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Portland State University Portland State University PDXScholar PDXScholar Dissertations and Theses Dissertations and Theses 11-4-1994 Two Dimensional Finite Element Modeling of Swift Two Dimensional Finite Element Modeling of Swift Delta Soil Nail Wall by "ABAQUS" Delta Soil Nail Wall by "ABAQUS" Richard James Barrows Portland State University Follow this and additional works at: https://pdxscholar.library.pdx.edu/open_access_etds Part of the Civil Engineering Commons Let us know how access to this document benefits you. Recommended Citation Recommended Citation Barrows, Richard James, "Two Dimensional Finite Element Modeling of Swift Delta Soil Nail Wall by "ABAQUS"" (1994). Dissertations and Theses. Paper 4741. https://doi.org/10.15760/etd.6625 This Thesis is brought to you for free and open access. It has been accepted for inclusion in Dissertations and Theses by an authorized administrator of PDXScholar. Please contact us if we can make this document more accessible: [email protected].

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Page 1: Two Dimensional Finite Element Modeling of Swift Delta

Portland State University Portland State University

PDXScholar PDXScholar

Dissertations and Theses Dissertations and Theses

11-4-1994

Two Dimensional Finite Element Modeling of Swift Two Dimensional Finite Element Modeling of Swift

Delta Soil Nail Wall by "ABAQUS" Delta Soil Nail Wall by "ABAQUS"

Richard James Barrows Portland State University

Follow this and additional works at: https://pdxscholar.library.pdx.edu/open_access_etds

Part of the Civil Engineering Commons

Let us know how access to this document benefits you.

Recommended Citation Recommended Citation Barrows, Richard James, "Two Dimensional Finite Element Modeling of Swift Delta Soil Nail Wall by "ABAQUS"" (1994). Dissertations and Theses. Paper 4741. https://doi.org/10.15760/etd.6625

This Thesis is brought to you for free and open access. It has been accepted for inclusion in Dissertations and Theses by an authorized administrator of PDXScholar. Please contact us if we can make this document more accessible: [email protected].

Page 2: Two Dimensional Finite Element Modeling of Swift Delta

THESIS APPROVAL

The abstract and thesis of Richard James Barrows for the Master of Science in Civil Engineering were presented November 4, 1994, and accepted by it~e th.esis committee and the

department.

COMMITTEE APPROVALS: Tr~dr D. smith, Chair

MScott Burns Graduate Of - ·

DEPARTMENT APPROVAL:

************************************************************

ACCEPTED FOR PORTLAND STATE UNIVERSITY BY THE LIBRARY

b onlt1 cZ:wuc~~ /9?5

Page 3: Two Dimensional Finite Element Modeling of Swift Delta

ABSTRACT

An abstract of the thesis of Richard James Barrows for the

Master of Science in Civil Engineering presented November 4,

1994.

Title: Two Dimensional Finite Element Modeling of Swift Delta

Soil Nail Wall By "ABAQUS"

Soil nail walls are a form of mechanical earth

stabilization for cut situations. They consist of the

introduction of passive inclusions (nails) into soil cut

lifts. These nailed lifts are then tied together with a

structural facing (usually shotcrete) . The wall lifts are

constructed incrementally from the top of cut down. Soil nail

walls are being recognized as having potential for large cost

savings over other alternatives.

The increasing need to provide high capacity roadways in

restricted rights of way under structures such as bridges will

require increasing use of techniques such as combined soil

nail and piling walls. The Swift Delta Soil Nail wall

required installing nails between some of the existing pipe

piling on the Oregon Slough Bridge. This raised questions of

whether the piling would undergo internal stress changes due

to the nail wall construction. Thus, it was considered

\

Page 4: Two Dimensional Finite Element Modeling of Swift Delta

2

necessary to understand the soil nail wall structure

interaction in relation to the existing pile supported

abutment.

The purpose of this study was to investigate the Swift

Delta Wall using finite element (FE) modeling techniques.

Valuable data were available from the instrumentation of the

swift Delta Wall. These data were compared with the results

of the FE modeling. This study attempts to answer the

following two questions:

1. Is there potential for the introduction of new bending

stresses to the existing piling?

2. Is the soil nail wall system influenced by the presence

of the piling?

A general purpose FE code called ABAQUS was used to

perform both linear and non-linear analyses. The analyses

showed that the piling definitely underwent some stress

changes. In addition they also indicated that piling

influence resulted in lower nail stresses. Comparison of

measured data to predicted behavior showed good agreement in

wall face deflection but inconsistent agreement in nail

stresses. This demonstrated the difficulty of modeling a soil

nail due to the many variables resulting from nail

installation.

Page 5: Two Dimensional Finite Element Modeling of Swift Delta

TWO DIMENSIONAL FINITE ELEMENT MODELING OF SWIFT DELTA SOIL NAIL WALL BY "ABAQUS"

by

Richard James Barrows

A thesis submitted in partial fulfillment of the requirements for the degree of

MASTER OF SCIENCE in

CIVIL ENGINEERING

Portland State University 1994

Page 6: Two Dimensional Finite Element Modeling of Swift Delta

ii

THESIS APPROVAL

The abstract and thesis of Richard James Barrows for the Master of Science in Civil Engineering were presented November 4, 1994, and accepted by the thesis committee and the department.

COMMITTEE APPROVALS: Trevor D. Smith, Chair

Matthew Mabey

Scott Burns Graduate Office Representative

DEPARTMENT APPROVAL: Franz Rad

************************************************************

ACCEPTED FOR PORTLAND STATE UNIVERSITY BY THE LIBRARY

by on ~~~~~~~~~~~~~

Page 7: Two Dimensional Finite Element Modeling of Swift Delta

iii

TABLE OF CONTENTS

LIST OF TABLE5 .. · · v

FIGURES vi

APPENDICES viii

INTRODUCTION 1

SWIFT BOULEVARD DELTA PARK INTERCHANGE SOIL NAIL WALL . 4 Project Scope . . . . . . . . . . . . . . . . . . 4 Construction . . . . . . . . . . . . . . . . . . . 6 Construction Problem Areas . . . . . . . . . . . . 7

INSTRUMENTATION .

SOIL TESTING Laboratory Soils Testing At Swift Delta Insitu Testing At Swift Delta . . . .

12

21 21 24

TWO DIMENSIONAL FINITE ELEMENT MODELING . . . . . . . . 29 ABAQUS . . . . . . . . . . . . . . . . . . . . . . . 2 9 PATRAN . . . . . . . . . . . . . . . . . . . . . . 3 0 Finite Element Mesh Development . . . . . . . . . 30 1 ksf Line Load Validation . . . . . . . . . . . . 32

PLANE STRAIN MODELING . . . . . . . . . . . . Fringe Plot Scaling . . . . . . . . . Geostatic Turn On . . . . . . . . . . Incremental Modeling . . . . . . . . . .

NON LINEAR PLANE STRAIN ANALYSIS Introduction . . .

38 41 42 42

58 58

RESULTS INTERPRETATION . . . . . . . . . . . . . . . . 62 Interpretation of Instrument Section #2 Results . 62 Horizontal Soil Stresses . . . . . . . . . . . . . 62 Vertical Soil Stresses . . . . . . . . . . . . . . - 62 Nail Stresses . . . . . . . . . . . . . . . . . . 63 Def le ct ions . . . . . . . . . . . . . . . . . . . 6 3 Section #1 Results . . . . . . . . . . . . . . . . 75 Horizontal Soil Stress . . . . . . . . . . . . . . 75 Vertical Stresses . . . . . . . . . . . . . . . . 76 Nail Stresses . . . . . . . . . . . . . . . . . . 76 Pile stresses . . . . . . . . . . . . . . . . . . 78 Deflections . . . . . . . . . . . . . . . . . . . 78

Page 8: Two Dimensional Finite Element Modeling of Swift Delta

COMPARISON BETWEEN MEASUREMENTS . .

FEM RESULTS

Deflections . . . . . Measured Nail Stresses . .

CONCLUSIONS AND FURTHER STUDY .

APPENDICES . . . . . . . .

AND INSTRUMENT

iv

80 80 82

128

131

Page 9: Two Dimensional Finite Element Modeling of Swift Delta

v

LIST OF TABLES

TABLE I: Construction Equipment . . . . . . . . . . . . 8 TABLE II: Triaxial Test Results . . . . . . . . . . . . 22 TABLE III: Triaxial Test Results . . . . . . . . . . . 23 TABLE IV: Summary of Pressuremeter Test Results . . . . 25 TABLE V: Model Material Properties . . . . . . . . . . 60

Page 10: Two Dimensional Finite Element Modeling of Swift Delta

vi

LIST of FIGURES FIGURE 1: Location and Wall Plan . . . . . . . . . . . 10 FIGURE 2: Developed Elevation View. . . . . . . . . 11 FIGURE 3: Instrument Section #1 Cross Section . . . . . 14 FIGURE 4: Instrument Section #2 Cross Section . . . . . 15 FIGURE 5: Instrument Section #1 Nail Load Plots . . . . 16 FIGURE 6: Instrument Section #2 Nail Load Plots . . . . 17 FIGURE 7: Pile Cap Extensometer Plot . . . . . . . . . 18 FIGURE 8: SD 129 Slope Inclinometer Plot . . . . . . . 19 FIGURE 9: SD 130 Slope Inclinometer Plot . . . . . . . 20 FIGURE 10: EX Probe Pressuremeter Test Results . . . . 26 FIGURE 11: BX Probe Pressuremeter Test Results . . . . 27 FIGURE 12: Pressuremeter Test Results Summary . . . . . 28 FIGURE 13: 1 ksf Line Load Vertical Stress . . . . . . 34 FIGURE 14: Finite Element Mesh Instrument Section #1 . 35 FIGURE 15: Finite Element Mesh Instrument Section #2 . 36 FIGURE 16: 1 ksf Line Load Horizontal stress . . . . . 37 FIGURE 17: LINlN Geostatic Turn On Model Step 2 Horiz.

