt INDZ SHIAR CoWS0o.L-DATIoN H EAVE f4 LEWT 2 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR NORMALLY CONSOLIDATED SOIL-NO DEWATERING FIG. 2.1.32 51 + _m 2u 3 -~~~~ LLSS - :'\-s Z-3S C045 - i'4Fcs Z U-sNM 4e54AR I.) tn'ntoN a 'i. Vbhe TV*Y 0,14c, P, P LE M'-eA/T / i'o ± L-i d(/q 131-4 / - 12 1p . PATH Co IJSo seM.10MIt t>At -r 1.-Z - LNDRAINEb SHEA. Z - Ic! 4L5JEMEAIT CNs o u r,N ,f 2Z STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR NORMALLY CONSOLIDATED SOIL-WITH DEWATERING FIG.2.1.3b 52 -I3 II 1~~~~ .1 Sk49EAQ- co Z-'s ~vo~~K:s, Mn UAN0rItAPrl> -'Z - -- - I 1 S0Pl>APn> -I U. 0 .EL.P1MEAT I 4U8 ~J-~ T401 17-vo P,' zs :1 PATH Cof45o,.V"A'IOAV 4r- HFAVAE i-2 UNtMAINED SIAEP 2-5 C_6ricbAiNl ELE-MEAvT a. STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION OVER CONSOLIDATED SOIL-NO DEWATERING FOR FIG.2.13c ,t3~~0 53 *K *Pof+ a -____ Lt.,* - xrDRANEt 54EARL cONSOUriOJ ~140 pi a oELE.MA17A/ I(f / ~-' + k-k 0 -1 / ~ATM i--Z LJ-4O /uNE Z-'S a-ESP 4 Cou4soubA1IoN Co ,IoLIO4-io HEAVE-1- z'EWrERJAG REL'uzcES HEAV ass ELEMEAT s| 2 STRESS PATHS FOR UNDRAINED UNLOADING FOLLOWED BY PORE PRESSURE DISSIPATION FOR OVERCONSOLIDATED SOIL-WITH DEWATERING FIG. 2.1.31 54 //%\ w ow DEWATER K0 he- o= hea.d drop /7 ss5 ss) SZD(s iota/ /tead -lo EXCAVATE time r0 aL=head~ drop 06 hA 5 -h-LL( h > tofca/ /ead DEWATER + EXCAVATE AVAT E XC 6 -) t o-ti heoxd = h - G s -a cdewoter- e xcvate a +er- La-mbe. DETERMINATION OF TOTAL HEAD - TO EXCAVATION SUBJECT (19618) AND/OR DEWATERING FIG. 2.14 L 250 0 14000 T 3.0 5000 N A - 6m 2.0 20C 4000 12-000 I3 b t5o 0/ 1.0 3000 -- G00ps0 0 7 7' 8000 % 2000 --- SC 0. so 0 4 000 - 0 1000 3000 2000 5000 4000 STRESS PATH FOR SPECIMEN 6000 7000 0 t1 0* ACTIVE CASE STRESS 500 1000 500 0 pSi Oh; PATH FOR 2000- pst ACT!VE N SPECIMEN N- I-fl CASE 0 0 5000I N 2500 40001 P - 4000 e 8000 6000 Stress History For Specimens N Gnd 0 2000 p / 3000 1500 Ov P-s - I- O5 p s.I P th 2000 1000 1000 50C 0 to 7 .7p .6p faces% FROM HENIKEL (131O) 0 0 2000 1000 2000 3000 5000 4000 hl1 P 6000 I. STRESS PATH FOR SPECIMEN 0: PASSIVE CASE 7000 0 500 1000 1500 2000 2500 3000 0r, ps. STRESS PATH FOR SPECIMEN N. PASSIVE CASE STRESS PATHS FOR ACTIVE AND PASSIVE CONDITIONS FOR NORMALLY AND OVERCONSOLIDATED SOIL FIG. 2.1.5 4~1 -a EXCAV'ATtoM 0 TV ru N. T> P o It-4I hp,, . Y pressure un N + U. (StATIC) RVo, l EtP 10 0 'V 1/ FLOW NE T ;u71 1 ressire h0ea.d 4-5 ot4 - e\eJQ oVIheod Vecxd STRESS 2a -4 PATHS FOR EXCAVATION IN COHESIONLESS SAND FIG. 2.2.1 Flow Flow FILL SILT -SAND.-. -- GRAVELLY'. 'SAND o . 5 6 U, B - . - //IA\\WI/ , Piping of of Fines into Fines from Coarse Structure Coarse Structure -A]Movement - I. FRoM CLOuG6 PIPING/SUFFOSION MECHANISMS a' DAvI1OSoij ('977) F IG. 2.2.2 58 t -i, L-r.I 0 .6I I,1j .aa C - 02 / C a er A.erg -- -tr. ~ - 0 2 0202 LA!~I lod .lt -e~ cpr 06&CJ, Air teripero;bre I - p% Avercge strut lood, ion vrsus cepto 0 2 4 0 2 202 0C 202 6 2 LWIJ~H EF - E -2-0- c 'A' level struts c 'D level struts 2-0- - ~ .0 __ C 7 -0 6-0 5-0 ------- ~ ---- -- --- levei stru s Q3 2. 0 110 9- Dlevel struts C 7, 6- 5. 4- 0- I 3. 0-2I. 0 L.. A-mx - vOd tes Min. voues 10 9. 06- 76 0[ 5 4. 33. 2 E'level struts OF L.--Al -- EXcavotion cod braccing cornpiefed wedges removed .0 7 6 0- * F level srt 3. .0 A 2' I. O__.. 2 -19.15 %' 26 1 6 seot.+ - 20 14 22 30 1 Oct D/o/AG/a f V.TrAPUA 15 7 -Nov 23 - 1 -DeC 9 17 2 5 1 10 47956 1 26 Jan. - 13 wi 11 Feb.- (1957) INCREASE IN STRUT LOAD VS. BRACED CUT IN STIFF TIME FOR A FISSURED CLAY FIG.22.3 59 C /2 V K~.. 1 t t A/o&7-HAMP7Zw VAKYEZ) dAY (DD '2- V /sSA97) /0 2. 0 0.8 __ ____ Ilt I Z 5-0 0 _ ___ _ ___ __ _____ /00 20 00 CYtCLE_ _ _ ILL -ruTA LOADING (-) II I . 2 CA S c 5 20 50 -rs '\ 7.EST VARIATION /0 IN COEFFICIENT /00 CoO 4o AFTEZ LADO 973) OF CONSOLIDATION FIG. 2.24 E description Water con!ent SSoil 20 30 40 50 Undrained shear strength Unit weight J /m t /m? 3 1 2 3 -IT IV rS-61 ITS-62 St S-631 S-190 T . 5 FILL -87 186 188- CLAY CRUST 0 ---- w L- -L -- -5 EARTH PRESSURE CELLS 89 5 187 E 5 192 7 194 11 - 01 5 0 20 184 li natural water content : liquid limit wp= plastic limit w S V sensitivity z cone z vane 121 131 141 2 Key S - Settlement bolts P - Piezometer _ 15 I -14.1 --E -15.3 = Typical soitl data 0 5 10 Scale, m Instrumentation details - Tdlefonhuset. FROM DtAw'io ; SOIL PROFILE, 0 11 1 -15 w ON' 101 ___2_ 208 -3.6 81 P p_9 z -10 - -5' 71 w V+i 187 2 -112 + -02 6 t 868 -1 - 0- SILTY CLAY I ------ 2 5 185 1 - ------------------------ --- EXCAVATION, AND INSTRUMENTATION DETAILS WALL IN SOFT CLAY, OSLO FOR A RoTi (97Z.) BRACED SLURRY F-IG. 2.2.5 61 100 0 200 50c /00 600 700 Indr cf nistollation 300 ottm is B EARTH PRESSURE 16 .12 * - 10 -~ , ,-- --P -- T0 I 3 . ---- d 8-- o~~~N i * a>r~ 5. C TOTAL FORCE -200 041 LOCATON T-. 0 038 E PORE PRBECSSUR E SUMMARYOF .OBSER.E --.. .PP 2--------- 9 0 0 0 C 130 rC 0 . 0 2 E - 2 1 Po'i 0 100 5-63 -'-" SETTLEMENT- ...- 400 30C 20C DAY Summary OF Soo 60070 NUMBER of observations FROM 1D'tB,,Aci0 SUMMARY F - - from Ren' Dec 1969 to Sept 1971 (1577.) OBSERVATIONS FOR BRACED CUT IN SOFT CLAY, OSLO F IG.2.2.6 1 62 SI-2 T S4 is- +20 - 0 - IS-2 /WAAA7AaywA Sand JS-3' -20 Medium clay layer I P5-25 o S4-39 -40 layerclay s___o WIS-1 o-25 -39 P6-52ijo P1 S2 o-52%, P2 -60- Soft clay-sand layer III -80 P3 -77;, N -92Bl Tif BMf 0 -991, +2 B p, 2 > (tons/m ) - 20 10 2DL STRESS BELOW THE CAES PATH FOR PIEZOMETER P-1 FOUNDATION EXCAVATION F G.2.7 BOSCO SCHOOL DON 3, 70 ,, 0-0 0 12 7 20- / / -5 22 /*/ N I- 40- W 15 a 60- -20 *- H ~- -- + H to Stiff ld -+ H C /C (3.6 M) (.,3 50FT Bottom of Excavation P-_ Concrete Wall l80FT Boston Blue 10 H STRUTS Z 12' -1*--- bIv Medium 100- 30 _+ Stiff Boston Blue Clay with Sand Len ses a. H N Very Stiff to 10 /////// 122 HARD Y E LLOW CLAY / V. Fl LL ,3 STRUT CLAY B 14WF127 TILL C D 14 WF 103 14WF 176 WALF 36WF170' 36WF 150 36WF30 FRom 3AWORSKi (1973) ROCK SOUTH COVE SUBWAY EXCAVATION TEST SECTION PIEZOMETER P-4 FIG. 2.2.8 Ut~~~ ao- n 44oSDE WALLS Mo / 00- -44 -0 L&PPR L04". (a -4 /00- -- -Zoo BEAM ThTS R4jM0Y*D - - 48- //0 /Ole -//0 I//0 4- iA/Jr/AL. ocr /969 949 86 -78 78 AFTEP, DATA FRoM .3AvOtKi AuG SEp OC-r NOV DOC JAN FES JAA. AP1 . AY E 9 (1973) - :3-"L.Y 1970 STRUT LOAD AND PORE WATER PRESSURE VS. TIME-SOUTH COVE SECTION FIG.2.29 65 z I-i PRESSURE _j w w 0 120f 0 20 HEAD 40 (FT) 80 60 A 100 FILL -10 I- Hd. Yet. -CLAY 0 INITIAL READINGS (3/69) EXCAVATION 00- -20 Stiff Boston -30 80_h40 FINAL CLAY PH-3 (4/70) p_-- /777 N PH-4 P5 P -(ON Medium -70 READING < -P 4 Blue -50 COMPLETE (11/69) H . OF EXCAVATION) Boston 40- -80 Blue -90 CLAY -__ n--P6 _____ STATiC 20 -100 Uss K walI =Kh I TILL soil Don Bosco High School PH -4 H - 0~"7 ~ P nu .- II P-I-H FROM ~SAWORSKI (11-7) MEASURED AND PREDICTED PORE PRESSURES-SOUTH COVE STEADY TEST STATE SECTION F 1G. 2.2.10 66 EA E . 2 Open tiroe,' panel ( -0x E V, Steei [p, . E ~ E - EE E Water conten (%) 0 1-7 1- !-9 s/QkC 2m density(ton/-' B.lk 10 20 30 40 50 60 70 E Ock beading plre Screw type steel struts Stee' re'erence 0-9 M 1-33m) waling(.70NP) 2-0 2-1 Shear stre-grh (ton/m2) 24 6 81012141618 Sens;tivity 4 LL PL Uncor fined1 compressior tests fIn I 1 /one g -_ _ 3 boring 27 -_--_-_-_-_-- - 30 120 ~ C, MaxImLim winter strut 0 ; 7 6 5 4 lood(ton/m rur) 3 2 1 Autumn stru load (t 0 7 2 0 m run) 4 5i5 5 A -+ Max'mum frost penetration .. 15Nov -25 Nov. C-. 4 Feb. , Isept(Before 27.ar..956 excavation) 20 Sept. Lines of zero pore wcter pressure F- 0 1 Distance scc'e 2 rn TIME DEPENDENT BEHAVIOR OF TEST CUT (Ju20Sept ? 21 Oct. T 5 Nov. 25 NO V. FROM WERLLM AN[) DSAGio (1950 IN STIFF FISSURED CLAY FIG. 22.11 67 2c Z 29 psi. 2ct= 23 psi. w 31-0 %Le p.s. 30-9 - 14-5 psi. 9-.p.si. 320 - 14 p-s-i. 17 31-0 -- Shear zone 15 min. test p =30 ps 7 day test Ct= 1 7 0 0 ps.f. c = 2100 ps.f. Aj 4 9.3 51 .20-8 C A = "rheolog;cal" +0-6 decrease in strength 100% ecrease due to 6") c 80 cl - 60- Block 2 6 31 Water content 41 increase in 0 Aw 2015 mns. 6 hrs. l aCy 2 5 Time to failure t 15 10 (fi scale) 20 days c= rzor sirength, time to fcilure =15 mins. c1zsheor strength, tirr.e to failure =t ROm EFFECT OF ON STRENGTH VARIATION IN OF TIME TO UNDRAINED TRIAXIAL sKEMP-roej Aus LAROCHELL1E J% FAILURE TESTS FG. 2.2.12 > 68 At-/h SAM^' (o p~s) 5' | AoArxdrw*N 10 IL4 -50 oc/47 -50 L6 0 T74 1 /cc/e /03eH 71s T S-c1roN A i- 0. - lr7, 0 "*C *5)',-i, 4 /0. &0. - Se - / / O#9d7J K A- .e4 '/Oa0*~ cm/s, N K * r ro-.sc //7~ -,/0 8ro #0. 4/s/ o cr/7"5 s o pio .$a*! N 428I7m7 GO - . /L o /0,4 -'/Xie GP-ay .5o7 - C/ey A/5O7O' y ... ,awn any,,-,,,,, S.'leebn; - SO./ A1-4 r cl"ece See/c -/./ 7 EXCAVATION PENETRATING 5sr SEcf/oA B SILT: MBTA FRMo\ TEST LAMBE 0570) SECTIONS A & B FIG. 2.2.173 69 0 F/LL AMLasured Pote Pressures x 40 feet from wo// * /8 feet from wo/I /0 o 9 feet from woll on 6/1/69 Steoy S..pge K 20- Best Estrnoe- Kj S1L T Stoic , /4s 30 x 0 40 7LL 0 / 2 60 - 3 PPESSLE' IN K/PS/FT 2 POPE PPESSUPE .ECT/ON A 0 Teas4jred 20 ft from x C /0 M easured wa// a/ong wo// //IG4/68 FIL L K t~J K k 30- 0 StOfc, LIS SILT Q 40- TILL Steady Seepcpe 60- 0 , U4. 5 I I I I 2 3 K/PS'/T PPc'SLPE /N POPE PPESSUPE SEC 7/ON MEASURED AND PREDICTED PORE MBTA TEST SECTIONS A AND B I 4 2 B PRESSURE FIG. 2.2.14 GANDY CLAY5, CLAYEY SAN D5 STRUT -- H 0 71=1 ":-- O.65kH 0.65KVH K=TANz(45-/) K, =TAN2(i5-/) TiER-AGHi AtN4DkCK PE.CK (Ie7) TERZAGHI & PECK I HTAN(+S- (tc3(3) DESIGN ENVELOPES FIG. 23Ia 'PECK (1%69) P0EC K, "ANSON A wTHORNBURN (1'314) fP~ f(~~/( 0.s H 0.15 H o.751 --- 4 YT-4UT L! H-4CFOPt N z--mg ,'~ YH-c CLAYS N *~oiZ' 47 Y H '7,,,.' 0.25H N=c N H os H 0.75H 6. 0.25 H YH -2j ozH N > 6 " 8, LARGE DEPTH OF CLAY BELOW 0 -H CUT TERZAGHI & PECK DESIGN ENVELOPES FIG. 2.3.lb TIME TO COMPLETE EXCAVATION 0 5 days A 50 days o 500 days a0 0 z 0 CE 80- 50' C04 Cm/seC 60k) LX 0 Cl) 0 0 7VT k = 0 Lu EXCAVATION Ift = 0.305m 40- 10-6 cm/sec 20 - 1.5 x 10-5 cm/sec -I YO~8 cm/Sec- 0 0 0 2 4 2 4 8 6 RATE OF EXCAVATION . in 10 ft/day FROM CI0ot-H A, OSAIMI (979) CONSOLIDATION AT THE END OF ONE-DIMENSIONAL EXCAVATION FIG.2.3.2 73 NS. '.(&T7 -500 Imeavation K K Iy Rate - 0.5 ft/day 10-8 o/c rr 3o cr 60 r_^ ll wall 30 -500 -500 Vro- O"SPm (i9T7) ONTOURS OF EXCESS PORE PRESSURE (pof) AT THE END OF EXCAVATION. CONTOURS OF NEGATIVE EXCESS PORE PRESSURE FOR TWO-DIMENSIONAL EXCAVATION FIG. 23.30 74 Strut K all W- . 100 -2500 -ow 3o FT 40 $r Strut Wall 'iT KI . 300 Cnod"ks ,,wmvbe-) -2500 Ffw OSAIMI (s9TT) CODNiOURS OF EXCESS PORE PESURE (psf) AT THE ED OF EICAVATIO. CONTOURS OF NEGATIVE EXCESS PORE PRESSURE FOR TWO-DIMENSIONAL EXCAVATION FIG. 2.3.3b 75 CHAPTER THREE PROPOSED PROCEDURE FOR INCORPORATING TIME IN THE PREDICTION OF THE PERFORMANCE OF A BRACED EXCAVATION INTRODUCTION 3.0 In to this chapter the writer outlines a proposed procedure (pore pressure incorporate a major time effect construction performance. the prediction of dissipation) in Acknowledging advantages of certain aspects of available Finite Element the writer to use both procedure integrates The Marr Method is for this method The basic stress is equals the the Stress Path is presented by Lambe and principle behind the the effective stress the effective Hence this Path Method approach. The most recent edition (1979). lead the use of a sophisticated computer fundamental basis Method. Path Method, in a composite procedure. a tool for a Stress model as Stress techniques and the principle, total Stress Path which states stress minus that the pore pressure. TI Soil behavior is dependent on the effective and future changes in effective Table problems; 3.1 illustrates force, stress history stress. the types of geotechnical deformation, stability, geotechnical engineer must face and flow, which the in practice. Generally, he 76 Table must predict the performance of constructed facility. 