Stress . . . . . . . . . . . . . . . . . . . . 4 4 FIGURE 18: LINlN Model Step 3 . . . . . . . . . . . . . 45 FIGURE 19: LINlN Model Step 4 . . . . . . . . . . . . . 46 FIGURE 20: LINlN Model Step 5 . . . . . . . . . . . . . 47 FIGURE 21: LINlN Model Step 6 . . . . . . . . . . . . . 48 FIGURE 22: LINlN Model Step 8 . . . . . . . . . . . . . 49 FIGURE 23: LINlN Model Step 9 . . . . . . . . . . . . . 50 FIGURE 24: LINlN Model Step 3 . . . . . . . . . . . . . 51 FIGURE 25: LINlN Model Step 4 . . . . . . . . . . . . . 52 FIGURE 26: LINlN Model Step 5 Major Stress . . . . . . 53 FIGURE 27: Model Step 6 Major Stress . . . . . . . . . 54 FIGURE 28: LINlN Model Step 7 Major Stress . . . . . . 55 FIGURE 29: NOLINlN Step 8 Major Stress . . . . . . . . 56 FIGURE 30: LINlN Model Step 9 Major Stress . . . . . . 57 FIGURE 31: NOLIN2N Model Step 3 Horiz Stress . . . . . 64 FIGURE 32: Model NOLIN2N Static Step 5 Horiz. Stress . 65 FIGURE 33: Model NOLIN2N Static Step 8 Horiz. Stress . 66 FIGURE 34: Model LIN2N Static Step 3 Vert. Stress . . . 67 FIGURE 35: Model NOLIN2N Static Step 5 Vert. Stress . . 68 FIGURE 36: Model NOLIN2N Static Step 8 Vert. Stress . . 69 FIGURE 37: Model NOLIN2N Static Step 3 Major Stress . . 70 FIGURE 38: Model NOLIN2N Static Step 5 Major Stress . . 71 FIGURE 39: Model NOLIN2N Static Step 8 Major Stress . . 72 FIGURE 40: Model NOLIN2N Static Step 8 Horiz. Strain . 73 FIGURE 41: Model NOLIN2N Static Step 8 Vert. Disp. . . 74 FIGURE 42: Model NOLIN2N static Step 8 Horiz. Disp. . . 84 FIGURE 43: Model NOLINlN Static Step 3 Horiz. Stress . 85 FIGURE 44: Model NOLINlP Static Step 4 Horiz. Stress . 86 FIGURE 45: Model NOLINlN Static Step 5 Horiz. Stress . 87 FIGURE 46: Model NOLINlP Static Step 6 Horiz. Stress . 88 FIGURE 47: Model NOLINlP Static Step 9 Horiz. Stress . 89 FIGURE 48: NOLINlN Model Static Step 8 Horiz. Stress . 90 FIGURE 49: Model NOLINlP Static Step 8 Vert. Stress . . 91

Page 11: Two Dimensional Finite Element Modeling of Swift Delta

vii

FIGURE 50: Model NOLINlP Static Step 5 Vert. Stress . . 92 FIGURE 51: Model NOLINlP Static Step 6 Vert. Stress . . 93 FIGURE 52: Model NOLINlP Static Step 7 Vert. Stress . . 94 FIGURE 53: Model NOLINlP Static Step 9 Vert. Stress . . 95 FIGURE 54: Model NONLINlN Static Step 3 Vert. Stress . 96 FIGURE 55: Model NONLINlN Static Step 5 Vert. Stress . 97 FIGURE 56: NONLINlN Model Step 8 Vert Stress . . . . . 98 FIGURE 57: Model NONLINlN Static Step 3 Major Stress . 99 FIGURE 58: Model NONLINlP Static Step 4 Major Stress 100 FIGURE 59: Model NONLINlP Static Step 7 Major Stress 101 FIGURE 60: Model NONLINlN Static Step 6 Major Stress 102 FIGURE 61: Model NONLINlP Static Step 9 Major Stress 103 FIGURE 62: Model NONLINlP Static Step 8 Major Stress 104 FIGURE 63: Model NONLINlP Static Step 3 Major Stress 105 FIGURE 64: Model NONLINlP Static Step 4 Major Stress 106 FIGURE 65: Model NONLINlP Static Step 6 Major Stress 107 FIGURE 66: Soil Excavation Lift Displacement . . . . 108 FIGURE 67: NONLINl Wall Face Deflection . . . . . . . 109 FIGURE 68: NONLINlP Wall Face Deflection . . . . . . 110 FIGURE 69: Model NONLINlP Step 8 Horiz. Disp. . . . . 111 FIGURE 70: Model NONLINlP Step 7 Horiz. Disp. . . . . 112 FIGURE 71: Instrument Section 1 Row 1 and 2 Nail Loads 113 FIGURE 72: Instrument Section 1 Row 3 and 4 Nail Loads 114 FIGURE 73: Instrument Section 1 Row 5 Nail Loads . . 115 FIGURE 74: Instrument Section 2 Row 1 And 2 Nail Loads 116 FIGURE 75: Instrument Section 2 Row 3 And 4 Nail Loads 117 FIGURE 76: Instrument Section 2 Row 5 Nail Loads . . 118 FIGURE 77: NONLINlN Nail 1 and 2 Stresses . . . . . . 119 FIGURE 78: NONLINlN Nail 3 and 4 Stresses . . . . . . 120 FIGURE 79: NONLINlN Nail 5 Stress . . . . . . . . . . 121 FIGURE 80: NONLINlP Nail 1 And 2 Stresses . . . . . . 122 FIGURE 81: NONLINlP Nail 3 And 4 Stresses . . . . . . 123 FIGURE 82: NONLINlP Nail 5 And 4 Stresses . . . . . . 124 FIGURE 83: NONLIN2N Nail 1 And 2 Stresses . . . . . . 125 FIGURE 84: NONLIN2N Nail 3 And 4 Stresses . . . . . . 126 FIGURE 85: NONLIN2N Nail 5 . . . . . . . . . . . . . 127 FIGURE 86: Measured and Predicted Wall Face Deflection 130

Page 12: Two Dimensional Finite Element Modeling of Swift Delta

APPENDICES

APPENDIX A: INSTRUMENTATION . . . . . . . . APPENDIX B: NOLINlP INPUT FILE ... APPENDIX C: LINEAR ELASTIC PATRAN PLOTS . APPENDIX D: NON-LINEAR PATRAN PLOTS ....

viii

132 134 141 145

Page 13: Two Dimensional Finite Element Modeling of Swift Delta

1

INTRODUCTION

Soil nailing is the term used for a t~chnique of reinforcing

the earth in-situ to provide stability for excavations and

slopes. The technique employs the introduction of reinforcing

elements into a soil mass. The elements, called nails,

develop a tensile component in the soil mass and are

fabricated of steel. An un-reinforced soil mass may not be

stable, especially if it has a free face with a steeper angle

than it's apparent cohesion and angle of repose can support.

In which case the free face is stabilized with a structural

facing element (e.g. shotcrete). The reinforcing elements

interact with the soil mass to form a gravity block which can

be used to hold back vertical faces. This process is called

mechanical stabilized earth. Soil nailing uses passive

inclusion to mechanically stabilize in-situ soils (cuts) .

There are also methods for constructing mechanically

stabilized embankments and fill walls (eg. geotextile walls).

Soil nail stress development (top down) is different than

that of reinforced fill walls (bottom up). Stresses tend to

be higher at the top of the wall and lower at the bottom.

Therefore soil nail walls deflect the most at the top of the

wall face as opposed to mechanically stabilized fill walls

which show the roost horizontal deflection at the bottom of the

wall. Soil Nailing uses a top down construction sequence and

Page 14: Two Dimensional Finite Element Modeling of Swift Delta

2

was first used in Versias, France to construct an 18 meter

high wall1• The first Soil Nail Wall in the U.S. was

constructed in Portland, Oregon at, the Good Samaritan I

Hospital Expansion.

Since 1972 several design methods have been used in the

United States and Europe. Most of these design methods are

based on limit equilibrium principles. The major differences

in analysis procedures being in the definition of factor of

safety, soil reinforcement interaction, and resisting forces

provided by the reinforcing nails.

The Federal Highway Administration has recognized soil

nail walls as having large potential cost savings over other

alternatives. Because of this, they are backing the

development of nail wall technology and have provided

financial support for this project.

The increasing need to provide high capacity roadways in

restricted right of ways under structures such as bridges will

require increased use of techniques such as combined nail and

piling walls. Thus, it was considered necessary to understand

the soil nail wall structure interaction in relation to the

existing pile supported abutment. This research attempts to

answer the following two issues:

1 Transportation Research Board, Report 290, New York, NY, 1980, page 66

Page 15: Two Dimensional Finite Element Modeling of Swift Delta

3

1. Is there potential for the introduction of new bending

stress to the existing piling?

2. Is the soil nail wall system influenced by the presence

of the piling?

Page 16: Two Dimensional Finite Element Modeling of Swift Delta

SWIFT BOULEVARD DELTA PARK INTERCHANGE

SOIL NAIL WALL

Project Scope

4

The Swift Boulevard Delta Park Interchange is located in

Portland, Oregon approximately 1 mile south of the Oregon­

Washington border. The interchange allows access from both

north and south bound lanes of I-5, Swift Boulevard, and the

Delta Park shopping area. The Swift Boulevard Delta Park

Interchange is owned by the Oregon Department of

Transportation. The Oregon Department of Transportation was

responsible for reconstruction design, as well as construction

contract administration and construction inspection. Partial

funding was received, for the junction reconstruction, from

the Federal Highway Administration (FHWA). As part of the

interchange reconstruction, highway engineers were faced with

widening swift Boulevard from two lanes to four under

extremely limited geometric and traffic constraints ( Figure

1) . These are summarized:

Geometric: The proposed widening was located under the

South end of the Oregon Slough bridge. The widening was

bound by the Oregon Slough, north of Swift Boulevard, and

the Oregon slough bridge abutment, South of Swift

Boulevard. The existing bridge abutment was a pile

Page 17: Two Dimensional Finite Element Modeling of Swift Delta

5

supported spill through type with a 2H:1V end slope.

Traffic ClQsure of I-5 was not allowed. Swift Boulevard

traffic volumes are extremely high and only temporary

non-peak period lane closures were allowed.

Clearance Highway engineers decided that to accommodate

the proposed widening, the existing abutment slope would

be removed and that a retaining wall would be needed in

it's place. A cast in place retaining wall was

considered; but was not cost effective due to the

anticipated cost of an extensive temporary shoring

system. A tied-back soldier pile wall was also

considered; but would require installing the soldier pile

through the bridge deck. Thus interrupting I-5 traffic

flow and extra cost for repair to the bridge. Soil

nailing was considered feasible because it's top down

construction method does not require temporary shoring.

In addition soil nailing can be performed with relatively

small equipment that would be clear of traffic and could

also operate in tight spaces.

The permanent wall was next designed by the Oregon

Department of Transportation Bridge Section using the Shen

Page 18: Two Dimensional Finite Element Modeling of Swift Delta

6

analysis method2 • An approximately 250 foot long structure

with a maximum height of 19 feet was proposed. Figure 2 shows

the developed elevation view for the wall.

Construction

The prime construction contractor was Kewitt - Marmjaeo. The

subcontractors that worked on the wall were Schnabel

Foundations (Nail Wall Construction), L.R. Squire and

Associates (Instrumentation Installation), and Johnson Western

Gunnite (Nail Wall Structural Shotcrete). Approximately 166

feet of the wall required removal of the abutment end slope

and nailing between the existing 14 inch diameter pipe piling,

on approximately 4.5 foot centers. It required 275 permanent

nails. The nails consisted of #8 (1.0 inch diameter) and #9

( 1.125 inch diameter) epoxy coated grade 60 Dywidag Bars.

There were 28 sacrificial nails installed to prove that the

design anchor capacity could be developed. The structural

shotcrete had a 1.5 to 3.0 inch slump and an air entrainment

of approximately 7.5 % by volume. The nail grout consisted of

Type I/II Portland Cement, with a water cement ratio of~ 0.5.

The basic construction sequence used on this project is

as follows:

2 Bang, S. ; Shen, C. K. ; Investigation of Soil Nailing Research Record 1369, 1990.

Kim, J.; Systems.

Kroetch, P. Transportation

Page 19: Two Dimensional Finite Element Modeling of Swift Delta

STEP

1. Cut

2. Reinforcement

7

PROCESS

- Excavate to the back of shotcrete wall

face.

- Place reinforcing steel (W20xW20 mesh)

(construction sequence continued)

STEP

3. Guide Wire

4. Shotcrete

5. Drill

PROCESS

- Place guide wires to control the

shotcrete lift thickness.

- Apply shotcrete pneumatically.

- Drill nail holes.

6. Nail Installation -Insert #8 and #9 nails (Dwyidag bars) in

dry nail hole.

7. Grout Pressure grout nails with a minimum 150

psi pressure.

8. Repeat - Start the next wall lift.

In general the construction

compact. Table I shows

equipment used

the equipment

construction sequence above, and it's purpose.

Construction Problem Areas

was small and

used, in the

The temporary cut face suffered sloughing problems during the

project. Sloughing was attributed to loose material at the

face and accidental over excavation during the cut sequence.

Page 20: Two Dimensional Finite Element Modeling of Swift Delta

8

I TABLE I

I Construction Equipment

Construction Process Equipment Model/Type Purpose

Phase Time

Hrs/Lift

1-Cut .75 Dozer Catapiller Rough cut

D6 wall

excavation.

1-Cut .5 Loader Rubber Removal of

Tired spoilings

from wall

cut.

1-Cut .75 Dozer John Deer Close up wall

450 excavation.

1-Cut . 5 Backhoe Case 580 Close up wall

excavation.

2-Shotcrete 2.0 Shotcrete Swing tube Apply struct.

pump. type. shotcrete.

3-Nail 12.0 Drill Krupp Drilled nail

Installation DHR-580A holes.

Page 21: Two Dimensional Finite Element Modeling of Swift Delta

9

I TABLE I

I Construction Equipment r

Construction Process Equipment Moqel/Type Purpose

Phase Time

Hrs/Lift

3-Nail 8.0 Grout Pump Positive Press. grout

Installation Disp. Type nails.

The sloughing was severe enough at times to influence the

instrument readings, possibly giving misleading information

relative to the specified wall construction procedure.

The project created a unique problem in that the stress

states of the existing bridge foundation would be disturbed.

Past experience has shown that soil nailed structures deflect

horizontally about .1 - .4 percent relative to wall height3 •

At swift Delta, predicted maximum horizontal deflection would

then be approximately .75 - 1.26 inches. Since the wall face

would be directly in front of the existing bridge piling, it

is assumed that the piling also would deflect laterally and

therefore a new bending stress would be induced.

3 French Soil Nail Manual

Page 22: Two Dimensional Finite Element Modeling of Swift Delta

~ 1

VICINI TY MAP NO SCAL(

").,,,, _4; =c-=-- N

Le1~,,., d

~<::C4 <v~.,

~ /est ?d (rP)

·~ 23 or-1~3 (TB)

'(.,.,

/ ,c

·-r-i____ ~ -

I

a:,_~ ~) ..;.;-0 '> 0 -S>,

~ .o't·o1 -.~r .ov.;>·· ,,J

-...... Section Sl

PLAN Scale: r • -:o·

after ODOT ref 1.2

FIGURE 1: Location and Wall Plan

10

¥

Page 23: Two Dimensional Finite Element Modeling of Swift Delta

f · •' r - ··•

Instrument Section #2

Extensometer Locat.:onl·· Pile Cap l' •... _._· · . -- ·_ Sl-130

~--=-~=~-~~ - ~--_..}. --- . - .. ___::i -- . 1--r-..

,, .. .. : '. :: :; ;: L; 'I II •I 11 I• II It 'I

~ ;..: ;.: ~ :.; ~ ~ ~I ~\/~ I•

Existing Pipe Pile Instrument Section # 1

FIGURE 2: .Developed ~levation Vie~

__ .,._

r-i r-i

Page 24: Two Dimensional Finite Element Modeling of Swift Delta

12

INSTRUMENTATION

The wall was fully instrumented with two separate sections

located at UV line station 130+59 (instrument section #1) and

UV line station 131+05 (instrument section #2).

Figure 4 show typical cross sections

Figure 3 and

for the two

instrumentation sections. The wall was instrumented to

monitor nail stress distribution, pile cap deflection, wall

deflection, pile bending strain, and wall earth pressure. The

instrumentation consisted of vibrating wire strain gages,

slope inclinometers, load cells, earth pressure cells, optical

survey, and a single point extensometer. Table A-1 of

Appendix A lists the instruments employed as well as the

quantity, manufacturer, and accuracy. Vibrating wire strain

gage locations were equally spaced down the dywidag

bars(nails). Each location contained a gage on the top and

bottom of the bar. Electronic load cells were located at the

nail heads on rows one , three, and five at each instrument

section and were cast into the final shotcrete face. The

inclinometers were installed at UV line Station 130+62 (SI-

130) and UV Station 131+25 (SI-129) approximately 3.5 feet

behind the wall face. During construction instrument readings

were taken after each wall lift was completed. Figures 5

through 9 are typical plots from the reduced instrumentation

data with the reading date given on each figure. Post

construction instrument readings were taken on monthly

intervals. The full data is not presented in this report but

Page 25: Two Dimensional Finite Element Modeling of Swift Delta

13

is available in the Swift Delta Interchange Soil Nail Wall

Instrumentation Data report, available from FHWA, Region 10.

The vibrat~ng wire strain gages were placed along the

nails to measure both axial and bending strains. Load cells

were placed at the nail heads to measure the nail load

developed at the face. The single point extensometer was

installed behind the pile cap to measure outward deflection of

the pile cap. Four strain gages were also placed on two of

the bridge piling at depths of approximately 5 and 12 feet.

Earth pressure cells were placed behind the wall facing to

measure the earth pressure behind the wall. Optical survey

points were established along the wall face to measure

horizontal deflection. Finally slope inclinometers were

placed behind the wall as an additional means to monitor

horizontal wall deflection. Instrumentation results for the

earth pressure cells, pile strain gages and optical survey

were found to be inconsistent and thought unreliable. Because

of this they were not referenced for this report.

Page 26: Two Dimensional Finite Element Modeling of Swift Delta

IJOmm dla. concreld grout~ soil nail No. 9 f29mml £p0q ccat~ ~

q:J strain govge

Dywldo<J l>ar

E (\,

ti

E

.

Original

Bottom strain gc~

SECTION A-A No Scale

f Pl~r IO -J

:i ,,

'Of /

E ...,

c:)

E 0\,

E 0\

ci

eOI E O"I 0

E O"I

0

E 0\

0

~

£.dstlng .JS61Dtf1 $lf/fJI pl~ pl~

INSTRUMENTATION SECT ION

<Sta. "'UV- 130 • 58..9SJ

e ""I ..... ....:

}i ~~ ~ ..._

;~ ..... I()

......: .....:

Nolt11

·· [:::> Loo<J aJll

FIGURE 3: Instrument Section #1 Cross Section

14

Page 27: Two Dimensional Finite Element Modeling of Swift Delta

.. @T°" strain <PU9"J IJOmm dlo. c011Crt1f'1 - •

grovtod .soil nail ·"-... ·. .• •. · .-No. 9 l29mmJ Epoxy ccot'1d • : • ~ ... ~ · Dywldcg bar

\_ Bottom strain <Put;;e

E

"' ci

E '£>

./

SECTION A-A No Scole

c5

Original G~~ i:t 5-0ll-Nollod Wot! ./ I~

E ......

c5

E

°' cl

"'' ~ c5

~

e

E ...., ...:

2

INSTRUMENTATION SECTION 2

tSta. •I.JV" /JI • <H.811

NoftJ1

[::::> Load cell

FIGuRE- 4: Instrument Section #2 Cross Section

15

Page 28: Two Dimensional Finite Element Modeling of Swift Delta

I . t x

I -I "' - .!J 0 cO <0-

0

t t -N ";-' O> -cO W'

<!> 0

t t l'V

I

"' - I

O> "' cD I

tO 0

t r w

I I - "' O> I

cO tO

....

91

z ~ r Ct> ::J co -';;j"

"T1 .... 0 3 ~ ~ "T1 Q) n Ct>

:::;; Ct> Ct)

e

0

0

CJ'1

N 0

"' CJ'1

0 .;:.

Axial Nail Load (kips)

O') co 0 N ~

--t Cl)

:J ~. Ci)'"

z ~ . r 0 Q)

a. (/)

a c ::::? • :J cc CJ 0 :J en ....+ ..., c (") ....+ c;· :J

en C'O (") ....+ 6' :J -Jo

JJ 0

~ -Jo

Page 29: Two Dimensional Finite Element Modeling of Swift Delta

t-.rj H Gl q ~ txj

°' .. H ::s en rt t;

~ c;; a.

CD ~ ::s -rt "'O ro

(/) 0 -' CD ·n; 0

rt z ~- n; 0 ·x ::s

< ~ (\.)

z Ill ~-,._,

t"i 0 Ill ~

"'d ,._, 0 rt en

14

12

10

8

6

4

2

0

0

Tensile Nail Loads During Construction, Section 2, Row 1

5 10 15

Nail Length From Wall Face (feet)

--0-- 12-10-90 -0-- 12-13-90 ---- 12-18-90 •

20

1-16-91 -::!(- 3-16-91

25

1--' '-l

Page 30: Two Dimensional Finite Element Modeling of Swift Delta

c;; G> ~ 0

:§ c 0

"+:l 0

0.50

0.40 +

I 0.30

~ 0.20 -<I> 0

0.10

0.00

0 Dec. 1990

c 0

'+J u s Cll c 0 u -0

"O c w

I

A

1.1,

6

Swift - Delta Park Interchange Single Point Extensometer @ Pile Cap

12

Time (Months)

FIGURE 7: Pile Cap Extensometer Plot

I'

18 24

I-' a:>

Page 31: Two Dimensional Finite Element Modeling of Swift Delta

Multi-Deflection Plot - 50129 . Vector Magnitude

Deflection {in)

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

0 I I I I I I• I I I I 1 I I I I I I I I I I I I I I I I I I I I I I I I 1 I I I I I I I I I Li I I I

~ CJ)

.E Cl) tO u .... 0

-5

-10

a. ~ -15

~ 0 a; co .i::. .... a. Q)

0

-20

-25 -

-30

Deflections During Construction (to 3-16-91)

--0-- , 2-9-90

--0-- 12-15-90

---- 1-5-91

--tr-- 1-12-91

--x-- 1-23-91

.._ 2-2-92

--+--- 3-16-91

FIGURE 8: SD 129 Slope Inclin.ometer Plot

19

Page 32: Two Dimensional Finite Element Modeling of Swift Delta

Multi-Deflection Plot - SD130 Vector Mt!gnitude

Deflection (in)

0 0.1 0.2 0.3 CA 0.5 0.6 0.7 0.8 0.9

0 1......-r• I , I I I j 1-r-·1-1-t-•-rrl" i..,....,-,-,-+-r-.-.-rf-r--,~rrf~T-r~r-rrl

r ~ ~ !!' . /'' />' /+ /

-5 -w f y{/ /+-/ /

~,I ; Li,/ ,// / ! /,., -r-

I /,-

Wt . xi + ?-' f\._ t /1 / / ~ .. x~ .. f.