3.2 summarizes the predict performance the classes of problems presented in Table 3.2 the steps follows writer for The method developed in this chapter by 3.1. Table Stress Path Method to steps used in the in the and for force deformation. OUTLINE OF THE PROPOSED METHOD 3.1 This procedure is each pass improved with solution can be an iteration whose the steps through outlined. Actual field performance measurements during construction can be input to update or procedure is as adjust proposed follows: Description Step (1) The the solution. Using computer program which a finite element models braced excavation an initial geometry and properties (i.e. (i.e. input BRACE), initial soil and structure strength, moduli, pore pressure parameters). (2) From Step (1) obtain total stresses (approximate). Ac~ (3) From Step (2) obtain usE(the generated by the change excess pore pressure in total stress due to excavation). (4) Estimate u (the excess from the altered pore pressure flow conditions resulting associated with 77 the excavation). method Run dissipation analysis condition (i.e. one, for actual drainage two, or point (7) a representative and an undisturbed Consolidate in-situ three way drainage) coefficient of consolidation. Estimate the percentage of Select if steady state anticipated. with estimated (6) flow net or other (FEDAR) may be necessary conditions are (5) A hand drawn the soil stresses. dissipation, D. element(s) or soil sample(s). specimeNs) to Measure prediction the the estimated coefficient of consolidation. (8) Shear the obtained other the be for words shear sheared second the sample set the by applying procedure, The conditions executed after partially the first of stress element. Measure strains 2S . are total representative apply ACrF. under a In actual set of pat h uE tests no drainage. the drained first tests a nd If pass may might a th rough be required. (9) (10) Using the results estimated time determine the t of (5) and for the excavation percentage of of (7) and the constructio n, dissipation,D. Then, AUJT~ D 4UE) +_ 1. One might use superposition as shown previously in Figure 2.1.4 to obtain the initial net excess pore press. 78 (11) to Apply the consolidation (12) strain, £c- = ES+Ee Find; E This is a convenient simplification of the partially drained behavior. that the shear summation of for Later, the one might drainage the strains Compute same use to refine a final stress path in that parameters the actual established contours of equal Figure determined for to the path tests with Eva the computer program tests, undrained effective stress. partial stress 3.1. From such any element fL ~ strain 2EV curve passing level. from (BRACE). strain ratio ,v; ~ through the actual stress Re-input assumed equal be replaced with a single modulus passing seen for soil modulusE and Poisson's Here we assume into is actual, the solution. V (14) it a partially drained stress terminating at can Here followed by consolidation are strain (13) the Measure specimen. soil the test data For a series of can be plotted as plots moduli can be by plotting the total 79 estimating the stress path on this plot, "undrained" strains and adding them to the estimated consolidation strains. Check against original (15) reiterate procedure total stress paths and if necessary to refine solution. Below are summarized the main simplifications and assumptions made in the presentation of the method; Deformations (1) for an undrained unloading followed by consolidation to a final effective stress equal deformations for a partially drained path terminating at The actual (2) stress the same point stress effective stress. final strain curve can be replaced with single modulus passing through the actual stress level. The dissipation analysis (3) details of initial pore is not pressure distribution. Contour plots of equal vertical (4) constructed similar consolidated soil too affected by to the strain can be plot for the normally in Figure 3.1. Obviously this method relies on a laboratory technique other in to obtain a soil modulus. factors influence this value. Sample disturbance and Another the difficulty in correctly assessing the dissipation. of this Stress However the writer Path Method type approach for obtaining input for Finite Element testing believes technique limitation lies pore pressure the application is a rational the computer program. parameter studies have shown for As supported 80 excavation, notably the Palmer soil deformation or stress the greatest and Kenney (1971) strain modulus influence on the solution. is found study, to have One of the proposed method's main objectives is to obtain and use in a way which considers the effect of pore pressure dissipation. the this modulus 81 TYPE EXAMPLE Predicted Para meters Needed T U, ()h F Forces,E Wall s,E H Deforma- c H v Off-Shore w Au with cycling Structure FS F FS Dam Stability Natural Slope q, ht Flow -- - Flow through Dam underprtce from Stability of soil particles Lambe and Marr GEOTECHNICAL k (1979) PERFORMANCE TABLE 3.1 82 Step (1) 1 2 3 4 5 6 Force and deformation (2) Stability (3) Flow (4) Estimate flow Estimate location of pattern surface of minimum stability Select average element or select several elements For selected element(s), determine stress paths for: (a) Geological history, i.e., past; and (b) design life of structure, i.e., future On soil existing at or near selected elements in field situation Run tests along stress paths determined in step 3 (Orient samples for tests same as in field) (Use field permeant in flow tests) Obtain permeability; Obtain strength or Obtain stress strain Measure any strength parameters or modulus movement of soil fines Determine flow net Factor of safety = Force = f(stress) or average strength/ f(modulus) average shear stress Evaluate stability of Average shear stress Deformation = soil to flow from: Force polygon; f(strain or) or elastic analysis; f(modulus) or frnite element analysis; or stress paths Estimate stressstrain pattern from Lambe and Marr STRESS (1979) PATH METHOD TABLE S0 0 w 3 I Il I --7-EN- 2------- ba 62 I --I b 1 a , , , 3 I -- 0.70 =. 0. H -t 1 ~1*~ V 2 00~ w~ % 0.071% -~ 2 2 3 5 2= LAN|LLMNILLAS CLAY CONTOURS (kg/cm 2 ) FROM LAMSE OF EQUAL VERTICAL 1 WHrTMAW (1963) STRAIN FIG. 3.1 84 FOUR CHAPTER ILLUSTRATION AND OF THE PROPOSED A TO To outlined prediction of The Japan. 29.5 take the Specifically, meters. and the loads stage. The excavation depth at stage this is is of depth to excavation a critical for a Tokyo, in attempt will writer deformations predict make a design to reach years two the drained and currently underway is over partially a braced cut of performance illustrate the writer will 3, chapter in excavation to scheduled the develop and to handle the method of conditions approximately meters. It is emphazized the good stress history of information pertaining below 45 meters. static or lacking Initial non-static) have is deposit, the soil available the that Particularly insufficient. the STUDY CASE to a vehicle as serve application on PROCEDURE INTRODUCTION 4.0 20 APPLICATION to the character groundwater not been (1) stress (2) u. (3) limited history soil (oedometer samples and as measured. tests) tests a the of conditions information: missing well is information adequate as data test lack of soil (i.e. Summarizing 85 is to of this chapter the main purpose Nevertheless, its illustrate the proposed method and demonstrate In applicability. the available test and boring data. 4.1 PREDICTION TYPE OF In Lambe's (1973) Rankine lecture "Predictions Engineering", Lambe classified predictions A Before event --------- B During event Not known Bl During event C After event Not C1 After event Known The prediction writer's A prediction prediction. underway currently writer stages AT TIME OF PREDICTION MADE TYPE did prior would Known will be of early fall into a known classification stages of A the excavation the class B category. not have measurements to Soil in follows: as RESULTS WHEN PREDICTION PREDICTION The made using the process a prediction is of performance of these prediction. PROJECT DESCRIPTION 4.2 4.2.1 The facility General excavation for the is for construction of a pumping station Nakagawa Sewage Treatment Plant in Tokyo 86 and is designated designed wall. 79 as Plan meters internal mediate deep dimensions long and vertical Figure locations. 4. 2.2 Cons truct pertinent 4.3 4.2.2 Soil Limited profile preliminary of silty clay extending Below these sandy clay soil below this from a approximately wall columns of plan details. to wall, have excavation, 25 meters the schedule this inter- supported by lime soil has view and Also shown been cross secton are recent for construction and period. lies soil data intensely sandy silt, to a stratified fine depth a relatively indicated sands, of that the deposits clayey of silt approximately 45 dense stratum of soil sand and meters. and layers. cohesive are from pile Conditions soft of are pipe is CONDITIONS consists plasticity. filled system Schedule during relatively The support bracing will the shows depicts events SUBSURFACE 4.3.1 ion wide derived upper 4.2.1 concrete excavation lot construction boring Figure the Within the excavation meters support of these of Cross piers. stabilization The braced, 52.5 dimension. executed. B. a cross-lot concrete showing site Blow soil counts typically depth deposits to are of moderate (blows/30cm) in less than 10, approximately 50 the gradually at to high top 30 meters increasing a depth of 50 meters. 87 Groundwater 4.3.2 Groundwater level is encountered at 1 to 1.5 meters below ground surface. approximately coincides with depth Elevation on the boring logs (i.e. 5 meters, elevation = -5 meters).Unfortunately = depth in borings sea level) datum (i,e., to which not known it is these elevations are referenced to. Unfortunately conditions site. at this in this assumed nonstatic groundwater to verify static or available study. groundwater Static It 55 meters long term pumping below the ground surface. layer was ultimately reduced static (1968) are that a at that pore pressures were Kawasaki City Site revealed to conditions should be noted however, previous work in the Tokyo area by Lambe non-static due are not initial pore pressure data lower acquifer from the The total to -5 meters. head in this Therefore the initial condition assumption may be in error. NAKAGAWA PREDICTION 4.4 4.4.1 Initial Model of Field Situation Following the steps of the 3 the writer limited computer selected an initial preliminary soil data. developed to model program. closely model outlined procedure this soil profile A finite excavation using based on the element mesh was the BRACE The mesh geometry was organized excavation and bracing levels simplified soil in Chapter stratification. as well III to as Areas of anticipated high 88 stress concentrations modeled with finite is smaller element a detail of excavation to the and Linearly the mesh initial 250. were as to III Run and for This of us ed Poiss on 's cohesive fie ld the run the situation. for employed will be referred using an t o a value of th e Etx ent ire 0.40 and 0 .45 of co hes ion les s and 4.4. 2 were model Ratio are and sh owing zone rough ly to wall) Figure 4.4.1. obtained w ere corres po nds were values wall to profile, s tra i n moduli Values 75 which initial to model analysis. A. adjacent in Figure levels These values selected The shown are bracing Input deposit. elements excavation BRACE equal /St= e lements e lastic stress henceforth E ,/W (i.e. s 0 ils, respectively. 4.4.2 -Stress Paths To check A) (Run the selected in Figure stress paths unloading of near paths path the for might excavation. the less become extended simpler were plotted on both the element and elastic the No. for the ed, although initial and final extension mode of unloading. for the are shown The extension and categoriz the within analysis. wall 345), analysis, diagrams paths and exc avation III p-q stress compre ssion Within be twe en behind total behind e asily Analysis BRACE linearly the III initial expect (e.g ., wall, BRACE the these this illust rate one the e lements Severa 1 of 4.4.3 of paths s "average" excavation. Initial re s ults stres total from at the soil total type bottom elements stress a s traight points indicates 89 4.4.3 Laboratory Test s And Revised Soil Profile General Five "undisturbed" 1 meter Shelby tubes to excavation the stress path and limit index (mechanical and supplement Visual Results of one at addition consolidated the and above, Soil Classification to 4 the path 6 combined executed information torvane by writer for tests, sieve by the 10 analyses writer to soil conditions. tests were also Mr. results adjacent on undrained tests borings anisotropically stress were supplied compression also all, and unconsolidated were of triaxial Matthew six performed made. test Southworth. isotropically in a Japanese lab obtained. Table 4.1 summarizes classification of the through A.6 for combined the tests, available MIT were to In triaxial hydrometer) classification performed In the available at MIT. undrained from recent samples were made testing consolidated Atterberg 7 jar long, 8 cm diameter brass in the plasticity chart the index tube and jar appendix give sieve analyses. . properties samples. c omplete Figure Atterberg Limit s plot and Figures grain 4.4.4 near visual size gives the A - A.1 plots the line. 90 Tests Path Stress stress "undisturbed" samples In order would predicted 3 was for flow Consequently 1o w in g (1) the field in Based it on the would the testing silts. that changes of that in writer Chapter time construction dewatering is to due consolidation within particularly occur, the inevitable. of consisted procedure the procedure the length assumed was construction the 3 steps. envelope undrained to the via This Pat hs from tes ts were BRACE of loc al stress were allowed decrement of Applying a simulat e applied change post coefficient Unfortunately no III to Run failure the of integrit y trends of t he reflects procedure pressures the situ extension or ( define envelope failure subs tantia 1 zones to in estimated the ompression w hile maintaini ng sample). The to state. Shearing Stress sampl es the Consolidating unload ing (3) clayey occur conditions stress (2) and stress where excavation sandy the project, this of the four for the writer simulate employed. altered fo to by executed tests path of results illustrate 4.4.4d through 4.4.4a Figures indicated A w hich yielding Pore controlled for each stabilize stress. in pore shear pre ssure ( back consol ida t ion and pressure) measure of con solidation. tes ts were performed whe re negative 91 excess pore pressures were this situation is This is because mainly dewatering was not was the initial computed to be plan. pore pre-shear likely occur the writer assuming a to in static assumption field to in the the as well. assumed deep that knowledge field, triaxial pressure although learn sufficient for pore the later distribution stresses dissipate originally implemented, pressure this to Not having effective Admittedly, allowed this of the initial tests were conditions. may be in values of coefficient error for the actual case. Coefficient Table of 4.2 Consolidation summarizes consolidation computed consolidation. Both methods were used. yielded type III time for this type the 100% of change A.14 plots Revised Soil Based results these on of prediction. The curves plot. of show for both pre-shear root of small load (Ladd, time and for difficult log time to writer has more square root of typical the square triaxial root of the from confidence data. time often and obtain this CV time ratios Thus, time post-shear log increment 1973) was and Figures vs. in A.7 volume tests. Profile the the borings square consolidation reliability through from of recent tests run a revised The profile soil at soil is borings MIT on the profile shown (October in samples was 1979) taken constructed Figure 4.4.6. and the from for the Strata 92 below 45 meters was inferred from older borings in the same general area. in the The strength profile shown for this The selection of extension and compression unloading. simple profile was (1) influenced by: available undrained strength data -high Su/ T, values determined (to be discussed from triaxial stress history missing and would help put perspective. Other such data factors such unquantified effects deep deposit, the Su/T-Y (2) of lack of better the writer used tests run at MIT, in and strain the stablization of strengths. information on this strength data selecting the from lower values of to represent the deposit. Limitations of the BRACE III computer BRACE III is materials that may be use the lime increased the test Because of the tests data is as high rate used in CIU compression tests soil may have although later)indicated some over- , useful consolidation selected figure was limited -- in the number of soil input. the maximum number different moduli at program the (20) The writer elected of materials "cost" to to model of assuming a simple strength profile described by two values of the ratio Su/0 0 o. The CIU compression tests plotted with the triaxial shown in Figure 4.4.7 tests performed at MIT. are The wide 93 of scatter attributed of time applied is high a as tested give because at ra te source of the are longer increments shown on as which time Figure during undrained Consequently Skempton extrapolated the chart. the octahedral effective words retrieved for strengths equalize. path it per pore took This is tests a increment, to pressures shear. a First, strengths series of correction for tests associated with the were the based sample obtained on depths by insitu stress. ocT In other 4.4.5) the per minute most th at i ndicated the Similarly st ress stress, applied strength to stress (Figure un drained higher writer from each estimating of 0 .5% + 5 minutes (15 shear showed dec rea se. allowed controlled significant ly samples an d to and increasing By Laroche 1le r ate not the at wh ich will strength por e pressures pressures a series error. and can be consoli dated w ere a strain tests CIU confining strain performed b y the writer the of unrepresentative subs tantiat ed by equalize Ja panese depth Skempton th e measured tests, likely given also fai lure to 2.2.12), CIU The the range wide from a at. sheared from the to samples was strength for from 3 example, a depth if of two 10 undrained meters were tests of sheared at 94 consolidated pressures of 5 TSM and 10 TSM, and FOc-r in the 6.3 TSM the approximated strength was extrapolated field was following fashion: in the strength was then reduced by 20% This excessively high strain CIU strengths as well as corrected data from the good for the compression of consolidated Kawasaki Clay from Ladd et P.I. higher equalling two is the tests have the strength comparison, undrained triaxial test In test compression tests. in the measured The extension tests. equalling approximately 50% strengths other triaxial the The agreement between MIT tests. the Table 4.3 summarizes rate. for the to correct .445 and .225 al for (P.I. data on normally = 40 + 10%) (1965) with a slightly show values of s compression and extension respectively. Although indicates define because the is showing large Su/:, 0 study the ratios probably some overconsolidation stress history data is degree of preconsolidation. of the assumed to for that there 28 meters, 18 to this the strength data lack of sufficient strength for data, not available to As previously stated for the agree well with Ladd et al purpose of the undrained deposit will be increase constantly with depth equal compression and 0.22&,o from for extension. (1965) although to 0.43 V, These values they may be 95 slightly conservative values in of test data the light available from 18 to 28 meters. Contours of Equal Vertical on the available Based vertical effective stress stress CIU and CAU tests, plots of equal Figures 4.4.8a and 4.4.8b strain were constructed. show contours of vertical the Strain paths path compression strain on a p-q plot for the CIU tests. tests TC-1 and and show reasonably good agreement. the two stress path tests TE-1 drawn through The two TC-2 are also For plotted extension unloading and TE-2 are plotted on Figure 4.4.8c and estimated contours of equal vertical strain are averaged These through these effective stress plots will be used to extrapolate loadings 4.4.4 at any depth Revised BRACE paths. strains for various to obtain soil moduli. III Analysis for Partially Drained Conditions A. General As previously stated, this prediction will address excavation when it has attained a 20 meter depth. reason for selecting of Figure 4.4.9. this depth is This figure profile and the Nakagawa excavation geometry for excavation stage (depth = bottom stability due One illustrated with shows a simplified 19.5 meters). to uplift becomes At the the help soil the sixth this depth, critical. A simple computation for the geometry critical depth, ZCR for equilibrium of the soil mass against uplift; in the figure determines the 96 -Z br - 45x I. - at 45 excavation this and meters Consequently III runs final to where B Run force of safety is this equals prediction will bottom instability is C are made for stresses updated the zero is downward force one). for treat a depth the loads and just prior to new BRACE Two imminent. from For prediction. this previous the run the the are used obtain moduli. B.