~ I/ I ,

;!;f + ' i / 1 I I

-10 T ~ 1<• T I - .1JJ1! I ~ 11-11 rt t ,... I e. Xlf -'- I ~ I ~!J; -f-

.:::: r]1 , , . /

~ r l II I I 0 I r·>';tf .. ;- " ! \1 \ . n. I I ' \

0 -1 5 -+t:.:. ~ + ~ ~ i(' \ .\ \ ~ ~_J:.\ :e. + A

_g ~ I \ 1 C> ~ +

~ ~1 rh j i;1

o. ;I/ ,, I Q.) JJ. .if I

o -tlrf.Y. + ~ -20 JI. _//

.1/ // 'Ir, r«, ~t !fl

-25 f t

-30 I lDetTecti~~-~ D~ring. Construct.ion .J I (to 3-16-81) .__ ______ _

----0---- 12-2S-90

-----+--- i-s-s:

--t._'r-- 1-~-91

--x--- 1-12-9:

---·--- 1-16-91

---1-- 1-26-91

---k--- 3-1 6-9 1

FIGURE 9: SD 130 Slope Inclinometer Plot ·

20

Page 33: Two Dimensional Finite Element Modeling of Swift Delta

21

SOIL TESTING

I

The soil fill behind the wall generally consisted of clean,

uniform grained, loose dredge sand, previously borrowed from

the Columbia River. There were also zones of low plasticity

silt fill material and large pieces of wasted concrete,

asphalt and cast iron pipe.

Laboratory Soils Testing At Swift Delta

Laboratory testing was performed by the Oregon State Highway

Division (ODOT) during their investigation for the soil nail

wall. Table II and III summarizes the laboratory testing

results with the following notation:

LL - Liquid limit

IP - Plastic index

Gama dry - Dry unit weight (pcf).

Gama sat - Saturated unit weight (pcf) .

Su (torv) - Undrained shear strength from torvane (psf) .

Phi - Internal friction angle degrees.

uses - Unified soil classification system.

Table II represents the results of the only triaxial testing

performed for this project on an undisturbed sample taken from

test boring TB 115. This boring was not located in the

immediate vicinity of the wall. The extent of shear strength

testing conducted for wall design was not judged adequate for

refined FEM input.

Page 34: Two Dimensional Finite Element Modeling of Swift Delta

I TABLE II Triaxial Test Results

Hole # Depth LL PI Gama Phi dry

TB-115 16.0 38 12 90 23.5

c Su (psf) (tsf)

129.6 .37

uses

ML-CL

I

IV IV

Page 35: Two Dimensional Finite Element Modeling of Swift Delta

I Hole # Sample # Depth % Mc

TP-1 5.0

8.0

11. 0

TP-2 6.0

9.0

TB-124 N-5 10.0 33

N-6 13.5 38

N-15 38.0 32

N-16 43.0 45

TB-125 U-1 10.0

U-2 40.0

TB-127 N-2 8.0 40

U-1 8.5

N-3 13.0 30

U-2 18.0 8

N-7 33.0 36

TB-128 N-2 8.0 33

TABLE III Laboratory test results

LL Pi Gama dry Gama Sat

36 1

40 10

37 12

45

38 10 78.4 109.9

28 7 89.4 116.1

34 10 84.6 115.4

34 10 84.7 112.3

s (torv) Phi

0.6 tsf

.8

0.8-1.0

0.35

0.35

32.4

uses SM-GM

ML

SM_

SP

SP

ML

ML

ML

ML

ML

ML

CL-ML

SP

ML-CL

ML-CL

I

N w

Page 36: Two Dimensional Finite Element Modeling of Swift Delta

24

Insitu Testing At Swift Delta

To supplement t:t,le laboratory test program and form a test

basis to develop constitutive parameters, Pressuremeter

testing (PMT) was done in December 1990 and May 1991. Five

pressuremeter tests were performed behind the wall in the

vicinity of instrument section #2. A Texam pressuremeter unit

(manufactured by Rocktest Inc.) utilizing EX and BX (32mm dia.

and 62 mm dia respectively) probe sizes was used for these

tests. The primary soil parameter used in the following

report was the soil modulus E0

• From the pressuremeter

testing a modulus value ranging from 200 - 500 ksf was

estimated. It is interesting to note that French soil nail

wall preliminary designs are based on correlations to

pressuremeter test data4• The following table summarizes the

pressuremeter test results for this project, in terms of net

limit pressure, Pl*, with Po as the at rest pressure.

All holes were drilled by hand augers and each test

conducted in accordance with ASTM D4719. The results shown in

Figures 10 and 11 illustrate the high quality data which is

generally consistent with testing uniform sand at increasing

depth. Figure 12 is a summary of the limit pressure and

modulus at depth for the testing.

4 page 11, FHWA Tour for Geotechnology-Soil Nailing, June 1993

Page 37: Two Dimensional Finite Element Modeling of Swift Delta

25

Table IV

summary of Pressuremeter Test Results I

Test # Probe Depth Po Eo Pl* Eo/Pl*

(ft) (ksf) (ksf)

(ksf)

1 BX 2.5 0.1 98.3 14.9 6.6

2 EX 4.25 0.2 28.8 4.8 6.0

3 BX 6.29 0.3 56.9 7.7 7.4

4 BX 8.96 0.5 55.8 9.0 6.2

5 BX 4.38 0.2 47.3 6.3 7.5

Page 38: Two Dimensional Finite Element Modeling of Swift Delta

LL Cf) ~ <D .... :J (/) (/) <D 1.-(L

SWIFT DEL TA PMT 5/29/91 TESTS I ,3,4 and 5

O~·····~·······t························

-1 I 0 5 10 15 20 25

I I

Radial strain (%)

FIGURE 10: EX Probe Pressuremeter Test Results

:1 •I

30

N

°'

Page 39: Two Dimensional Finite Element Modeling of Swift Delta

SWIFT DELTA PMT 1/10/91.TEST 2

(l) L-

:J (/) (/) (l) '-

D...

L

., 4.25ft Deep~ · ·

51 i

4.;;~······00••••••••••• I i ,

. !

0 ., .. 0 5 10 15 20 25 30 35

Radial strain (%) ·FIGURE 11: BX Probe Pressuremeter Test Results

~ ~

Page 40: Two Dimensional Finite Element Modeling of Swift Delta

Swift Delta PMT Summary Pressuremeter Limit Pressure (ksD

, 2 3 4 ,1J1 I I ~ 1 ,5 6 7 8 I 9, 1 0 f 1 1 2 0 I i !

I :. . : : ! 1 l Increase of Eo with Depth

; -2

r················1············ ~t·················1···· ·· ·r·· · r·· · r··· ··r · ·····r···············r··· :f --0 c ::J 0 )....

tr\ I i i I : .1'. '·i. : :_' : -....• \...J ; ; ; .!/'f ' ; ··... ! : ' : ·· .....

-~

~ ! Increase of Pl* f \. f l ~ i -8 ·····················-!-·············· 1

with D~pth 1

.. • ... 1.>:· :.· .. 1

... ······U : ... . 0

-1 o ····················l·····················l·················i················ I···················, ................. \ ................ J ............ f .............. J ............... .

. I I j ~I* @ 1 ksf/ft \ j Eo @ 5 ksf/ft J J

l I , , . : : : :

12 I : I : : I : : :

- Io

1 Q 15 201• .I I 125 30 35 40 45 50 55 .. 60 Pressuremeter Modulus Eo (ksf)

FIGURE 12: Pressuremeter Test Results summary

:1

tv OJ

Page 41: Two Dimensional Finite Element Modeling of Swift Delta

29

TWO DIMENSIONAL FINITE ELEMENT MODELING

The monitored results of the project instrumentation are not

enough alone to ~nswer the questions pre~ented in Section 1.

Instrumentation data in conjunction with soil nail wall/bridge

foundation modeling was performed to provide a more thorough

analysis. Limit equilibrium based analysis can only describe

the wall soil stress state at plastic failure and has no

provision for linking the pile into the soil nail model.

Limit equilibrium modeling was not suitable for the scope of

this report. Finite element modeling was chosen as it had the

ability to model the stress state of the soil nails, wall

face, piling, and the soil during construction.

Instrumentation data was used to assist in calibration of

the soil parameters. Attempting to correctly predict the

exact soil stresses would not be practical, because of the

limitations of two dimensional modeling and the limited

information available on the soil strength parameters.

ABAQUS

All modeling was performed with the commercial finite element

code ABAQUS versions 4. 8 - 5. 2. ABAQUS is produced by

Page 42: Two Dimensional Finite Element Modeling of Swift Delta

30

Hibbitt, Karlson, and Sorenson Inc5 • It is a general purpose

finite element program widely used for geotechnical analysis.

It's capabilitiep are well documented for solving non-linear

soil deformation problems. ABAQUS was run on both SUN SPARC

one UNIX based work stations, and on the San Diego Super

Computing Center's Cray MXP computer.

PATRAN

Pre-finite and post-finite element work was done using the

UNIX based program PATRAN (produced by PDA Engineering) . The

pre-processor generated the finite element meshes used in the

modeling. The post-processor generated all stress, strain,

and deformation fringe plots. These fringe plots proved to be

a very powerful tool in analyzing the complex output from

ABAQUS. Figure 13 is an example of PATRAN postprocessing

graphics.

Finite Element Mesh Development

The soil nail wall/pile foundation system was simplified to

two dimensions. This was necessary due to the extremely large

computational effort that a full non-linear, three dimensional

model would require. Wherever the mesh geometry would allow,

5ABAQUS USER MANUAL, Volumes 1 and 2, Hibbitt, Karlson, and Sorenson, Inc. 1992

Page 43: Two Dimensional Finite Element Modeling of Swift Delta

31

4 node quadrilateral elements were used, to achieve the slope,

3 node triangular elements were also used. Past research has

indicated that tqe behavior of anchors in.sand is concentrated

in it's near vicinity. Anchor influence is considered to be

insignificant at a maximum distance of 30 diameters. The

location of the boundary of discrete semi-infinite zones was

found to be 20 diameters by Deasi et. al. 6 An 84 foot long by

35 foot high mesh boundary was used. The back of the wall

face was placed a minimum of 80 diameters from the rear

boundary (behind the nails). The nails were modeled with a

single column of elements using a hexagon shape. The

shotcrete face was modeled as two columns of elements; the

first column to simulate the shotcrete wall face being placed

in a "lift by lift" sequence; the second (outer) column to

simulate the single application of shotcrete that was applied

to the entire wall face. Bridge piling were modeled similar

to the nails, with one column of elements and a hexagon shape.

Two wall geometries were modeled, the first of which is

located under the bridge Figure 14 (instrument section #1 UV -

Station 130+59). Figure 13 also shows the intensity of the

mesh in the areas of interest such as the nails and wall face.