-Computation of Partially Drained Moduli partially drained moduli incorporate consolidation strains in relation: The and upward stress effective anticipated and C the depth, be to deformations depth - C4-5-1-S9 lO the factor the (i.e., xu)Y' 2.1MIETERS ~/cm At (2- w h the both undrained ere: w h e r e: ET = 1) Undrained Shear Using linearly selected the terms of and p-u 0 elastic 50 tabulated and o= - E AL. VO&..u.MET IC SnTrA W Strains approximately excavation in TiA^L STRAW vCn -crA. q BRACE elements the for values the III RUN inside of initial the writer and outside total and A, stress sixth of the change excavation 97 stage. the (Table 4.4 shows such tabulated values of stress for final BRACE constructed III RUN C). Total from these values. stress paths are then Using the appropriate of strain contours,(see Figure 4.4.10)the total stress (minus the static pore pressure) can be superimposed undrained can be strains the estimated effective 2) plot path and the scaled off between contours along stress Consolidation Strains Due path. to Dissipation of Excess Pore Pressure within the Excavation Given the the final effective stress undrained shear, shear (typically negative subtracting stage from the value of estimated using excavation lateral pore pressure ~u. in this case) (p6 - the value of 'p. The average the the excess point established by u) can be obtained by for the Refer sixth excavation to Figure 4.4.10. degree of consolidation for one dimensional consolidation the wall drainage. impermeable is likely The Terzaghi equation for dimensionless time factor Tv due to this geometry theory. to Within inhibit the is; CVt V For a depth factor within (a) H of excavation equal the excavation is C 3 x 10 -3 to 20 meters the time computed using: ' c-wn/sec-nd selected as an average value from the stress path test data (b) t :.St 5 8inoriths is computed from 98 to represent an average Figure 4.4.11 unloading similar settlement time Whitman p. 414 for The drainage factor path procedure used to compute embankment This 0.05 for For a linear distribution of excess approximately observed within the verti cal any of depth or degree of pressure pore dissipated. to due be to added for estimates This to plot pr ess U re.) value the surficial or belo w the is posit ive to excess a one pore exc es s pore pressure for the bottom of the Uz would be derived the distribution specific in it i al excess ta bu late d excess also indicates a c tua 1 initial t he pressure the ac tua 1 nega t i ve th en and Having approximate mult iplyin g t i me s pore which 12b Z vs. of By t he 4.4.12a. nega tive 4 .4. negative element Uz of this of linear (1977) Figures r e present dissipation one Osaimi u ses (Ide all y a t o reasonably dissipation disc ret e constructed excess by dissipa tio n excavation. and to be excavation. pressure negative excess of s tudy the writ er of pore from Figure dimensional degree the bottom of the % obtained dist ribution drainage. stage of 2 the pressure this of consolidation considering Lambe & consolidating average degree excava tion the at the assumes double for yield an soil for construction will (see loading vneters LS .. 2 = - length then equals the for 1969) cohesive layer. time the HA = (45- L(.s) (c ) The to time excess (Table por e pressure shal low dewate ring within the pore pressure 4.4), later dissipated, excavation. 99 The excess pore be pressure due to shallow dewatering can analyzed using Figure 4.4.13 for level a change at one drainage boundary only. in piezometric This case also experiences double drainage and therefore the time will dissipated be the same as previously computed. excess pore pressures are computed for various obtained using this depths and elements The summation of Au, + 6u dissipated pore pressure and/or 4.4.14b based on the series of strain can be path stress The = (AuD). consolidation from volumetric and vertical extrapolated for a given depth. Since stress tests with dissipation of negative excess pore pressure were not run the plot in Figure 4.4.14a shows for case. this strains due are not likely and and are Using Figure 4.4.14a the post-shear tests, figure Au, gives a net value of in TSM. path factor Since to be in the zone likely in pore pressure recompression stage (3) is an unloading problem, to dissipation of negative excess therefore are changes this to have the pore pressure of primary consolidation a similar (but opposite in of the inferred lines stress relationship to sign) as the early path tests. Consolidation Due to Pore Pressure Dissipation Behind the Excavation The steel pile wall steel interlocks between prevent leakage. is assumed the to be impermeable. piles have been grouted to The 100 Below the lower silt remain constant access to and this layer the stratum is assumed a distant source Given these total head is of groundwater. assumptions, dewatering due to shallow pore pressures the wall. The stress organic silt path has test TC-1 that the upper of consolidation cm /sec. doubly drained stratum 20 meter indicates a coefficient approximately 7 x 10 this to to have free pumping within the excavation will not affect behind assumed for of Computing a time the time factor for associated with the deep excavation we get: T .0 1 and from Figure 4.4.12 U(k 12 */ A'VG similarly for the lower clayey silt we compute .03 A'/G Continuing with used for within the cut, tion and added of one dimensional strains are to the undrained contours of equal (4) the use strain plots. estimated theory as was for consolida- strains obtained from the See Table 4.4. Contours of Moduli Contours of moduli can finite then be element grid using the constructed across tabulated values for the the 101 discrete elements analyzed. contours of moduli in moduli for Figure 4.4.15 shows tons per square meter. the granular layers the Stress above and below the cohesive soils were estimated using empirical formulas based count (Mitchell and Gardner, for granular soils modulus the layered lower in the literature. level in this interior secant modulus will be BRACE III soil materials of moduli computer the fact that the from this plot were computer program by substituted initially assuming finite elements. Total stresses to improve the in Figure The final Run C was made using Fig. 4.4.16 and 20 The current version of BRACE III will handle a of 20 soil materials. Ideally zones of soil with similar modulus and Poisson's ratio would be contoured, since 4.4 these values for the materials can also be estimated as final run. of BRACE III is as shown in Table Unfortunately, the current version previously stated, limited to how many may be input. Ultimately the writer observed that Poisson's 14 from this solution by determining new or updated moduli as shown maximum the (moduli) and assigning the appropriate values to the materials. shear stress lower. Run B were used 4.4.16 1000 within zone is higher and therefore The values of modulus into the The sand and sandy clay stratum was reduced from 1650 outside of the excavation to the excavation to recognize on blow 1975) and compared with ranges of modulus in strain ratio will follow the trends in general outlined below: 102 Inside Zones a) 1) where the Excavation dewatering prevails and the net excess dissipation will pore pressure is positive, tend to increase Poisson's ratio 2) where the net excess pore pressure dissipation will tend is negative, to decrease Poisson's ratio Outside of Zones b) 1) where the the net excess dissipation will 2) where Excavation tend pressure pore to reduce Poisson's ratio the net excess pore pressure dissipation will tend positive is to is negative, increase Poisson's ratio 0.49 was Ultimately an average value of this value at cohesive soils, (0.2 - values 0.5) modeling of soil. the upper range usually used In general case tended to dominate selected in the for of typical finite element analysis the undrained strains in this the deformations. Ko (5) Ko = stress 0.5 for all soils was selected based path Ko consolidation data i equation and empirical on review of on these soils, the 1-sin correlations of Ko versus P.I. Anisotropy (6) To account Christian Also, for anisotropic (1971) shear strength, The Davis and yield criterion was used any yielded Elements are in BRACE assigned a modulus III. equalling 103 1 to 10% of the unyielded modulus, depending on the initial modulus value. C. ,Loads Deformations Predicted (1) Stability and General From the final BRACE III run, contours of deformation and stress are shown in Figures is Figure 4.4.23 through 4.4.23. undissipated excess a contour plot of is pore pressure and to show the approximate 4.4.17 trends prior intended to consolidation. Related aspects of techniques used interaction are (2) soil the III computer program to model in the BRACE structure section. discussed in this Deformations Figure 4.4.17 the deformed geometry illustrates of the steel pile wall towards from 12 centimeters at the the excavation range depth. line. lines at to a a 27 meter from 40 centimeters Bottom heave varies the wall the wall top of maximum of nearly 44 centimeters near Inward movement the sixth excavation stage. after to 76 centimeters Figures 4.4.18 and 4.4.19 at the center show selected of lateral displacement and bottom heave, respectively. Maximum ground surface excavation is 20 settlement behind the centimeters behind the excavation. occurring 25 meters Figure 4.4.24 compares 104 ground surface settlement with Note Peck's chart. the uncharacteristic heaving of the excavation settlement begins to occur at Ground surface face. In a distance of 3 meters behind the excavation. the 3 meter wide zone between the wall net upward movement a very small point the writer's opinion, since this and this In occurs. is contrary to the downward movements we would normally associate with past experience, face is lifting of this the way which the in part to due to the nodes applied the upward forces upward is When excavation release interaction. surfaces of the excavation the excavation heaves, on the newly include an Consequently, as sheeting elements. simulated the nodes shared by to force applied BRACE III soil-structure the computer program models exposed the excavation the bottom of the sheeting may also heave slightly. This behavior intended wall. to allow stiffness of above the enforced by soil the technique to slip behind involves setting sheeting equal set the axial to the soil the level BRACE axial soil (usually III runs stiffness of the stiffness. the to either the or zero above a selected the depth of excavation). this study equal the technique This stiffness, is in sheeting 105 fixing fixing b ehind method. A ithough the install at i on no b) ze ro s trut B, of no the III Run B ( the m agnified timber wedges) alr eady occurred assumed set of modulus) to (up by no the at was struts 1 linearly elastic first the