The second is located outside the influence of the bridge

foundation system (instrument section #2 UV - Line Station

131+05) Figure 15. Instrument section #1 consisted of

6c.s. Deast, A Muqladir, F. Sheele; Interactive Analysis of Anchored Soil Systems; ASCE Geotechnical Journal, May 5, 1986, Volume 112

Page 44: Two Dimensional Finite Element Modeling of Swift Delta

32

approximately 450 elements and instrument section #2 consisted

of approximately 435 elements. The two sections were analyzed

for comparison of the effects of the pile foundation relative

to a section that was not influenced.by the pile foundation.

Both plain strain and nonlinear analysis were performed on the

same -finite element meshes.

1 ksf Line Load Validation

The global geometry for the two finite element (FE) meshes is

very similar, with the difference being the removal of

elements near the pile cap for instrument section #1 to create

a 2H: lV slope above the wall face. This removal creates

instrument section #2. Thus instrument section #1 was

constructed first and verified by placing a 1 ksf surface line

load behind the pile cap and then analyzing it under purely

elastic conditions. Figure 13 is the horizontal stress fringe

plot and shows very reasonable results with a maximum

compressive stress of approximately 1 ksf transitioning to

lower compressive stress states below and outward from the

load initiation area. Figure 13 is a combined deformed mesh

and vertical deflection fringe plot. It can easily been seen

that the maximum vertical deflection is at the surface and is

on the order of two tenths of a foot. This deflection was

compared with a closed form approximation to the vertical line

Page 45: Two Dimensional Finite Element Modeling of Swift Delta

33

load on a finite layer7• The closed form solution predicted

approximately .16 foot deflection. This is a very good

comparison to th~ FE results. Appendix B contains additional

fringe plots of horizontal stress, vertical strain, horizontal

strain, and maximum shear stress for the 1 ksf line load

condition. The results presented show that there are no

obvious defects in the FE model and that it is ready for more

advanced FE modeling as follows.

7Poulos and Davis,Solutions for Soil and Rock Mechanics, pages 28 - 32.

Page 46: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.1-RES=4.1-P3/PA TRAN R.1-0/ ector-Y)-ABAQUS-18-Feb-94 12:55:01

Deformed_plot: LC=2 .1-RES=4.1-P3/PATRAN R.1 .2-Deformation-ABAQUS-18-Feb-94 13:3

Swift Delta 1 KSF Line Loac:Oeflection

FIGURE 13: 1 ksf Line Load Vertical Stress

0.

-.01331

-.02663

-.03994

-.05325

-.06657

-.07988

-.09319

-.1065

-.1198

-:1331

-.1464

-.1598

-.1731

-.1864

-.1997 L_J w ii::.

Page 47: Two Dimensional Finite Element Modeling of Swift Delta

SWIFT DELTA FINITE ELEMENT MESH

FIGURE 14: Finite Element Mesh Instrument Section #l

w U1

Page 48: Two Dimensional Finite Element Modeling of Swift Delta

SWIFT DEL TA SOIL NAIL WALL INSTRUMENT SECTION 2

FIGURE 15: Finite Element Mesh Instrument Section #2

w O"\

Page 49: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.1-RES=1.1-P3/PATRAN. R.1-{Tensor-XX1:ABA9US-18-Feb-9412:23:02 Swift Delta 1 KSF Lrne Load 2 -· :_ • -s .09416

.03374

-.02669

-.08711

-.1475

-.2080

-.2684

-.3288

-.3892

-.4497

-.5101

-.5705

-.6309

-.6913

FIGURE 16: 1 ksf Line Load Horizontal Stress -.7518

-.8122 w -..J

Page 50: Two Dimensional Finite Element Modeling of Swift Delta

38

PLANE STRAIN MODELING

Finite element modeling steps were first performed in

plane strain elasticity for all models. This simplified the

initial debugging process of the models. Three models were

developed, two for instrument section #1 and one for

instrument section #2. The instrument section #1 models

consisted of one with the nails active (file name = linln) and

the other with the nails and pile active (file name = linlp).

In order to model the actual construction process a dynamic

excavation process was developed. This process included

removing elements to simulate the excavation of a soil lift,

removing elements to simulate the drilling of the soil nail

hole, replacing the nail drill hole elements with steel/grout

elements to simulate the nail insertion, and adding shotcrete

elements to the exposed soil face to simulate the structural

shotcrete wall face. ABAQUS would not allow two different

material properties to be assigned to one element. This would

be needed at the nail locations to model the removal of soil

and the insertion of a grouted nail by changing the soils

material property to that of a nail section. Since this could

not be permitted, dual elements had to be developed at the

nail locations so that both soil and nail material properties

could be used there at various stages of the model execution.

Capturing the piles influence was done with model linlp.

Page 51: Two Dimensional Finite Element Modeling of Swift Delta

39

The nails and pile are connected to each other as one material

where they cross each other in the mesh. The nails are

modeled in all cases as a 6 inch tall cross section with a 1

foot width. The nail modulus was proportioned to take into

account its width and steel/grout properties. The instrument

section #2 model (file name = lin2n) contained just the nails.

The FE modeling steps are listed below for the linlnp

model and are based on the actual construction process that

was used to construct the Swift Delta Soil Nail Wall as

discussed in the construction section of this report.

Page 52: Two Dimensional Finite Element Modeling of Swift Delta

linlp (nolinlp) Instrument Section #1 Soil Nail

Modeling Steps

Step 1 - Removal of shotcrete, Nail, and pile elements.

Step 2 - Geostatic Turn On

Step 3 - Pile Installation

Step 4 - a) Excavation #1 ( 3. 5 Ft)

b) Add shotcrete to face.

c) Drill nail hole by removing slope elements.

d) Install Nail #1 (15 degrees 21.0 Ft)

Step 5 - a) Excavation #2 (5.5 Ft)

b) Add shotcrete to face.

c) Drill nail hole by removing slope elements.

d) Install Nail #2 (15 degrees 21.1 Ft)

Step 6 - a) Excavation #3 ( 2. 0 Ft) .

b) Add shotcrete to face.

c) Drill nail hole by removing slope elements.

d) Install Nail #3 (15 deg. 22.3 Ft).

Step 7 - a) Excavation #4 (3.0 Ft)

b) Add shotcrete to face.

c) Drill nail hole by removing slope elements.

d) Install Nail #4 (15 degrees 20.9 Ft)

Step 8 - a) Excavation #5 (3.0 Ft).

b) Add shotcrete to face.

40

c) Drill nail hole by removing soil elements.

d) Install Nail #5 (25 degrees 20.3 Ft)

Page 53: Two Dimensional Finite Element Modeling of Swift Delta

41

(Model Steps, continued)

9 - a) Excavation #6 (1.5 Ft)

b) Add shotcrete to excavation #6 and the

second shotcrete application to the entire

wall face.

10 - Geostatic turn on.

Fringe Plot Scaling

All of the vertical and horizontal stress fringe plots have

been scaled to show soil response. Therefore, fringe plot

ranges start at zero stress and end at a maximum compressive

stress of -3500 psf. All of the major stress fringe plots

were scaled to show nail response. These fringe plots start

at zero stress and end at 10,000 psf (tension).

Page 54: Two Dimensional Finite Element Modeling of Swift Delta

42

Geostatic Turn On

The FE modeling, begins with the activa:tion of a geostatic

stress field. This stress field sets the mesh to a gravity

stress state which increases with depth in proportion to

overburden pressure. ABAQUS requires that all non-horizontal

boundaries be fixed in the horizontal direction. This results

in a pseudo-geostatic stress field for slopes, such as the

2H:1V at swift Delta. With this, good comparison was still

obtained between ABAQUS for step 2 geostatic turn on of

horizontal and vertical stress ( Figures 17 and 18) and the

predicted stress states for instantaneously loaded linear

elastic embankments by Poulos et al 19727 •

Incremental Modeling

All three models were checked in linear elasticity through the

complete incremental modeling process. This included the

introduction of the five nails and the separate application of

a final shotcrete lift. For the sake of redundancy, linln are

the only linear elastic results presented in Figures 18

through 23, which are the horizontal stress fringe plots and

illustrate the sequential modeling steps. The plots show

reasonable results except for a small stress anomaly below

nail #5 at the wall face. It appeared to be a defect in the

7Poulos and Davis

Page 55: Two Dimensional Finite Element Modeling of Swift Delta

43

mesh but after analyzing the input data it could not be

isolated. It did not appear to interfere with the models

functioning. Apalysis of the major s:tress fringe plots,

(Figures 24 through 30), show the .behavior of the nails.

Figure 24 shows that the 1st nail installed is in an extremely

high ·state of stress (maximum 3, 300 psf) relative to the

surrounding soil. This elevated stress state is not what

would be expected from a typical nail installation, there the

nail would be at a zero state of stress until a soil lift was

excavated below the nail. The reason for the ABAQUS model

high nail initial stress state is probably do to high soil

strains developed after the soil cut lift was made. The

problem occurs when the nail elements are introduced as a

material with a much higher modulus that must undergo the same

amount of strain as the lower modulus soil did originally.

Therefore a correspondingly high state of nail stress is the

result. Figures 25 and 26 show that the second nails initial

stress of approximately maximum 3, 300 psf dissipates to

approximately 2, 000 psf with the subsequent excavation of lift

#3. This same phenomenon is repeated for nails #3 and #4, but

is not seen in nail #5 which is installed at a high stress

state and seems to remain at a high stress state. This FEM

anomaly illustrates the difficulty in modeling soil nails.

Page 56: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.1-RES=1.1-P3/PATRAN R.1-(Tensor-XX)-ABAQUS-05-Mar-94 14:20:32

SWIFT DELTA FINITE ELEMENT MESH LIN1N GEOSTATIC TURN ONMODEL STEP 2

. . . . FIGURE 17: LINlN Geostatic Turn On Model Step 2 Horiz. Stress

34.96

-197.1

-429.1

-661.1

-893.2

-1125.

-1357.

-1589.

-1821.

-2053.

-2285.

-2517.

-2749.

-2981.

-3213.

-3445. ~ ~

Page 57: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.2-RES=1.1-P3/PATRAN R.1-(Tensor-XX)-ABAQUS-05-Mar-94 14:26:22

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 3 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2,100.

-2333.

-2567.

-2800.

-3033.

-3267. FIGURE 18: LINlN Model Step 3

-3500. - ~ U1

Page 58: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.3-RES=1.1-P3/PATRAN R.1-(Tensor-XX)-ABAQUS-05-Mar-94 14:57:19

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 4 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

'-2100.

-2333.

-2567.

-2800.

-3033.

rrGURE 19: LINlN Model Step 4 -3267.

-3500. - ii:::.. (j\

Page 59: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.4-RES= 1.1-P3/PA TRAN R.1-(T ensor-XX)-ABAQUS-05-Mar-94 15:04:32

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1 N MODEL STEP 5 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

FIGURE 20: LINlN Model Step 5 -3267.

-3500. ~ -.....)

Page 60: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PATRAN R.1-(T ensor-XX)-ABAQUS-05-Mar-94 15:24:58

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 6 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

FIGURE 21: LINlN Model Step 6 -3267.