Acknowledging C inc luded: of s ing i n itia shee t in g movements shims. in dif ficulty s tru t for (or of movement pr e stres partial 1y drained depth) th e realistic ts stru shims s h im c rush i n g was Run revised of C fixing ion. used Run imple- level for employed of latter the more a interact final crushing Al th ough Run the p ercentage a be evidence prestressing a) as in may options Input III BRACE in occurs not anal yses structure soil t he modeling w i th III BRACE is Therein approach. face was directions both i n node ement technique this current the in settl excavation the directly mented more that indicated directions applied and horizontal vertical in both node by comparing this me thod with the writer the made II I computer A BRACE the horizontal direction. study by is strut the node at which the is installation strut of Simulation to the crushing two showed runs large A and firs t using the inward 1 meter at a 20 meter of crushing this The 50%. Run error, the the of final s hims. BRACE Unfortu- 106 are experience or knowledge the (3) drawn usually parameters input related engineer's the from in performance actual of of bracing function the of selection The details. a states, (1973) Jaworski also are level excavation the above Movements as excavation. this for details and techniques shimming and prestressing actual the of knowledge have not does writer the nately, field. Lo ad s stresses lateral in negative lower level factors. to The this can struts early for stages convex tendency back to the load unusual struts While result, is lack is the top of from the excavation for This stages. loads shifted probably Jaworski of excavation of negative of struts. the in least at distribution away strut negative a cantilever as a non-prestressed two total and attributed be prestressing of bend upper Consequently struts. The excavation load the indeed wall. the to is later during the a more by displacement, sheeting behind typically behaves sheeting followed loads since Furthermore, the strut lack the to part the several in values shows 4.4.25 Figure strut, upper to the in as result that lower of one prestressing may notes give would illustrate. load a the four of the several contribute to five 107 sheeting elements required to accurately between strut model levels the Otherwise,uncharacteristic forces may be to three levels sheeting elements in this were strut. used Only between two strut study. for Stab il ity 4.4.26. cases basal where sta bility indicat in g meters. Also support For For ana lys is made ity an note stabili columns area of the is along the a t that for z ing e ffects bot tom heave Eide in would section both excavation, be the level the of any concrete The 13% used 4.4.4A analyses of shown recall excavation the assumed as comparison n eglected. 0f d imensions (H/B< 1) a ppr 0 ximately bo t tom th e Nakagawa strength and H/B> 1. p iers have been of these view Bjerrum instabil beneficia 1, Terzaghi's shallow excava tion for Figure for an excava tion of these analyzed using typically analysis in the sheeting Stability 4., is to be sheeting behavior. transferred may of plan area the plan excavation. the failure average surface can be estimate d by: (1) selecting the several assumed average failure elements surface along 21 108 determined equation The 4.4.26 extended time open excess negative the within strength decreases value drained" below. used " This 5= 0 is strength Factor Hence used is where concept into input c is of the for substituted the in soi swells H the the equation of the comp monl y undrained c; simplification, -c/B "I5= if it 0" is approach used for and the 1 Safety a "partially instead Su, the of soil n et outs ide elements the or in of dissipation as Ter zaghi excavation majority actual the method of Although the time with analysis stability shown for increases. content water Safety Consequently, cut. the elements the for and the this a in pressure pore excavation of which for resulted has point input and Factor Figure remains of for star t ing path (2) strengths the average (4) in b ased element stress effective final the from loading failure assumed on an each for strength selecting a (3) dissipation pressure of pore effects the including paths stress constructing (2) is a convenient this case the 109 Factor of Safety may Figure meter 4.4.27 stage and stress paths 4.4.28 and estimated shows the excavation "average" these elements average from unconservative. several for an be the strength stress geometry at elements. have been selected paths the Several plotted from in 20 of the Figure strengths is 8 TSM (refer safety using this to Table 4.5). The Using r esulting the same 29.5 mete rs, some erro r the s tres is strength the s paths as strength does assumes) and depth probably well not the of for computed involved different is factor the final factor in making of the "average" as the strengths. equal factor a of constant safety overestimated. excavation safety is elements In (as for is depth 1.1. 1.6. of Al though extrapolation be cause this for method will other the the be words, Terzaghi full 29.5 so lut ion me ter 110 NORTH ) &cnii 80-' M APPROX. 4LOF CROSS LO T BRACING -i-I 3.25 0 '-RIN 2-1 IK?~ - 6~ 16 Jz54 W" ii I 19.2SM 6 * 6 6 K 6~6 I 9 U~TYTI TI 1-2.N o1 34-75M 3.25 7.01 9.0 1 9.0 1 9.0 17.5 80 3.2 5 6- 15 7 5.5 7-5 t 3.25 1.52 M DIA.CONCRETE FILLED STEEL PIPE PILES 2-5 M DIA.VERTICAL SUPPORT PILES TO DEPTH OF 55 M. (TYP.) PLAN VIEW 50-5 M± , 15M±I , , ZONE A -0 I if -- 10 "*/'-*"jjll1l1j (.4 -25- w a I -40 50 L60 M C/C) 0.4M AUGER HOLES -20 -30 W f (0.7M C/c -ALT 14M AND 25M DEEP HOLES .14- w 15Mt , VZONE A , , ZONE B STABILIZED WITH LIME L -25 ,-* 2 CAST-IN- PLACE CONCRETE PIERS FOR VERTICAL SUPPORT COLUMNS CROSS SECTION X-X PLAN VIEW AND PROFILE OF NAKAGAWA SEWAGE TREATMENT PLANT EXCAVATION - SITE B FIG. 42.1 SOIL )RIVE STEEL PtLE WALL 5TAB i LlZ. - 1 I . , , i I I 1978 C6NCRETEF L' PIER 5 I I I II I 1979 EXCAVATION 6. o -03.5 STAGES -14.0 1980 - I -20.0 M ETERS) -e3.0 1991 SITE I 1990 (ELEVATIONS -rr.0 3.0 - B CONSTRUCTION - 0- 29.5 193 SCHEDULE F IG. 42.2 38 0- ift, 4--7q G07 SAND 350 ~s ~ -V -- 5-04 Wo 2 ti-i; 2ZZ tr g-3 0 .=W 4-1 32 4-0 30 3o 97 '4 4-9 ,7 Ci 4 38 4 'I go 41 SAND a 49 489 28 '3 73 -T - 4U. 37 45 11) 1 4o_ 4) -35' SANDfl Cp sf 493 ,A4 - =L35' .3Z -J 9 44 '9 * I., 4I N '3 I. N .7' 54 44 'I 2 t4- 9e' 0 '4 70 4-3 25 3- 8 95. / '9 * 2 4 5-4 4 0) I" 7 f. '4 C '40 8 3 4- " - 4821 4-7 9+' - 30- 60 2,3 I 30 49' 495 44 V20 50 s'l '7 4ii 497 SILT 50 - "7 G. (-7- "3 5,01 so $1~L I- 23 '9 8 244 33 0 - ^ ALL SOILS: Y-, =- %15-fCM E/,=75) K,=0.5 INITIAL PROFILE AND FINITE ELEMENT MESH 4.I FIG.. * e BACM EXCAVfli 0 9O srAGE /0- - 20 30. 40 60 I 0 II /0 I 20 zs I -I 3o DETAIL OF FINITE ELEMENT MESH 40 IN I I So o ZONE OF EXCAVATION 7o F IG.4.4.2 /0 6/ * 8 6 If tJ z 0 I ~ i~/ a - I 4 4~1 /0 TYPICAL TOTAL STRESS PATHS INITIAL ANALYSIS LINEARLY ELASTIC MODULUS BRACE III FIGAA.3 115 -rMf MP E A uo MIETEKS - -. 9 1c30 21.4 ( T/ 2-2 ST .4 (.3 ST 51 3 2-2 ST 33 3o O - 3- 'A0 44.Z 53 3/ 22 3.6' 22. 55.4 57 3/ Z( 3.2. - 29 22 4. 3 -- . 5) 2-1 ST -35 93 3+.o Z-1 Z- 7AW .s,.e F 2.7 59 0s.5- Z-Z 0/ r.8.Z 2.o 31.3 S W OZ-MH " MW CH -MR CTE-2) 6 - 38 2- (3 40 5 41 3z 20 S 2 ML ML (TE-0 34-'> 4-2.15 Z-Z .15' z-Z _T ST = SHELBY SOIL TkAEE. INDEX 37 Z_ 25 Z-zs*.5 'sZ MOTE: 2IZ SANOy SPAfl>JF PROPERTIES, AND - - - No 'z cL *3( H- roiz'RAlZ CLASSIFICATION TABLE 4.1 r K I I 56 z CH z i 401 -- 7oe i f i eV U oo Z- -0 0 0 CL x /0 _ MH _ o< ML '7 _ - _ _ G 40 m /0 .o 30 4o 50 IJQLUD PLASTICITY a go 70 80 CI0 /00 41/-I7 CHART FIG. 4.4.4 I /5 / /0 z g S- 'ES 5 ~5?- E u 5- 0 /0/5 P P FTL 3 / 4. (C0MWR~E~S 5* 3- 2. -~ T /0 ' Zo STRESS : STRESS Cc1NT ot.LEID j. -'a- e ~7' T5M /v7zs ,~ ' seN') BORt4G Z-2. DEPT" C K,.C(u) 10 MEnERS Zs' PATH TEST TC-1 FI G..4.5 8 1.' /0 /0 ESP CT 5-. 0 0 / 6Z-30 /5 3z.. / 5- Z E S A/oTES 1. SrRsS COOT I.nLET- CiUC (u.) "-3 4 : '4J~ 2. BORIWG ~ 3 DEPTH 19 METERS E ~J) 1.A)0 U 0 V-" ~_ ___ ______S c 5" 20 /0 __ ~ 30 >-5 TEST TC-2 -1-sm STRESS PATH FIG.445b /V s-+ o-( i z I I I- _ [ _ _ _j _ _ _ _ /~ 2. 35 3 U 0~ -3--i z5- t~7I i - -/0 _ C -A TMIJSIOhJ) EvJEr CAIW . 4 STRESS CONTR-kEk> 0I I2 2. 11 3 zG I0 BoRiNG 2-I Ciz. E (u.) DEPTH 34 METEAS ~j Zs5 30 "N P -F St STRESS PATH TEST TE-1 FIG.4.4.5c /0 /0 ______________ - I /0_ ~1 6Z5U) 4- 0 I- 0 __00 pp . 1 5' ' 7 8 25 SA -.5-. __ -/0 _ _ _ _ _ _ _ k) 0 (ExTEInsIL) E V~P.TCA NoTECS.* 7 I. STRLss CoNTRO LLED o- 2. SoBC r-IG 2-) IDEPTH C<LE C.) 28 tAETERS tvc in 3o 5 FIG.445d p STRESS PATH TEST TE-2 Triaxial Test TC-1 TC-2 Depth m 10 19 Fitting Method Pre-Shear log t 0.27 0.03 V log t 0.30 7.1 0.12 3.5 1.4 TE-1 TE-2 74 28 log t logt 1.1 2.0 5.0 4.5 2.1 0.26 0.74 0.26 0.60 0.65 0.85 0.22 0.26 0.33 0.72 1.15 Average Post-Shear 0.15 0.21 3.0 0.08 2.3 1.8 0.06 Average 2.7 5.0 0.07 3.4 1.3 OF COEFFICIENT DATA FROM STRESS 0.55 4.6 1.3 2.0 3.1 0.60 2.8 0-30 2.7 1.3 COEFFICIENT OF CONSOLIDATION CM/sEC x 10 SUMMARY 0.25 -3 OF CONSOLIDATION PATH TESTS TABLE 42 0 TV 4S B840VAIS 7-1, zz,- MIEIA$ iMASO 4V 0 8 aopteW4 oftims 1-13 IT + r32* 6 P2AY - AP :1 U s U..Aw. - TEMT c-TO F/A/E 5/9A/D a. etA K Wp -rPUS 7. - , - A1DI M . SA All) C YEYS whelt& .9 . > WJI' I =.43 I ASSU MED Y*/. 75c g LK 'I) I 01 44 1~- 114 So - i.- LT. GAY F/*-. 4- - -- Y eI.S 7C'f 0 SILT 4.0 19 SAM01 3g.Z2 bp' DG~ - rI'Q L~ 3/uTY CL4 S-54AJD .- ~AJO CY 60 soIL COAJnoafs FA.&tj 4Cl 040o A &)* A'A 04ri $ SPM.G l5CAfE499L Aite4 o lo z6 3a 40 0 20 40 (0 W..ATAX COW-rsr REVISED SOIL PROFILE so s - ,e '- to cs~ *. F IG.44.6 123 boring 22-2 00 0- 10- 20Lu 0-0 .30] -- 0 40- 50Ca-E 60- UU I10 I 0 cmuc- L U CAUE-1 U u S /ow 46 20 su t/ma /oZO46- 30 40 = 5,10,20,&.46 t/mL C 7 UNDRAINED STRENGTH: TRIAXIAL TEST RESULTS VERSUS SAMPLE DEPTH FHG.4.47 124 DEP77 7uST - 7sm /o.zt C/aCU) /0.3+ o.3± /9.4± rsmE 7.1 (AZTER.5) /0.31 a CtA - As 5.7 (75A4) 5.? C/uc-) Lt1L() 3.9 CALUCc') 3.9 cia.c-G2 /*. /f.3 CA Zo.± c I tcL) 43 -3 -/45 0/ 7 93 7.e(, /4. f / 16.9 20 /0.Z ~ /3.7 .51 4.6 22.0 // /4.7 34-3! coquE(u) 6.2 27.5 /3.7S( /8.3 /3.0 Z8.3 /4./ /8. ? I ________ I _________ t ________ /3.7 - ST RAI SUMMARY /A) OF @ .- 27 - .77- 22 .37 ________ EXTRAPoA.ACO FROMl 4 SERI6s OF CoNF/A// AJG PRE.5.5$ ES (SEJE TEXT) o .66 . /0.1 C/l" srREcA-N3. 0 7,EsTs RUA/ AT TC-Z. 8 /6.7 i/., CAWE (k) I Z. > . /0./ 29.3± 35-.3 t 43 - UaC(t) c. 26.4± cC C J-) 7 4 4 -9 TESTS 4T D/FFEREA)- R4TJE OF o.S; /, P.Q. MmotarE SHEAR STRENGTH DATA TABLE4.3 125 3C % 2E 2C q -t/I -(4 IE .) *Ir i0 5 C 0 10 5 15 20 25 30 45 40 35 0 dep+h = 10.00- 1tO1 'm 25 I r-I 2C .- 17 - -_ \u i )- E O 15 10 5 20 25 30 35 40 45 50 / p t tIr L -rc - I at ., Lx I MT stcain cdept1a. % ESTIMATED CONTOURS OF EQUAL STRAIN - S I..9--.o ' COMPRESSION FIG.4418a 126 30 1 1 25- 20[ i ll. i 15 ---- 10 -1 5 0 5 -re- t L 10 bo - i, 15 20 1 p % 3 0 25 30 35 40 bor qK t / dr 45 50 2.-i - It.som deptK z.00 4*. STAa 3C 2C 2C 9 15 47. IC C Ds -% 5 10 15 20 25 p t /'Mz 30 35 40 borvn 45 5 ?.