-3500. ii::. ())

Page 61: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3. 7-RES=1.1-P3/PATRAN R. t-(T ensor-XX)-~BAQUS-05-Mar-94 15:49:49

SWIFT DEL TA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 8 -233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

- -2333.

-2567.

-2800.

-3033.

FIGURE 22: LINlN Model Step 8 -3267.

-3500. '---I ii::. l.O

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Fringe: LC=2.8-RES=1.1-P3/PATRAN R.1-(T ensor-XX)-ABAQUS-18-Mar-94 13:32:49

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1 N MODEL STEP 9 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267. FIGURE 23: LINlN Model Step 9

-3500. U1 0

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Fringe: LC=3.2-RES=1.1-P3/PATRAN R.1-(Major)-ABAQUS-05-Mar-94 14:41 :43

SWIFT DELTA FINITE ELEMENT MESH 10000.

LIN1N MODEL STEP 3 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---X 1333.

FIGURE 24: LINlN Model Step 3 666.7

-.0001221 .....__. U1

1--'

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Fringe: LC=3.3-RES=1.1-P3/PATRAN R.1-(Major)-AB~QUS-05-Mar-94 14:46:44

SWIFT DELTA FINITE ELEMENT MESH 10000.

LIN1N MODEL STEP 4 9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---X 1333.

FIGURE 25: LINlN Model Step 4 666.7

-.0001221

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Fringe: LC=3.4-RES=1.1-P3/PATRAN R.~ -(Major)-ABAQUS-05-Mar-94 15: 13:48

SWIFT DELTA i=INITE ELEMENT MESH 10000.

LIN1N MODEL STEP 5 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---.X 1333.

666.7 FIGURE 26: LINlN Model Step s·Major Stress

-.0001221 U1 w

Page 66: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PATRAN. R.1-(Major)-ABAQUS-05-Mar-94 15:18:11

SWIFT DELTA FlNITE ELEMENT MESH 10000.

LIN1 N MODEL STEP 6 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000 .

. 3333.

2667.

2000.

---X 1333.

FIGURE 27: Model Step 6 Major Stress 666.7

-.0001221 L-J Ul .t:;..

Page 67: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.6-RES=1.1-P3/PATRAN R.1 ~(Major)-ABAQUS-05-Mar-94 15:40:43

SWIFT DELTA FINITE ELEMENT MESH 10000.

LIN1N MODEL STEP 7 9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000. ___ x 1333.

FIGURE·2a: LINlN Model ·step 7 Major Stress 666.7

-.0001221 U1 U1

Page 68: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.7-RES=1.1-P3/PATRAN R.1~(f ensor-XX)-J\BAQUS-26-Mar-94 14:33:31

SWIFT DELTA FINITE ELEMENT MODEL 10000.

NOLIN1N STEP 8 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000.

- 3333.

2667.

2000.

---X 1333.

FIGURE 29: NOLINlN Step 8 Major Stress 666.7

-.0001221 U1 O'I

-~ ------ ---- ----------

Page 69: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.8-RES=1.1-P3/PATRAN R.1-(Major)-ABAqUS-18-Mar-9413:14:24

SWIFT DELTA FINITE ELEMENT MESH 10000.

LIN1N MODEL STEP 9 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---X 1333.

FIGURE 3 0: LINlN Model Step 9 Maj or Str.ess 666.7

-.0001221 U1 ......J

Page 70: Two Dimensional Finite Element Modeling of Swift Delta

58

NON LINEAR PLANE STRAIN ANALYSIS

Introduction

Most engineering construction materials, including soils,

initially respond elastically on loading. Elastic behavior

implies that when a material is loaded and then unloaded, the

deformation is fully recoverable and the materials shape is

left un-deformed. If the load exceeds the yield load then

deformation will occur. Plasticity theories model a

material's mechanical response as it undergoes nonrecoverable

deformation in a ductile fashion. Plasticity theories have

been developed mostly for metal, but they can also be applied

to soils, rock, concrete, ice, and other materials. Metals

and soils behave very differently when loaded but the

fundamental concepts of plasticity theories are sufficiently

general that models based on this concepts have been developed

and proven for a wide range of materials. Most of the

plasticity models that ABAQUS uses are based on incremental

theories, in which the strain is decomposed into an elastic

part and inelastic (plastic) part. Plasticity models that do

not use the above method are usually called "deformation"

based plasticity models, in which stress is defined from the

total mechanical strain. Incremental plasticity models are

usually formulated in terms of a yield surface, which

generalizes the concept of yield load into a test function,

which can be used to determine if a material will behave

purely elastic at a particular state of stress. A flow rule,

Page 71: Two Dimensional Finite Element Modeling of Swift Delta

59

that defines the inelastic deformation that must occur if the

material point is no longer performing purely elastically, and

some evolution laws that define the hardening, the way in

which the yield and or flow definitions change as inelastic

deformation occurs. These models also need an elasticity

definition to deal with the recoverable part of strain.

Rate independent, yield behavior does not depend on soil

pressure state. Due to the lack of sophisticated soils

testing at the Swift Delta site, a complex soil plasticity

model is not appropriate. A simple soil model using bilinear

material idealization was used. The kinematic hardening model

used in ABAQUS was the Prager-Ziegler model. This model gives

good results up to about 20% strain, but does not take into

account rate effects or soil pressure state in relation to

yield behavior.

The elastic region of the soil model was defined the same

way as the purely linear finite element analysis, with an

elastic modulus and a Poisons Ratio. The plastic region is

defined by the yield stress, hardened stress, and hardened

strain8•

In the past two decades many formulations of nonlinear

soil behavior have been published. The most successful being

the hyperbolic soil model proposed by J.M. Duncan, which has

8ABAQUS Theory Manual 1992, HKS, Rhode Island.

Page 72: Two Dimensional Finite Element Modeling of Swift Delta

60

been incorporated into numerous geotechnical problems9• There

are many short comings of the classical solution such as the

parameters descr,ibing the soil behavior. being derived from

conventional triaxial tests. The hyperbolic, stress-dependent

soil model proposed by J.M. Duncan et al utilizes a total of

nine-parameters to describe stress-strain characteristics of

the soil.

I

TABLE V

I Model Material Properties

Modulus Poisons Unit

(ksf) Ratio Weight

(lbs)

Soil 250 .25 105

Layer #1

Soil 350 .25 105

Layer #2

Soil 500 .25 105

Layer #3

Nail 8.352E5 . 3

9Duncan, J.M.; Byrne, P.; Wong KL.S.; Mabry, P. Strength, Stress-Strain and Bulk Modulous Parameters For Finite Element Analyses of Stresses and Movements in Soil Masses. Geotechnical Engineering. 1980. Department of Civil Engineering, University of California, Berkeley.

Page 73: Two Dimensional Finite Element Modeling of Swift Delta

61

TABLE V

Model Material Properties

'

Modulus Poisons Unit

(ksf) Ratio Weight

(lbs)

2.16E5 .17 145

Shotcrete

Concrete 6.0E5 .2 155

Pile 2.65E4 • 5 200

The non-linear ABAQUS models were developed by modifying the

linear models discussed previously and incorporating the

material properties shown in table 4. The modification

consisted of replacing the single layer linear elastic soil.

properties with a three layer elasto-plastic system. The non­

linear file names are as follows:

nolinln - Instrument section #1 nails in, pile out.

nolinlp - Instrument section #1 nails in, pile in.

nolin2n - Instrument section #2 nail in, pile out.

An example input file nolinlp is located in appendix D.

Page 74: Two Dimensional Finite Element Modeling of Swift Delta

62

RESULTS INTERPRETATION

Interpretation of Instrument Section #2 Results

The interpretation of the results consist of PATRAN fringe

plots and x-y plots generated in a spread sheet using PATRAN

output data results. Instrument section #2 has the least

complicated model and the least number of variables. Because

of this detailed discussion of Instrument Section #2 results

are presented first:

Horizontal Soil Stresses

Horizontal stress fringe plots for models 3, 5, and 8 are

shown in Figures 31, 32, and 33 respectively. In comparison

to the elastic results, there is only a slight difference in

horizontal stresses. The soil stresses within the limits of

the nails are somewhat discontinuous.

Vertical Soil Stresses

Vertical stress plots for model steps 3, 5, and 8 are shown in

Figures 34, 35, and 36 respectively. As with the horizontal

stresses, the soil stress within the limits of the nails are

somewhat broken up. The vertical stresses behind the nails

however, are not discontinuous and are at the same approximate

stress as before the nails were introduced. There is

considerable stress change in front of the wall facing. As

Figure 36 shows for step 8, the compressive stress is higher

Page 75: Two Dimensional Finite Element Modeling of Swift Delta

63

near the wall face, rapidly dissipating to zero vertical

stress, as would be required for the stress level, at the

ground surface in front of the wall.

Nail Stresses

Major stress plots for model steps 3, 5, and 8 are presented

in Figures 37, 38, and 39 respectively. These plots show the

nails being introduced at what appears to be an elevated state

of stress. This must be due to a modulus incompatibility that

has previously been discussed under plain strain modeling. In

Figure 39 model step 8, the nail stress conforms reasonably

well to what would be anticipated, which is to have the

highest nail forces at the top of the wall incremental

decreasing to the bottom of the wall. This is with the

exception of the newly introduced nail 5. Since tension in a

row of nails starts only when the lower levels are being

excavated.

Deflections

The soil deflection in front of the wall facing is shown in

model step 8 (Figures 41 and 42 ). The plots show that the

soil in front of the wall face along the lift excavation

boundary heaves up slightly. The heave is on the order of .05

feet for all three lifts plotted. This heave does correlate

with the vertical stress changes across the excavation lift

boundary discussed above.

Page 76: Two Dimensional Finite Element Modeling of Swift Delta

. Horiz Stress Fnnge: LC=2.12-RES=1.1-P3/PATRAN R1-(Tensor-XX)-ABAQUS-31-Aug-94 13:17:55 (psf)

0.

SWIFT DELTA SOIL NAIL WALL FEM RESULTS -233.3

MODEL NOLIN2N STATIC STEP 3 -466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

nolin2n1 .fil FIGURE 31: NOLIN2N Model Step 3 Horiz Stress -3500.

O"I ii:::.

Page 77: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.14-RES=1.1-P3/PATRAN R.1-(Tensor-XX)-ABAQUS-31-Aug-9413:36:13 Horiz Stress (psf)

SWIFT DEL TA SOIL NAIL WALL FEM RESULTS 0.

-233.3

MODEL NOLIN2N STATIC STEP 5 -466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

FIGURE 32: Model NOLIN2N Static Step 5 Horiz. Stress -3267.

-3500. O'\ U1

Page 78: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.17-RES=1. l-P31PATRAN R. l-(Tensor-XX)-ABAQUS-23-Jul-94 16:30:49 HORIZ STRESS

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 9221.

8384.

MODEL NOLIN2N STATIC STEP 8 7547.

6710.

5873.

5036.

4199.

3362_

2525.

1688.

850.5

13.44

-823.6 ---.X

-1661.

-2498. nolin2n 1.fil

FIGURE 33: Model NOLIN2N Static Step 8 Horiz. Stress -3335.

O'\ O'\

Page 79: Two Dimensional Finite Element Modeling of Swift Delta

. . . VERT STRESS Fnnge: LC=3.

2·RES=

1·1-PSWfFflfELtA>-so1r-NJ\tL WALL FEM REsuL Ts

0.

MODEL LIN2N STATIC STEP 3 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267. lin2n1 .fil

FIGURE 34: Model LIN2N Static Step 3 Vert. Stress -3500. ......__. O'\ -....J

Page 80: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.14-AES=1.1-P3/PATRAN R .. 1-(Tensor-YY)-ABAQUS-31-Aug-94 13:41 :12 Vert Stress (psf)

SWIFT DEL TA SOIL NAIL WALL FEM RESULTS 0.

-233.3

MODEL NOLIN2N STATIC STEP 5 -466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

FIGURE 35: Model NOLIN2N Static Step 5 Vert. Stress -3267.

-3500. 0\ (X)

Page 81: Two Dimensional Finite Element Modeling of Swift Delta

. . . : VERT STRESS Fnnge: Lc=3.

7-RES=

1·1-PSW1Ff·1DELfA-SQ1L-NJ\1fL WALL FEM RES UL TS 0-

MODEL UN2N STATIC STEP 8 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

lin2n1 .fil FIGURE 36: Model NOLIN2N Static Step 8 .Vert. Stress -3500.

°" \.0

Page 82: Two Dimensional Finite Element Modeling of Swift Delta

. . Major Stress Fnnge: LC=2.12-RES=1.1-P3/PATRAN R.1-{MaJor)-ABAQUS-31-Aug-94 13:32:27 (psf)

10000.

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 9333.

MODEL NOLIN2N STATIC STEP 3 8667.

-8000.

7333.

6667.

6000.

5333.

4667.

4000.

-3333.

2667.

2000.

1333.

666.7

FIGURE 37: Model NOLIN2N Static Step 3 Major Stress -.0001221

-....]

0

Page 83: Two Dimensional Finite Element Modeling of Swift Delta

Major Stress (psf) 10000.

Fringe: LC=2.14-RES=1.1-P3/PATRAN R.1-(Major)-AB~QUS-31-Aug-94 13:45:03

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 9333.

MODEL NOLIN2N STATIC STEP 5 8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7

-.0001221 --...J I-' FIGURE 38: Model NOLIN2N Static Step 5 Major Stress

Page 84: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3. 7-RES=1.1-P3/PATRAN R.1-{Major)-ABAQUS-12-0ct-94 18:33:29

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1N STATIC STEP 8

nolin1 n2.fil FIGURE 39: Model NOLIN2N Static Step 8 Major Stress

Major Stress (psf) 1 oooo.

9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7

-.0001221 .....J N

Page 85: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.17-AES=2.1-P3/PA TRAN R.1 ':'(T ensor-XX)-ABAQUS-23-Jul-94 16:54:29 HORIZ STRAIN

.001308

SWIFT DEL TA SOIL NAIL WALL FEM RESULTS .001061

MODEL NOLIN2N STATIC STEP 8 .0008126

.0005647

.0003168

.00006884

-.0001791

-.0004270

-.0006749

-.0009229

-.001171

-.001419

-.001667

-.001915

-.002163

nol in2n 1 . fil -.002410

FIGURE 40: Model NOLIN2N Static Step 8 Horiz. Strain .....]

w

Page 86: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.17-RES=4.1-P3/PATRAN R.1-(Vector-Y)-ABAOUS-23-Jul-94 17:06:55 VERT DISP

.05890

SWIFT DELTA SOIL NAIL WALL FEM RESULTS .05442

MODEL NOLIN2N STATIC STEP 8 .04994

.04547

.04099

.03651

.03203

.02756

.02308

.01860

.01412

.009645

.005167

.0006895

-.003788

nolin2n1 .fit

FIGURE 41: Model NOLIN2N Static Step 8 Vert. Disp. -.008266 - '1

~

Page 87: Two Dimensional Finite Element Modeling of Swift Delta

75

Section #1 Results

This report attempts the difficult task of solving a three

dimensional problem in two dimensions. Two separate models

were developed one with piles and nails present (nolinlp) and

the other with just the nails present (nolinln). The bridge

pile was inserted into the nolinlp model immediately after the

geostatic turn on was completed. This put the pile in the

model in a un-stressed state and the piles own self weight

stresses are not accounted for. Because of this it is

important to realize when analyzing the fringe plots for the

nolinlp and nolinln models that the nolinlp model has an

additional step and the same two model steps will not

correspond with the same excavation lifts. The following

sections presents the data for the two models simultaneously

and discusses the results in detail:

Horizontal Soil Stress

The horizontal stress fields for the two instrument section #1

models appear to be identical. Figures 43 through 48 present

the patran horizontal stress fringe plot results for nolinln

and nolinlp model steps 3, 5, and 8. The stress plots show a

very reasonable geostatic stress field at locations away from

the nail inclusions and clearly show the presence of the nails

as tensile elements.

Page 88: Two Dimensional Finite Element Modeling of Swift Delta

76

Vertical Stresses

The nolinlp fringe plot (Figure 49) clearly shows that the

piling was introduced at a zero stress state. In addition

there is some vertical stress imbalance in the pile at the

elevation of the bottom of the excavation lift. This vertical

stress imbalance is a sign that bending stresses are being

generated as a result of the excavation. Figures 50 and 51

show that new pile stresses are not introduced during

excavation lifts two and three. After excavation lift four

( Figure 52) some minor stress changes in the pile can be seen

above nail three. Again after excavation lift five, changes

in pile vertical stress can be seen ( Figure 53). At the

location were nail three intersects the pile continued minor

bending stresses have been developed. For reference nolinln

fringe plots are shown in Figure 3, 5, and 8 (Figures 54

through 56). These plots show vertical stress fields that are

consistent with the nolin2n plots and appear reasonable.

Nail Stresses

As discussed previously the nails in the first excavation lift

of nolinln and nolinlp appear to be introduced at a stress

level higher than the actual (Figures 57 and 58 respectively).

The major stress fringe plot for step 3 of the nolinln model

(Figure 57) also shows much higher tensile stresses in the

wall face (maximum 5,333 psf) than the corresponding maximum

tensile stress of 1,333 psf for the nolinlp model (Figure 58).

Page 89: Two Dimensional Finite Element Modeling of Swift Delta

77

It is important to note that the peak stresses for the nolinln

model are present at the back of the shotcrete wall face were

as the peak stresses for the nolinlp model are directly behind

the piling. This is because the nail and the pile are tied

together in the nolinlp model. Although this is not

geometrically correct it could be an approach to modeling

arching effects between the existing piling, nails, and

shotcrete face. Excavation step four shows a considerable

reduction in nail stress for nails three through four in the

nolinlp model (Figure 59) as compared with the nolinln model

(Figure 60). Closer inspection of figures 59 and 60 reveal

that there maybe significant pile nail interaction. This is

based on the fact that the nolinlp models stress is

distributed down a much shorter length of the nail than the

nolinln model. Logically if the pile had no nail interaction

effect in the nolinlp model than the nail stresses would be

the same as the nolinln model and shifted to the back of the

nail a distance equal to the pile diameter. This phenomenon

is also apparent in the last excavation lift ( Figures 61 and

62) but not as pronounced as in the previous excavation lift.

The effect maybe some what masked in the last excavation lift,

because a large overall stress redistribution takes place in

the existing nails due to the large lift height and the

steeper angle of the last nail.

Page 90: Two Dimensional Finite Element Modeling of Swift Delta

78

Pile Stresses

Most fringe plots were scaled in major stress from O to 1500

psf (tension) , for clarity other ranges were also used.

Figure 63 illustrates the true zero stress state that the pile

was installed under. After the first excavation lift ( Figure

64) shows the pile under going a stress change from zero

stress to one that is tensile. This appears to be a result of

the excavation unloading. The stress change is not

completely uniform and it is certain that some minor bending

stresses are introduced. Figure 65 further confirms that

tensile major stresses are induced in the pile as the

excavation sequence advances. Unfortunately it is very

difficult to determine true bending stresses. With this model

it is only safe to say that some bending stresses are being

developed.

Deflections

The same heaving of the excavation lift base has been

identified for both the nolinln and the nolinlp models as was

seen in the nolin2n model. The horizontal and vertical node

deflections for excavation lift 6 is identical for all three

models. An x-y plot of those displacements is presented in

Figure 66. This is reasonable since for the most part the

three models have identical conditions in front of the wall

face.

Page 91: Two Dimensional Finite Element Modeling of Swift Delta

79

Again the deflections correspond well with the vertical stress

fields in front of the wall as can be seen in Figure 56.

Figure 67 and 68 are x-y plots of the shotcrete wall

facing deflection profiles for the nolinln and nolinlp models

respectively. Both models show reasonable deflection of the

wall face with the maximum being at the top. The wall face

deflection are in proportion to the size of the excavation

lifts, which can be seen between excavation lifts one and two.

There is not a major contrast between the deflections for the

nolinln and nolinlp model and interestingly the nolinlp model

shows slightly more deflection (.033 ft) than the nolinln

model (.031 ft).

Figure 69 is a horizontal displacement fringe plot for

the nolinlp model after the insertion of the fifth nail (model

step 8). This plot clearly shows that the pile deflection is

in direct proportion to wall face deflection. Therefore the

pile cap translates the full .033 ft that the wall face did at

the end of excavation lift 6. This supports the fact that

some bending stresses were identified in early sections of

this report. For assistance in visualizing the pile bending

see figure 70 an exaggerated deformed mesh plot for the

nolinlp model.

Page 92: Two Dimensional Finite Element Modeling of Swift Delta

80

COMPARISON BETWEEN FEM RESULTS AND INSTRUMENT

MEASUREMENTS

The following section identifies the similarities and

discrepancies with the instrument data collected at the Swift

Delta wall.

Deflections

The field measurement data that will be used for comparison is

the single point pile cap extensometer located at Approx UV

Station 128+00 and the slope inclinometers SI 129 and SI 130

located at UV Stations 131+25 and 130+62 respectively. It is

important to note that SI 130 was a replacement inclinometer

for one that was destroyed during construction. Therefore it

does not cover full wall construction.

When interpreting soil nail wall deflection data it is

important to recall the following factors that effect wall

displacement:

Rate of construction

Height of excavation phases and spacing between nails

Extensibility of nails

Global safety factor of the wall

L/H ratio

Inclination of the nails and, in this case, their bending

stiffness

Page 93: Two Dimensional Finite Element Modeling of Swift Delta

81

Bearing capacity of the foundation soils 10

The nolin2n and nolinln wall face displacements are identical.

apparently the removal of the concrete pile cap was an even

exchange of overburden pressure for the 2H: 1 V soil slope.