-I de ptK = 35.o o -3S.To -m ESTIMATED CONTOURS OF EQUAL STRAIN - COMPRESSION FIG.4.4.8S ----- 10 TE-2 q TE- 100 t/m2 o -__ 0 5 10 25 20 1S 30 35 t/mO ESTIMATED CONTOURS OF EQUAL STRAIN - EXTENSION FI .48 0- TY LI) w - - F- ,,, CLAYEY SILT ~wfs 1 ~Fis c,7 y x 10 5arn cm/s 10- 20- - CLAYEY SILT with f sand lenss and 4hl Is -3 c = 3 x 10 cm /s 30- rN) 0 40- 50-GANDdSANDYCLAY LAYERS 60 _ i SIXTH EXCAVATION STAGE SIMPLIFIED PROFILE FIGA4.9 ~IS/ODE £XCAVATI O4 Xf 227T 31.3 Z5.( 231 30.9 18.6 7.9 135' Iz.5 f..- 2357 24.8 14.9 5.0 aLi t Ja ag lt 5 I.ss 4.o - 10.6 3.0 9.Z o.9 lc-. - 8.6 01 9.0 o4- 14.3 .24 13.) io. u ulsusrso *Acff -a 915 o.94 69 1(..o 0.17 *3.5 9.4 I.S9 1.1 - -13.o o.-7Z -92 7.8 8.1 11.1 - -1.0 0.ot 29S Z1.8 13.1 4.4- 3.3 ~4.7 -5.S 0.19 IG.4 342 43 Z.I C1 7.7 9.8 8.4 9.8B 1.1 3+4 3(.3 2S . Z -7.3 348 Z3.s 1.4 5.9 &.+ -3.:3 7 r .3Z S'.2- - 3. -5.G 011 11- 29.'5 1. 290 5.9 352 23.3 14.b 4.' 398 43S 24C.1 87 3-1 313 7.3. 7.9 4- l7. 94.1 S.(& 405- -11-0 T.I f7.1 5. r_9 -4.2 3o. 20.4 427 39.3 Z3.4 7.9 - 3.2 -4.o 3.( -Kg. 4 -Z.z 7.7 (-t 4S5 31.3 Z3.( 1.9 r.. 454 435 12. 45'1 34.6 20.4 4(. 74.% .8 .o 2M.3 17.4 488 414I . Zb.3j /2.2 COA4PESSE I±f.1 ISTR.AIS 3.C 0 0O(. 11-4 -7 -- 1. - 4.0 - 1.14 7.8 - -25 0-57 /?.9 .08 -/. o "43 /.SS .?7 -s.i-z.-ooC 455uMEo i. .I 174- - Z9 o.z o.8g 'IS- iZ.o 13.5 -/1 3-. .9 t. 'sl- Z5 -93 45?. *l.o4 -. C4 3.5' +35 -. +3.o -1?.z Z.3C 0.3 0.7 4'o- 70.~ -oS -. 17 7-t 0-c -o4 -6-14 ~o4! -015 0 19 ~3.0 ~014 -0.96 ~.06 7~.oz oz -Z.S -15:1 14-1 ~-~1 - -1.9 -1.9 -K . . /.o -1.4 84 IL o./( --. O3 oO -. f- f -/9.81-0.7 S /2 .64 2 -o4 1~/.7 T;7 0.1:3 Z241 0.43 4SI -Z.9Z ~.Z7 ~-S10 05 -0-s ~ 57 -o -/S -/s- *0.5- -/-1.3 (S ~.5. 2588 ~.1-4 S 1-9 -3oIS' 1-495 .45 '1.-Z ~2.o7 .04. C5 f.i1 -. 47 4.15- -2-34 0o-~5 .4 09S' L4 -o(s o-67 -/ - Z.47 0.G8 416 -17 ~o.t -/.o 3o0 ./39 . -1.! -0-5 3.3 .5 3/7 ~%-z -'os ~03 .59 3S3 -15 :51 7071-.5- -Z./ -0.4 ~.7 IL 7.1Z. -9I. ~12. (, .35 o *Z.7S 4.A l os -Z.3 -0.14 - 6is tor -.o5 07 -oj - .o *-S -4,5~ . LX /Z '_ Z6 i -O..s -0 -s +.2 'I-C.1 '0.S lo-o a -b-ov-o-oa 4 -'1.2 2 23.o O.84 ~0.c, - Z o.4-7o -6. *a.9 Io --. o.o oo 4 +4 + -0.7 o.z 0 .52. 333 ~SC - 0.09s ~0.32. -0.z -0-1 -&.1 - ::8 ~ _? - .63 382. -. 09 -0.4 -os -'s 3 -o- I -0.9 ~~.14 -o-oc-o.of 'I.I -0-77 -- 1.S %.3 9.4 -. 4 -.2-1 -. 0 *.5 -11.Z -o.3 -o. . o.-1 s.5 ~os -7.3 - -o.a. -o.o 1.4 +o.I1 *.3 o -01,5 0.0 -0.o4 -oo o-1 0.4 0.33 -7.v o:72. - - 6.04f '04 4.0 1,S 4.I */.3 - 7.Z 5.9 -15 4.1 1.14 7.8 -2.1 483 35.3 73.6 7.9 0.6-4 -oi 2.9 *0 - - 17. 0 72 181 o8 - .03 2.4 -2- 18 6 .3 4.G -/o-o 1.0 i.5 3.4 1.,R ~3.z o.- ~18.0 - 6.9 -'1i. .44 i.ss- +.a -7.3 -3:3 o .(.5 12.1 o40- -14bo C.5- 1,8a 9.1 49 -130 - 4-o I S-1 410 20.3 12.1 4.1 - -- 0.30 1S.3 1. '.O -1.2 401 63 1.4 6.1c -0.45 ~o.o - ~-7.o 10.1 4,.,' U. B 81 5.0 Z94 194 - Ej CcE V 4LLO ~70 7Z3 1.Z3 o.49 952 f./8 0.09 409 4 ' .17 39U. 1.45 .43 9381 ".47 -4. -7 8 to.- -/.57 *o- .4-3 1/63z .ozr -. 54 #.j. 4o 3333 9- o .- f -1 I.07n -7.07 -. . /g 8 x0(607 -PosTwE SUMMARY OF DETERMINATION OF PARTIALLY DRAINED STRESS STRAIN MODUI i TA BLE 4.4 BZH/MD EXCA9 V47TOA/ Eess fp.,.9. M* /5 288 5.8 '7. /C S (-.7 Zu.9 7o /2. o /9.3 9.3 17.3 /9 34'i ZI i / 0 c /0.8 2 .S o z2.8 7 3( 3.8 7.(p 13.11 Z1.1 9.Z 8.6 C.7 0.41 /3s 44 386 Z-8 ~7.( 3.1 44 ZGS 17.1 .7 y8 41 5(. 38.0 59 IT-o 8. 4S '.o r.o 91 33.. Zo.Z q 7- 27.4 75 2.0 414 24.8 e.3 i-4. /6.4q /zs /3? 43.5 Z./ q-3 /?./ /5b Z13 /7.4 0 - -2. 0 3. -- 3. o-1 4. - 08 o08 /0.7 /.Z .8 o - 0 - 0 Z4 7U4 Cd c1 o 0.04- 0 /44 0 o 0 3 o..3 o 0.01! :4 ~oSZ - 0 702 0 0 0 ) - C o 0 :3 / - *U.6 ~/.o +14 -70 -0.7 0.5- 2C -o. .79 -1/ OSI 3441 /.4 ~. -. ~ 0.s-o 344 s a -. 36 oa-3 c -0.78 -o.78 ,63 .o- 6f - - -6-0 O.Oz 0 -a./ -0.10 0 0 5. / .7- 0.47 o - -2.0 C 0 o - -i.o o-z c, -7.14 -7-14- a - -- 5 -o4 0 -0.38 -08 .4- 5.9 0_ - /0.1 //Z/ 0 o.7 O5 zS 06 - -1-o 6-76 0 ._ - -15.U 0 a -o.-7 0.4 - z 12.5 -0.3C 0/Z 5.0 9.4 0.9. 0 - -10. 0.61 0 /0.o 3.-7 0 0 __- -4.o 0.19 0 5.0 2.0 0.9_ -1.0 -o MerE: o 0 ~e tkEs -. / 1 z - -0.1Z 0 b7 .7(. 6 ti' o '.7S- o -.z5 SOS 4O/4 /.0 '35 OV5~ 25 0+ .o33 0-9S .9.5 1.9 o-So 38. OS-O 30o z7 /-2__ -72 0. -0 3S9 ss- 4 43 S .5 -0.5 "0.8 -. 70 0.83 489 779 3.39 -/97 -O.- "3. Z -/. L Oo .7 -Z.S '/.zf 'Z.4- 7.3/ zS 331 0 ~ 1.4 .32 -3 0. . 0 .0 ~3jo -0/s -o.65 75 ~0 /4 4, ~o.7 - 0 (0 o 3oo -13 -/. 0.0(. o.23 5,5- t.sz 2.45 0 -3.0 - /66 z. os/ .4 /.Z ~o.o6 / f73 Z, S -o.19 -0. Z3 -0.23 -. /0./ 0 0 c1. & _ a o _ 0 400 1/.8 033 a 0.5- 0.6-0 ZC 1.54 5-9~ 4 .4 -(..o 0.7( k.Z5~ -o -3.o // 0., -. 5 o.Sb a - 0 -obx 4 'i.2Y ~4 C o.. - -1.0 -. "o-56 ~o.W 0 388 -zd,4 o4 .iS 0553:s 7. I o.94 4-lb o5' o 05 #61 -4 t0-78 0-So 4-00 6Sb 0. 1. 0 o.us45 0. -~3 -4 Y/.I 0 0 z - 0 0 E, E %fiEN IE44 .46 ~0.15 'o SS 0 -0.4& -. 52 +O-7 0 7 0? -/.35 %cb.5 - /.7f 3.( 0 E., o a c.o 0 . o 0.79 0 0 /.9 . 0 -/44 14- 3.4 a - 0 -3-1 o o .01 -4. C> 0.4 o 42. - ?_ /373'.1( 721 135 5.1 08 c> .o' - C avc E,, 013 -013 o Z C 0.13 #8 z 73 8.i (-.2 0.37 8.7 /5-0 iz-.3 /5.9 /.g 2/8 /3.1 4.4 5-s 11 4.1 Z./ 6 u Avet C1 C- 13-1 6.4' 14- 139 3 /45' -13 A9 e8 /.o lo.1,'-S 4.7 5 - 1.52 -7& 4.3 0.3o Z03 /Z.z +.b 70 Z7g 7.4 /5.1- /4-9 /1.3 /.Sz 1. Z S4 o 4.6 Z.I 4. 4.7 39 97 /3.9 4., 7-/ a. -7 3.7 7./ QissfPorfb r.+ l .4 /1-0 38 /-3 .Z 2.7 ./ 88 3.( Z5 5 /s3 5.1 30 13 ExCE0 AtY *-C /aU "3.15- -6.7S /.57 #0.2 -4 45 -0. -033 £MitoR b'E 7- CapWUT-1A/Or ( 0.55 308 -/(5' 0-5-2 .317 ~o.7f aSo 333 C - /~ -o0S* o-D 300 .RO5 TABLE 44 ork"LI) Cc. ( 0 5t- \0-1 'r"SP FPoA ORACE 22 RSP £S'4 TEO FRop -7Ms P*r T E-2 ~--- TEI 5-1 -0 S.*' t/mri O - w _ 1-0I \0OI - - - 15 eI 27. - 5 10 15 D SUPERPOSITION ON CONTOUR 20 25 30_ __ 35 t/ma OF TOTAL PLOT STRESS OF EQUAL PATH STRAIN F IG.44.10 in TIME 0 ) MONTHS 12 24 I -2 I 4 I I 4 I I I I ~ 4 Lii ___I >~~~~___ 25- 30-- I. I A - DEPTH OF EXCAVATION VS. TIME FIG. 44.11 133 0 ----- 20 40 40 L__ _ _ - 0 -_ _- 0.4 0.5 Time factor T _ __--_ _ -7 0 80 - 100 0 0.1 4.4. 12 a 0.2 0.3 TIME FACTOR VS. 0.6 AVERAGE 0.7 0.8 0.9 DEGREE OF AeY~Iu0 1.0 CONSOLIDATION Ue/uo 0 4.LLA < 42 T= .LC4 7 77E1. 0 po 10 00 0- -0.15 0.40 0P fh - 0.60 -- - 0.848-- 070.90 N 1 Y17 72-& ", '7! 2 0 4.4. 12b 0.1 0.2 0.3 P- f'% , -. XA 0.4 0.5 0.6 0.7 Consolidation ratio U, NORMALIZED DEPTH VS. 0.8 0.9 CONSOLIDATION 1.0 RATIO FIG. 44.12 /E ~W~qVR/N6AT SUPPICF-11V714L LRs FG/9.SA4Em1sU____ k zx 0 =4Z 0.5 0.1 0..4(.4 8 0.2 SLT 1.0 1.5 4 F// 2.0 0 EXCESS 3 . mrro A . L- E XcESS P. fEL. ~ A ,4 Ss5 U, Lk~~ -7.2 19--2F= -I__ _____~~~~~~ 0.2 0.6 04 ____ =\L Z35 = LLTSE~ e 14 .3-i .-. =L -~C 10 aoe o.% Tsm\ L SAYtErs 1.0 0.8 uz NORMALIZED DEPTH VS. CONSOLIDATION RATIO TRIANGULAR INITIAL EXCESS PORE PRESSURE FOR FIG. 44.13 5 -i slr~vss461 4. I 3 '2 V d) -2 'I.) LLi 0 0i ______ 0. -I ______ ______ ______ ov .- 30 S wI -20 -' ;- -/0 I 153- I, E/IoA '-i, //,)ER %SA Tie O56 s / rc 1oT" t6 U.) - P 3 RA-SEn 5 10 z 0. x i I~ , 5 PAXh' Nvo-r.E -4-5- VOLUMETRIC STRAIN VS S.T:WAIj 67ED ___ I DiSsiPAiE DiSSIPATE -&L.(EXCU5S) IVeRrIcA A A.S7PA DISSIPATION +AU, OF PORE (ExCESS). PRESSURE F IG. 44.140 I Zo.0 I')10.0 0.0 4 30-0 40.05 0~ J4 .o 2.0 "3. 0zoo VOLUMETRIC STRAIN VS. LOGARITHMIC DISSIPATION OF PORE /.07 PRESSURE FIG.4.4-14b w TS^ E CAA t, r~t I v Z; Z - "50 r '05- s - TSAI 4-a 450 400 4-00 40oo ooors CONTOURS I- OF MODULI - BRACE III ANALYSIS - REVISED RUN NO. B FIG. 44.15 n I 11 F- ,E 'T T!5^1 ,\\\\\CA 20 35o7-,400 Tsm E 50 TTSA 40 E/000I,~ /=1650 Z -s TSM' 60 CONTOURS OF MODULI - BRACE III ANALYSIS - FINAL RUN C FIG.4416 SCALE METERS 0 0 0 020 DEFORMED FINITE ELEMENT 00 MESH FIG.4.417 w v 0 0 0 0 9S S 0 /2 C0'4 4.- -I SCALE AlErCRS p 0 IV S /0 I I /6 2o zs* SELECTED LINES OF LATERAL DISPLACEMENT F IG. 4.18 0 0 0 0 0 0 76I~ .Is SCA4E 0 5 ,o ^fCTERS /5~ Zo SELECTED LINES OF VERTICAL HEAVE FIG.4419 0 0 0 t+IXAr UM =0 . 3 /7 TsmA MINI MUM = -12. 3835 Tsm CONJTOUR INTERVAL - 0.900 0 I 2( Kil 1( 11r .317 7 7 j _I --- / P7 / OVN SCAA.E I 00 METEkS p I /0 is I I 2:5Z CONTOURS OF SHEAR STRESS FIG. 44.20 C-) MAXITMUM - MTNTMUM - 0 . 235 TSM -96. 860 TSM UONBJR I.NTLRVRL 7. 000 TSM + 5'- /0 o 20 TOTPL SiGMr7 LI is CONTOURS OF TOTAL SIGMA Z F!G.4-21 4D S SC MRXIMUM - e MINTMUM 0.0 00 -rSm TOTRL SIGMAi X - - 74. 760 TSM CONTOUR INTERVAL 5. 000 T-Sm o.co O.0o fr.J .Ls -/-04- Go SCALE i 05 /0 --- AfE7ERS 7 /5. I ZO 25. CONTOURS OF TOTAL SIGMA X FIGA4.22 0 21.500 TSM MH XlJ MUM PORE PHESUPE (LuNjDs-sipATED) +0. 683 TsM MINIMUM CONTOUR INTERVAL = 4. 000 rsM S/0 ! SCA.E zo rs -AIrERS .3 I-' V CU 9 ) CONTOURS SHOWING TRENDS OF NEGATIVE EXCESS PORE PRESSURE FIG.4423 146 5E/7-4kE/xNT ADJACEArr Tco EYcAVAIO/AIS PEC/< (1369) V/S~TAA/CE FROMA AMI/Uf EAcAVrrI/0 DEPin OF rXC4vq7oN/ 0 r IA * V.. PREDICTE D I~1 LQ // BA CE iTI 1z 14) 7z 3 Z =?,>FGUIe aM-l( 4 f.0 Zone I Sand and Soft to Hard Clay Average Workmanship Zone II a) Very Soft to Soft Clay 1) Limited depth of clay below bottom of excavation 2) Significant depth of clay below bottom of excavation but Nb<Ncb b) Settlements affected by construction difficulties Zone III Very Soft to Soft Clay to a significant depth below bottom of excavation and with 5 Nb Ncb COMPARISON BEHIND THE OF PECK'S CHART WITH NAKAGAWA EXCAVATION SETTLEMENT FIG 4424 73RAr'E 77T Z= 317.. STRU7T LOA)S - 57.7 -- , - 40.3 -' +2m. AND 9H DISTR/iBtIOAw (w.I'' 57 T e Av'A .,F (DEP VA 4".' rioA / -) S. L . -8.03 4 I -0 L 'lN ~Thuo 4 -1 ~0 SWAL - 60 S'o 40 ZO /0 0 5T7xE5S r0 /0 30 40 o0 -7r-S-l ESTIMATED TOTAL STRESS DISTRIBUTION THE STEEL PILE WALL BEHIND FIG. 4425 148 L= Length 10 Scuor S cuor (BAL = 1) B/L= 0. 5 8 H 4- 0000,00 e-000", 00011- Strip (B/IL=O) 6 k--B-. 4 0 Factor of Safety = -; CNc y 1 2 -3 4 5 H/B Bottom Heave Analysis for Deep Excavations (H/B >1)B JERRUM & EIDE (1956) B L/ 0.7B7 H + / D H - W 450 0.7 B Factor of Safety 1 H C Nc y- C/0.78 Factor of 1 Safety H CNc - C/0.7D Bottom Heave Analysis for Shallow Excavations (H /B<1)TERZAGHI (1943) BASAL Fr-GuGE FQO M HEAVE CLou44 CISC.WA1Tr C19-1-7) ANALYSIS F IG. 44.26 B iN -50.- T mrmes /7=fe r"+ a -= 1-r 0 r Z r 80 sErRs -- I- 4, MlER ( 114 EXCA-ATlJM -1 VTAGE FtGiTE EME M4ESH . -Aa L- - IA r represe t - - J - 2 iS ... ....- surfoTce - 4 36 -I - .. - .. -- -4 -4 '4 3 G = Ts.*I N -4 544 5" f,9, 1;; A= '37 / .4' N% x C.3 SIXTH EXCAVATION E S. = STAGE - / - c /' ..- c17,8 I /.5 ex .3 . 7 g 1.63 STABILITY ANALYSIS F IG.4.427 - - - DR AlEb 8.EMAVI O v 0 AOWiER $ANJDY LA.CY~e /0 - 4-0. %,TSM 0 2 /O 'ESP f 20T' SOXCA'4A1rof STAGE AStA.Akrr.. FA ItI UP ko.0 AfC7 .-' A.OADiAIC7 /0- PReITAL Ld,5,#/04P SpoE ESITI 10 AL LIoAJ~IuG 2o 30 _ 40 s-- /0 - STRESS PATHS FOR STABILITY ANALYSIS FIG.4+28 FL . D[P77/| ?.-u. g. 34 31.75 /9./ 6.4 38 /2.7 3.9 4o 5.3 .76 43 3.4 z4g U111 au,, 0 0 -3. 5 .0t -3-1 .42 2.6 /o.' 3.6 9. z- 44.o 4J/q P - u. zt .f 6.IT /-3. 0 0 a 0 -/o 0 0 0 0 0 0 //./ Aub, 0-'7 o au, -. 04 -. 04 0 -/1.4- 0 -. /7 -/.4 -. 7 o 0 0 si es 0 / * 3 /30 0 /3- 293 24's 5.0 '3.0 -/2./ o.57 OS - 5-0 41,9 Z.0o -1.0 (-4, 376 /7.(. 295' "'/.? 5. 1 -' . 0 77 /Y19 f/., -.47 0 ^-0 0t 397 4"- 4Z9 34-. C /7.,f 482Z 45t. 253 -510 Z9. 1 97 /70 -7-0 (.8 -4.3 /.' -0.B 4A4k 08 /. *0..6 24.- /04 TZ.A1S JSE0 ,,F - ^AlrE. aR 4,JO , 0 0 -208 0 -27.9 g .laz 0. 0 -3/ *.3/ 0 0 4 0 7.5 -U. I '- 0 718 Ao /'.9 . / -- 0 0 e S=STREA/7)Y MTr C TOAJS &JE ,,V6,-O H E 0- 4o, AVG. 4-078.3 - 33 TABLE 4.5 152 5 CHAPTER SUMMARY AND 5.0 GENERAL Review role of of response, the i s time effect will 0 ften lead to for environmen t Similarly, the safe ty of can be braced thes is excavation, p resents to intende d of effects method the the bet ter pore the also that Element effects of of thi s in a u rban combine the soil pressure pore deformations concern major This of a method the including a pplication Stress obtain a non-linear etc.). areas. by The warrants surrounding app 1 icat ion such movemen ts to of safety dependent time the and are anticipated Method of excavation of movement s can factor an dissipation. one soil func t ion a fo rmulation and pre dict the and Path powerful behavior of Method app roach and consolidat ion. The braced as sumption exc avation that in undrained cohesive soil conditions need not the pore s truc t ures, particularly pressu re shows F inite inc lud ing and tolerated in workers existing magn itude The because the p ublic, deformation s are which with av ailable (general d iss ipat io n. a decreas e that show s that o f excess influencing conclude s writer excavat ions Dissipation major The behavior, the important. t echnology best braced the time. with history case time pressures, in CONCLUSIONS prevail be merely in 153 accepted for lack model partially it illustrated is also be scale need a Method. is 5.1 to a Plant powerful tool, and applied. the problems to on geometries The such Although can as does not Stress the Path Nakagawa the finite element the use it is justified. method as applied of to a simpler One apply method method deformation. program Excavation, be excavation, and complex proposed can complicated element The program BRACE LIMITATIONS One limitation chapter work four not is of that involved. additional that excavation stages stage. execute and through fit the the hand stress strain test (1970) present (refer one can was data. to and s t udy entire for model to o ne must or curv e or all obtained from the Kondner (1963), discuss utilization and of ha ndwork 5 .1 helps it er ated to f or would be stages equation modulus undrained for stress Duncan and of hyperbolic the is of 0 ther stage s hyperbolic initial where; of hand two excavation An 5.2) be in s t ag e of Fi gure performa nce p roc e dure of one only data strain Figure amou nt p red i cted. approach amount al ternat iv e the the pre d ic t to work be to t ime cas e this a polynomial ear lie r stages model for A better the then testing In a significant is compa red performance illustrate proposed there and unreasonable. each the However, tests construction to a major stability for method. conditions less finite However Treatment III for estimate large another drained applied to of Chang the 154 As the although behavior, program could easily be modified. (1) Large finite element computer BRACE III program Stress to a tests although larger can disturbance test BRACE SUGGESTIONS in and (1) difficult stress carefully exe cuted mor e value significantly common than tests laborat ory factors su ch as sample laboratory influenc e significantly make the prop osed compatible are need ed dimension FOR soil area by Osaimi, the program to method ( i.e., ha nd 1 e input of properties) the writer interest of Additional to FURTHER RESEARCH suggestions this a nd expensive Well known III more many varied work the to run expensi ve results. modify Some both more Program modifications and 5.3 of be useage and proper results. several of Tests). also the are may be number UU can analyze path tests (e.g. It such as programs for experience require and run, path (3) proposed method. when using the effectiveness. (2) be aware of several should one a practical matter limitations strain such nonlinear stress capability to model this have does not III however, current version of BRACE The studies applied predicted vs to of deformations ). Such research and include: the actual actual further for type made excavations, performance study by for a Cl ough i. e., (e.g. variety of soil and 155 the ted numerical sophistica broa den hopefully time (2) and our understanding of the updating Evaluation and and method by comp arison the Nakaga wa test s) test data avai lable data and can the of modeling th e an and in and so il BRACE the (Jaworski is el ements node wh ich assum e the h ave limited the III not updated. interaction program. have maintain straight only tw o soil degrees boundaries in There between soil maintained along the and three test program one the two continuum. degrees of of freedom the The freedom cur ve d deformed positions. elements position. of (i.e. 1973). boundar ies between dimensional per BRACE computer sh e e tin g elements elements test ing prediction dimensional wall results. structure c ompatab ility inter-element field incompatability sheeting e lements this From add itional the III in proposed because of to date. s train inherent Displacement role of the additional are needed r ev ised be predict ion using measur ements field Improvement is the with actual site, oedometer input of oth er predictions paper, For (3) technique, of excavation. braced in the appl icability help evaluate conditions would Soil and deformed 156 Develop Brace (4) III program capability nonlinear stress to model strain behavior, perhaps by employing a subroutine which uses a hyperbolic (1963). relationship as proposed by Kondner 5.4 CONCLUSIONS The objective of this thesis was apply a method which includes the This thesis shows that effects of pore deformation in to predict change with time to formulate and one can combine the pressure an excavation. Stress Path Method to obtain soil parameters with the Finite Element Method to perform analysis in a way effect of time includes the on deformation of a braced excavation. approach is outlined in Advantages that of 3 and applied Chapter the approach outlined The in Chapter 4. in Chapter 3 are: (1) Complex nonlinear time analysis (2) The fundamentals of by the engineer as he A few tests avoided. field problem are examined selects his input so that he the problem. retains a feel for (3) the is can be used and extrapolated to cover an entire geometry. The proposed approach application to to for three the For is the example in an iterative procedure. Chapter 4 suggests that The two iterations give a reasonable solution, especially overall deformations. the example case consisting of an excavation in a 157 the clayey silt, effect of time the excavation is significant and on deformations within although not major. the excavation appear to inward wall movements within increase by approximately 10 to Heave 20 percent with consolida- tion. Within the the and the excavation at bottom of depth, the negative excess the 20 to 28 meters) of 20 meter excavation pore pressures due to unloading the positive excess pore pressures due to the dissipation of large negative excess pore pressure resulting heave this pressures due is minimized. particular soil the negative excess pore are offset by the excess pore to excavation pressures generated by surficial dewatering. of time the effects small in this case. of flow, pressure the dewatering In other words, because of for this case. For small net excess pore in a relatively results This shallow or dewatering, substantially offset each other. surficial and (depth of top 8 meters the effect on predicted movement Consequently, are relatively With other soils and other of time on deformations conditions could be con- siderable. In addition, for this shows that particular case the example the undrained heave is the consolidation movements. ving higher factors of contribution of significant. time large when compared to For other situations safety against invol- bottom heave the to total deformation will be more 158 Again, a practical advantage of is the proposed method that such fundamental behavior can be observed and quantified by the engineer during his analysis field situation. of the 159 DRAIMAGpE - - EC, - A:G7G - V T- o ^> Po-AG -io A' - A- ro I *4 8EQTCAL. ClIRVE ) - ACTLA L BEHANJIOR. Ci'J\ E (3) - - FrTS ALL 5TAGES TDE~L-ZEEh ~SEWWIFO APPLLCABLE Mr PREDICMlON er EXCAVATicb OF sTAGE - LSIN9,T+E $AME Motu.e.LU.S FoR- PREi'ou.5 EXCAVA~TON STAGES WLL R ESLLLT 1 MJ AN O\JER-PREtkCTlON OF STR AiN. SIW C, $A tE S CANIT MoO 5TAGES vJiLL RESLUT .US FoR. >EEPER It-)AM UJDER-PREIt 'C-nON OF 5TRAIN MA-GllTUDE. LINEAR VS. NON LINEAR STRESS/STRAIN FIG 51 160 Asymptote = (a 1 - u3)lt 1/b 1 E' = 1/a Ct C4 -4 U.) Hyperbolic Stress-Strain Curve 4 U Trans formed Hyperbolic Stres s-Strain Drve b -4 Axial Strain, E FRoim OSA/4/ /977 HYPERBOL IC STRESS STRAIN CURVES FI G. 5.2 161 LIST OF SYMBOLS a Intercept C Cohesion CAU Anisotropically consolidated triaxial sheared under undrained conditions test CRSC Constant test CAES Center CIU Isotropically sheared under c Coefficient v of K line intercept rate of of ESP Effective stress H Height cut h effective consolidation Engineering stress Study consolidation tangent of on consolidated triaxial test conditions of no drainage Initial e strain for Advanced E. h based modulus path Elevation head Pressure head p h t Total head Hd Length of K Active earth K At rest earth pressure ground surface OCR Overconsolidation P.I. Plasticity P 9 P T 3X 4 path pressure coefficient coefficient, horizontal ratio index ____ S Undrained TSP Total TSP-u0 drainage shear stress Total strength of soil path stress path minus initial pore pressure 162 u Pore pressure u Steady state pore pressure ue Excess pore pressure uD Excess pore pressure due to excavation unloading uE Excess pore pressure due to dewatering UU Unconsolidated undrained wn Water content, natural wy Liquid limit w Plastic limit P z Depth z Depth U to water triaxial test table Consolidation ratio z U Average degree Slope of the K of consolidation line Unit weight Total YT unit weight of soil Unit weight of water Strain E Young's modulus (Ty Total vertical stress (Y '3 o r Total horizontal stress Octahedral stress Vertical a Horizontal y, So, effective stress effective stress Initial total and effective stresses, vertical Initial total and Friction angle, stress effective horizontal stresses friction angle based on effective 163 REFERENCES K.J., Wilson, E.L., Element Analysis, Bathe, Bjerrum, Bjerrum, Clough, and 0, Eide L, Excavations in Numerical Mehtods in Finite Prentice-Hall 1976 (1956). Clay," "Stability Geotechnique of Strutted 1. 6, No. "Earth L., C.J. Clausen, and J.M. Duncan, (1972). Pressures on Flexible Structures - A State-of-theArt Report," Proc. of the Fifth European Conference on Soil Mechanics, Madrid, Vol 2, pp 169-196. G.W., and Davidson, R.R., "Effects of Construction on Geotechnical Performance", Dept. of Civil Engineering, Technical Report No. CE-214, January 1977. Clough, G.W., Duncan, J.M., "Finite Element Analysis of Retaining Wall Behavior", JSMFD, ASCE, Vo. 97, December 1971. Clough, G.W., Clough, G.W., and Schmidt, B, "Design and Performance of Excavations and Tunnels in Soft Clay", Dept. of Civil Engineering, Technical Report No. CE-235, Clough, G.W., Personal Tsui, Y., Communication 1980 "Performance of Tied Back Walls 1977 in Clay ", Paper presented at the National ASCE Meet ing, Cincinnati, Ohio, April, 1974. Cole, K.W., Burland, J.B., "Observations of Retaining Wall Movements Associated With a Large Excavation", Proc. 5th European Conf. on Soil Mech. Foundation Engineering,_Madrid 1972 Corbet, and "A Load Bearing B.O., Davies, R.V., Langford, A.D ., Diaphragm Wall at Kensington and Chelsea Town Hall at London", Proc. Diaphragm Wall s and Anchorages, Inst. of Civil Eng., London, 197 5. "Effects of Foundation D'Appolo nia, David J., (1971). Construction on Nearby Structures," Pan American Conference on Soil Mechanics and Foundations, Puerto Rico, pp. 189-236. Introduction to the Finite Element Desai, C.S., Abel, J.F., Method, Van-Nostrand-Reinhold, " Design Manual DM-7" Department of the Navy (1971). Navfac Naval Facilities Engineering Command, Washington, D.C. 164 Davis, E.H., and Christian, J.T. (1971), "Bearing Capacity of Anisotropic Cohesive Soil", ASCE, JSMFD, Vol. 97, Sm5,pp. 753-769. J.M. and Chang, C-Y.,"Nonlinear Analysis of Stress and Strain in Soils", JSMFD, ASCE, No.- SM5, Vol. 96, 1970. Duncan, J.M., and Chang, C-y., "Analysis of Soil Movement Around a Deep Excavation", JSMFD, ASCE, No. SM5, Sept. 1970. Duncan, "Earth Pressure DiBiagio, E., and L. Bjerrum (1957). Measurements in a Trench Excavated in Stiff Marine Clay," Proc. 4th Int. Conf. on Soil Mech. and Found. Eng., London, 2, pp. 196-202. DiBiagio, E., Roti, J.A. "Earth Pressure Measurements on a Braced Sherry Wall in Soft Clay, Proc._5th European Conf. Soil Mech. Found. Eng., Madrid 1972 Henkel, D.J., "Geotechnical Considerations of Lateral Stresses", State-of-the-Art Paper, presented at the Specialty Conference on Lateral Stresses in the Ground and Design of Earth Retaining Structures, ASCE, Cornell Univ. N.Y., June 22-24, 1970 Jaworski, Walter E., An Evaluation of the Performance of a Braced Excavation, Phd Thesis, M.I.T., June 1973 Kondner, R.L.,(1963), "Hyperbolic Stress Strain Response Cohesive Soils," JSMFD, ASCE,VOL.89, No. SMI. Ladd, C.C., (1973), "Estimating Settlements of Structures Supported on Cohesive Soils", MIT Class Handout. Ladd, C.C.. (1971), "Strength Parameters and Stress Strain Parameters of Saturated Clays", MIT Class Handout. Ladd, C.C. Wissa, A.E.Z. "Geology and Eng. Properties of Conn. Valley varved Clays with Special Reference to Embankment Construction", Dept. Civil Eng. Report R-70-56 Lambe, T.W., Wolfskill, L.A., and Wong, I.H., "Measured Performance of Braced Excavation," Journal of Soil Mechanics and Foundations Division, ASCE, Vol. 96, May 1970, pp. 817-836. Lambe, T.W., and Whitman, Soil Mechanics, New York, 1969. Wiley & Sons, 165 T.W., "Interpretation of Field Data", paper from Proc. of Lecture Series in Observational Methods in Soil and Rock Engineering, University of Illinois, pp. Lambe, 1970. 116-148, Dec. Lambe, T.W., "Predictions in Soil Engineering", 13th Rawkine Lecture, Geotechnique 23, No. 2, 149-202. 1973. Lambe, "Braced Excavations," ASCE Conference T.W., (1970). on Lateral Stresses in the Ground and Design of Earth-Retaining Structures, pp. 149-218. Lambe, "The Behavior of Foundations During T.W. (1968). Construction", JSMFD, ASCE Vol. 94, No. SM1, pp 93. Vol. 93, Lambe, Lambe, T.W., No. "The SM6, T.W., Marr, Stress Path Proc. Paper W.A. "The Method", JSMFD, ASCE, 5613, Nov. 1967. Stress Edition" JGED, ASCE, Vol. June M.I.T., Path 105, Method, No. Second GT6 pp. 727, 1979 Dept of Civil Engineering, "M.I.T. Test Instrumentation MBTA Haymarket - North Project" Mass -MTD-2, March 1972. Mitchell, J.K., ment of Section Extension and W.S. Gardner(1975), "In-Situ MeasureVolume Change Characteristics,6th PSC, ASCE,pp. 379-391. Peck, Hansen, and Thornburn, Foundation Engineering , Wiley, 1974. Osaimi, A.E. and G.W. Clough (1979) "Pore-Pressure Dissipation During Excavation, Proc. of ASCE, Vol. Osaimi, 105, No. GT4, A.E., "Finite Element Analysis of Time Dependent Deformations and Pore Pressures in Excavations and Embankments" Phd Thesis, Stanford University Dept. of Civil Engineering Palmer, 1977. "Analytical Study of J.H. Laverne, and Kenney, T.C. a Braced Excavation in Weak Clay" Can. Geotechnical Journal Vol. Peck, JGED pp. 481-499. 9, No. 2 pp. 145-164 May 1972. "Deep Excavations and Tunnelling in Ralph B., (1969). Soft Ground," State-of-the-Art Volume, Seventh International Conference on Soil Mechanics and Foundation Engineering, Mexico City, pp. 259-281. 166 Ries, the of Carol, Predicting Lateral Earth Pressures for Design of Tie-Back Retaining Walls',' Master Science Thesis, M.T.T. 1974. Skempton, A.W. Slip: "The Bradwell and P. LaRochelle, (1965). A Short Term Failure in London Clay" Geotechnique, No. Taylor, 15 pp. 222-242. R.L. and Brown, C.B., "Darcy Flow Solutions With Free Surface, "Journal of the Hydraulics D iv is ion ASCE, 93, Vol. No. HYZ, pp. 25-33, Mechanics, 1967. John Wiley Terzaghi, K., Theoretical Soil Sons, New York 1942. Terzaghi, Soil Mechanics K. and R.B. Peck (1967). and Sons, New Wiley Practice, Engineering and in York. Foundations, _ Retaining Tschebotarioff, Gregory P., (1973). Walls and Earth Structures, McGraw Hill, New York. Wong, I.H., Analysis M.I.T. 1971 Zienkiewicz, O.C., of Braced Cheung, Excavations, Y.K., The Finite Phd. Thesis, Element Method in Structural and ContinuTm~Hicnics,~Ion~on, McGraw-Hill Publishing Co., Ltd 1967. 167 APPENDIX A GRAINSIZE CONSOLIDATION PLOTS AND PLOTS - SQUARE ROOT NAKAGAWA SOIL OF TIME SPECIMENS IN. 2 100 - IIN.3/41N.1/2 N. - - U.S. STANDARD SIEVE SIZE NO.4 NQ20 NQIO - NQ 40 NQ.6 NO.OO NO. 200 - 90 - ----.-.-.-.-.- ---...-.- so . - . _ - - _ __ - _ -~- I ___ -.-- - - -........._ -- -_ _ I -__TI -_ - -I- -U T0 - - .-- 60 - - - - -- - - z -I 50 - 40 - - - - -I -- - -I - - --- E .- - _ - t0 0 10 100 1.0 SIZE IN GRAIN m{ - _ 20 4 G)C m - - -. 30 mmm>0 j -- -- > CDBLESC GRAVEL 0 COARSE IE UNIFIED TEST NO, sYM L-1 S-I 0 Tokyo, 0.001 SILT OR CLAY MEDIUM FINE SOIL CLASSIFICATION Japan i SYSTEM MATERIAL SOURCE SOURC - 0.01 SAND I ICOARSE1 0.1 MILLIMETERS REMARKS I lakaiaga. Treatment Plant I,te 13 . -. F6. A- IN. 3/41N.1/2 I l l--- 2 IN. 100 - 90 U.S. STANDARD SIEVE SIZE NO.4 NQ.20 RQ.4OfQ6ON.IOO NO.20 N .UO -I i IN. - I - 1 t~-- - I--- so T -- T r - -I -I- 1 -T~ I - - _ T - - I TO - _- -_ - I 60 50 0 x ~ 40 q r -4 I _I-I _ ~ - -- ~ -I ---- --------- F~ -I --- 30 - I- - _ - 20 I O 10 XI -3 <0 _j(flW -- m 0 - 100 10 GRAIN 1.0 SIZE IN 0.1 0.01 0.001 MILLIMETERS 90 SAND GRAVEL CDBLES m z >0 SILT OR CLAY FINE COARSE COARSE UNIFIED z TEST SYM. I N-2 0 A MEDIUM FINE SOIL CLASSIFICATION SYSTEM MATERIAL SOURCE Tokyo, Japan REMARKS I I Hakagawa Troatment Plant 2ite B FIG. A.Z U.S. STANDARD SIEVE SIZE I IN. 34IN.1/2 IN. NO.4 NAI0 k.20 2 IN. 100 I ----90 --- so Io - - - - T - - -- a- - - T - _ _ - - - - T a-a -- T rf - - - 0 NO.40 NO.60 NO.100 O.200 -- - - - I- -- - -- _- 60 so - - - mt - - -- - -- 40 1 ' 1 3D g--- - F' z -- -a C 20 I j II I I ______- 10 ci -X (n CD m :4 I0 100 0.1 1.0 GRAIN SIZE IN OBBLES z -> 01X 0 CO EA UNIFIED > TEST NO. 0-3 H-3 SYM. ___ MEDIUM 0 REMARKS ________ Japan CLAY SYSTEM MATERIAL SOURCE Tokyo, OR FINE SOIL CLASSIFICATION ____________ A SILT SAND GRAVEL COARSE COARS 0.001 0.01 MILLIMETERS _ Hakagawa Treatment Plant Site B - _ F/6. A.3 U.S. STANDARD SIEVE SIZE 4 Ni0 .N12I O IN .3'4!Nf/2 .N f./ 1N . 100 90 ---- N -T- - -T 0440 NO63NO.lOO 00N.0 m. O 0O O0 - 90 I V f"u Al 1 i -- -I 70 .1 60 so -- ~ I ~ -- --- A - -F- -- 50 - 40 - - - -F ~ - 30 -- 20 - - - -- - - rrI -IOV)>W to - y 0 09LE - C 0 SIZE IN GRAIN z0 C GRAVEL 00LSCOARSE FINE COARSEI UNIFIED TEST NO. SYM. - 11-4 A Tokyo, MILLIMETERS SAND SILT OR MEDU Japan CLAY FINE SOIL CLASSIFICATION MATERIAL SOURCE 0.001 0.01 0.1 .0 10 100 z 00 SYSTEM REMARKS 1Jakarawa Treatment Plant B : itr 6/G. A.4 U.S. STANDARD SIEVE SIZE NO.4 NQ.20 N .10 IN.3/4 IN.1/2 I2f IN. t00 IN. NQ40NO.60NO.100 ON.200 90 90 I TO -4 - 60 - --- - - - - - - i -- - - T TV1 ___ - - - - - - - --- - - - - .- - -- I - - --- - --- - - - - - TI I so z - - - 30 I - - - I - - - - - -. -- - -l - - - - - I - -'- ~ - -~-~ I I ___- I - -- .-- - 1'0 -- acn w rG m z to 0 too 10 GRAIN 1.0 SIZE IN 0.1 0.001 0.01 MILLIMETERS SAND GRAVEL x11 -3 - - -- -I 20 ;u I 40 -- -4 - I-I v"(i UNIFIED TEST S-5 -5 SOIL CLASSIFICATION SYM MATERIAL SOURCE 0 Tokyo, Japan A SYSTEM REMARKS lakagrawa Tratment Plant :"I t f B f16.A.s IIN.3'4IN./2 N. 2IN. U.S. STANDARD SIEVE SIZE NO.4 Np20 NQ40NQ6ONO.IOONO.2O NPO I ITII I 90 - I -....... __ _ _ I -- - . . -- - --- _ 0 TO I T 2 z1 I 60 i I i ii I 1T -_ ~ I-- ~ . . . . . 50 I 40 - I - -I - - L - - - - t - - ~ ------ _ -i~-- I.-- . _ ._ 30 0 0, > I - -. - - i- - - 20 - - - - - - -- 22 10 c2 < uT G) -1 n 0 10 t00 Z GRAIN in~I > GRAVEL COARSE TEST P SYM. NO. L-6s- 6 COARSE MEDIUM 0.001 0.01 FINE SOIL CLASSIFICATION MATERIAL SOURCE ______________ 0 0.1 SAND FINE UNIFIED r -icn 1.0 SIZE IN MILLIMETERS Tokyo, A Japan SYSTEM REMARKS Hakagawa Treatment Plant Site B F /6. A.6 0 S 0 0 YE - /7a 40 P1W -s#i~w~ / I. £~ ~.~0 - 'o .44 )*.05 /AIO At tJ. '.9. 1.40 -dc, 1.' A"a z*20 1.00 /CA * -Is -3 is f6(.1- A.oo aa -- ga - .z4 144> Iz /MC- so 4 4 * S Il -6 t i.0 ' .1 - 12- ' ( 9-1.3b) - I37 d,., -3- /A/: .. oo' (. 1 1 1- & 7 a 0-lo P 3 4 r fe -1 Q A 7 F/G, A.7 z1.2o 1'tj 00 0 0 S 0 / - ez 1 0 /ACRl Jcso - / .z-.-as) ( Po0-S SHEAR IAIca-7- 0 To .8- 0 .3 eiI- -^A=. (.-i .3 -L I.1t (J 90 0. t.> -4 U, 0.950 S4 7 4 W - -dd V . 7 o~sc) 6- s 1.00 a ~ / * 4 4- 1' 79 4L 0.10 160 - 10 .ao * ...- (~r-.8~ J4 ID" 9 7 U 0.$d4 0,80 o {o 0.40 - "'^ .&" ^8'- . 'o 0.50 .5AI. S 1 J .4 r- ' 7 . 8 *1 z 6.= Z.3 + * . -A.5 s 4 7i F/G. A, to 0 0 0 0 0 -n-zPRIE0.11 0*".( U iii ~ IAACR Jc, U - J. SHEA P 1IA/CR - 2 0,90 4,L* .:zo A'"s I UJ /,30 \ -~ 1.10 0 1-09 = -1 I /.70 Z. / I. su C311 I, / Z 3 5 6~~ MI/ Ift,1 al .3.13 .2 4.~/C. 100(2 ,7i (P ,4_ jA, 7 ' I.. I O/*~ *~~/J 1 ~ 16 I, pal I C,., * '-4 C'7'7 aoc "0, - C' CC~ C' 0*'c' ~CW7 eL '' L A - t, -. ,,-p~0 Sa q, (s o &VHg JISC~d 2-XL- 9 L 01 0 'T0 TC-/ /.(.o I / N.CR- - / S 0 PE- SYEAR fmAcR -2 l-za /10 /.2 V A20 /4b - Q - A c-o= 10 17 0.40 2.0 Q -o.L 2./. V : t 01 Z.3. / ~ 3 'f 5- 1 4 0 ~iI.sf4rES v.~ir-S 0 100 4. - o% (, -OIL); - . o 100 Fla.A- u 0 0 S n 0 TC-/ ogl -2 4, POST SHC-EqP .+ -. O oz.. Iv'+Is- 000 - -L T 1 -/4 - A6 d T(Un. $ /5~ /0 Le 7.5 30 35 t= .- 54 -4a ,A Ul le A"CR - ---- 4 Nr =i -L too 1,- o043 c.ZO -0.46 S.AG a0 -- ~~~>0 1S Z'~ 40 PA IP-JLdW~ 4 '' .5' s- 4." IZ-1 M14. 0 0 0 0 0 0 2/IA/C 0. 1, C z PRE - SHtR. - Z. db:(..(.--.iNC=..--I -- V - 14 1. 4- 040) I.J. ./......V C...R 0.40 --d - o.'0o ~(~ .Z) .c 0.4. '4ILL . oto- .0 Q 0. 10 /~VCJ(~ IICA- oIF A540 2. . /100 . /, C F/C)I- i -s 0 0 0 7 S T-C- Z o eo L) 0 /A/CR -/ .. g - /CR -*3 P0,5T 5HE~Qg -0 .sc. S - ,~1- '.4 /ZD 00' 0 /.70 Q - So /90 1.YO \z 3 'f~ * 71 q } i 30 4 J- .- ~------~--.- F16. A if I 182 APPENDIX VERTICAL EFFECTIVE STRESS B VERSUS DEPTH - NAKAGAWA 183 0- I0-L uh r 20- i LU LU 307 LU N 40+ 500 10 20 40 30 TSM NAKAGAWA VERTICAL EFFECTIVE STRESS VS. DEPTH FIG.B.I