This gives some validation to the nolinln model as being a

control section without the influence of the bridge pile to

the nolinlp model. Modeled wall displacements were slightly

less than those predicted by the h/1000 - 4h/1000 rule of

thumb however exceptionally good agreement was obtained

between the single point extensometer (max deflection= .32

inches from figure 7) and the ABAQUS models (max deflection=

. 4 inches from figure 6 8) . The two slope inclinometers

recorded higher deflections than those of the abaqus model and

the extensometer. SI 130 had a maximum deflection of

approximately .7 inches (Figure 9) and SI 129 had a maximum

deflection of approximately .5 inches (Figure 8). The higher

deflections can be attributed in part to excessive sloughing

of material during construction. This slough occurred in the

vicinity of both SI 130 and SI 129. Another reason for the

higher monitored deflections was the length of time it took

for construction in the area of the two slope inclinometers.

In this area it took longer than that under the bridge near

instrument section #1. This may be something to consider for

10 Recommendations Clouterre 1991 (Presses Pants et chaussees) ,p.55

Page 94: Two Dimensional Finite Element Modeling of Swift Delta

82

future FE modeling and that is to incorporate a time function.

The horizontal displacement fringe plot in figure 69

clearly shows that the nailed zone behaves as a gravity block.

This is the way soil nail walls are suspected to behave and

give strong validation to the ABAQUS modeling techniques used.

Measured Nail Stresses

The field measurement data that will be used for comparison

are the nail strain gages and load cells. Due to the modelia

soil nail with ABAQUS and the resulting high initial stress

states, direct comparison of nail stresses or loads will not

be made. Instead the nail stress distributions from the

ABAQUS models will be compared to the reduced nail loads that

were developed from the instrument data (figures 71 through

76). The measured data is not plotted with respect to lift

sequence but rather the date it was recorded on. The actual

construction lift dates are as follows: Lift 1 - Completed

12/10/90

Lift 2 - Completed 12/12/90

Lift 3 - Completed 1/8/90

Lift 4 - Completed 1/16/91

Lift 5.-- Completed 1/24/91

For ease of comparison of the model data to the

instrument data the nolinln, nolinlp, and nolin2n nail

stresses were plotted versus nail length (figures 77 through

85). In general the stress trends in the ABAQAS models

Page 95: Two Dimensional Finite Element Modeling of Swift Delta

83

nolinln, nolinlp, and nolin2n compare well with the measured

loads. In particular the instrument section one - nail one,

load distribution compares well with the nolinln and nolinlp

models. Some of the apparent random load measured in

instrument section two compares well enough to the nolin2n

model to make one reconsider it's randomness.

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.03487

SWIFT DELTA SOIL NAIL WALL FEM RESULTS .03254

MODEL NOLIN2N STATIC STEP 8 .03021

.02788

.02556

.02323

.02090

.01857

.01624

.01391

.01159

.009259

A006930

.004602

.002274

nolin2n 1.f ii FIGURE 42: Model NOLIN2N static Step 8 Horiz. Oisp~ -.00005384 (X) ~

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SWIFT DEL TA SOIL NAIL FEM RESULTS

MODEL NOLIN1 N STATIC STEP 3

nolin1n3.fil FTGURE 43: Model NOLINlN Static Step 3 Horiz · Stress

Horiz Stress (psf)

0.

-233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. ()) U1

. ,

Page 98: Two Dimensional Finite Element Modeling of Swift Delta

Horiz Stress (psf)

0. Fringe: LC=3.3-RES=1.1-P3/PA TRAN R.1-(T ensor-XX)-ABAQUS-13-Aug-94 12:49:31

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 4 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. 00 O'I

nolin1 p3.fil FIGURE 44: Model NOLINlP Static Step 4 Horiz. Stress

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SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 5

nolin 1 n3.fil FIGURE 45: Model NOLINlN Static Step 5 Horiz. Stress·

Horiz Stress (psf)

0.

-233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. OJ .......i

Page 100: Two Dimensional Finite Element Modeling of Swift Delta

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SWIFT DELTA SOIL NAIL WALL FEM RESULTS 0.

MODEL NOLIN1P STATIC STEP 6 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. (X)

nolin1p3.fil FIGURE 46: Model NOLINlP Statiq Step 6 Horiz. Stress (X)

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SWIFT DELTA SOIL NAIL WALL FEM RESULTS 0.

MODEL NOLIN1P STATIC STEP 9 -233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

nolin1 p3.fil FIGURE 47: Model NOLINlP Static Step 9 Horiz. Stress -3500. 00 ~

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SWIFT DEL TA FINITE ELEMENT MESH -233.3

NOLIN1N MODEL STEP 8 -466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

FIGURE 48: NOLINlN Model Static Step_~ Horiz. Stress, -3267.

-3500. \..0 0

Page 103: Two Dimensional Finite Element Modeling of Swift Delta

Vert Stress (psf)

0. Fringe: LC=3.3-RES=1.1-P3/PATRAN R.1-(Tensor-YY)-ABAQUS-13-Aug-94 12:21:58

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 4 -233.3

-466.7

-700.0-

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333. -

-2567.

-2800.

-3033.

-3267.

-3500. ~ ......

nolin1 p3.fil FIGURE 49: Model NOLINlP Static Step 8 Vert. Stress

Page 104: Two Dimensional Finite Element Modeling of Swift Delta

' Fringe: LC=3.4-RES=1.1-P3/PATRAN R._1-(Tensor-YY)-ABAQUS-13-Aug-9413:13:16

SWIFT DELTA SOIL NAIL WALL FEM RESULTS· Vert Stress

(psf) 0.

MODEL NOLIN1 P STATIC STEP 5 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

nolin1 p3.fil FIGURE 50: Model NOLINlP Static Step 5 Vert. Stress -3500.

l.O f\..)

Page 105: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PATRAN R1-(Tensor-YY)-ABAQUS-13-Aug-94 13:57:46 . .

SWIFT DELTA SOIL NAIL WALL FEM RESULTS Vert Stress

0.

MODEL NOLIN1P STATIC STEP 6 -233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

nolin1 p3.fil FIGURE 51: Model NOLINlP Static Step 6 Vert. Stress -3500.

\.D w

Page 106: Two Dimensional Finite Element Modeling of Swift Delta

Vert Stress (psf)

0.

Fringe: LC=3.6-RES=1.1-P3/PATRAN R 1-(T ensor-YY)-ABAQUS-03-Sep-94 14:56:44

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 7 -233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

-3500. -~

nolin1 p3.fil FIGURE 52: Model NOLINlP Static Step 7 Vert. Stress

~

Page 107: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC:::3.8-RES=1 .1-P3/PATRAN R.1-(f ensor-YY)-ABAQUS-21-May-94 12:54:22 Vert Stress

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 0.

MODEL NOLIN1P STATIC STEP 9 -233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

- -2333.

-2567.

-2800.

-3033.

-3267.

nolin1 p3.fil . FIGURE 53: Model NOLINlP Static Step 9 Vert. Stress

-3500. \,0 l1l

Page 108: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.2-RES=1.1-P3/PATRAN R.1-{Tensor-YY)-ABAQUS-31-Aug-94 09:55:34 .

SWIFT DELTA~SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 3

nolin1 n3.fil

FIGURE 54: Model NONLINlN Static Step 3 Vert. Stress

Vert Stress (psf)

0.

-233.3

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100 .

. -2333.

-2567.

-2800.

-3033.

-3267.

-3500.

Page 109: Two Dimensional Finite Element Modeling of Swift Delta

Vert Stress {psf)

0.

Fringe: LC=3.4-RES=1.1-P3/PATRAN R.1-(Tensor-YY}-ABAQUS-31-Aug-94 11 :11 :44

SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 5 -233.3

-466.7

-700.0_

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333 ..

-2567.

-2800.

-3033.

nolin 1 n3.fil -3267.

-3500. ~

FIGURE 55: Model NONLINlN Static Step 5 Vert. Stress '-.)

Page 110: Two Dimensional Finite Element Modeling of Swift Delta

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SWIFT DELTA FINITE ELEMENT MESH 0.

-233.3 NOLIN1 N MODEL STEP 8

-466.7

- -700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

FIGURE 56: NONLINlN Model Step 8 Vert Stress -3500.

\!) (X)

Page 111: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.2·RES;;1.1 ·P3/PA TRAN R.1 ·(Major)-ABAQUS-31 ·Aug-94 10:01: 13 .

SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 3

nolin 1 n3.fil FIGURE 57: Model NONLINlN Static Step 3 Major Stress

Major Stress (psf) 10000.

9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7

-.0001221 l.O l.O

Page 112: Two Dimensional Finite Element Modeling of Swift Delta

Major Stress

(psf~oooo. Fringe: LC=3.3-RES=1.1-P3/PATRAN R.1-{Major)-ABAQUS-13-Aug-94 12:44:44 .

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 4 9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---.X 1333.

666.7

-.0001221 ......

nolin1 p3.fil FIGURE 58: Model NONLINlP Static Step 4 Major Stress' 0 0

Page 113: Two Dimensional Finite Element Modeling of Swift Delta

Major Stress

(psf~oooo. Fringe: LC=3.6-RES=1.1-P3/PATRAN R.1-{Major)-ABA9US-03-Sep-94 15:02:30

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 7 9333.

8667.

- 8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7

-.0001221 I-' 0

nolin 1 p3. fil FIGURE 59: Model NONLINlP Static Step 7 Major Stress

I-'

Page 114: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PATRAN R.1-(Major)-ABAQUS-31-Aug-94 11 :33:38 .

SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 6

nolin 1 n3.fil FIGURE 60: Model NONLINlN Static Step 6 Major Stress

Major Stress (psf) 10000.

9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7

-.0001221 ....... 0 I\.)

Page 115: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.8-RES=1 .1-P3/PATRAN R.1-(Major)-ABAQUS-21-May-94 13:00:51 Major Stress

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 10000.

MODEL NOLIN1P STATIC STEP 9 9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

---X 1333.

666.7

nolin1 p3.fil FIGURE 61: Model NONLINlP Static Step 9 Major Stress

-.0001221 ........ 0 w

Page 116: Two Dimensional Finite Element Modeling of Swift Delta

•.

Fringe~ LC=3.7-RES=1.1-P3/PATRAN R1-(Major)-ABAOUS-09-0ct-9416:31:49 .

SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1 N STATIC STEP 8

~

no I in 1 n3.fil

FIGURE 62: Model NONLIN!P Static Step 8 Major Stress I '

Major Stress (psf) 10000.

9333.

8667.

8000.

7333.

6667.

6000.

5333.

4667.

4000.

3333.

2667.

2000.

1333.

666.7 '

-.0001221 ...... 0 .i:::.

Page 117: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC-=3.2-RES= 1 .1-P3/PA TRAN R.1-(Major)-ABAQUS-13-May-94 16:39:03 . '

SWIFT DELTA SOIL NAIL WALL FEM RESULTS

Major Stres (psf)

0.

... MODEL NOLIN1P STATIC STEP 3 -.6667

-1.333

- -2.000

-2.667

~ -3.333

-4.000

-4.667

·5.333

""6.000

-6.667

-7.333

-8.000

-8.667

-9.333

nolin1 p3.fil FIGURE 63: Model NONLINlP Static Step 3 Major Stress

t I

-10.00 1--' 0 U1

Page 118: Two Dimensional Finite Element Modeling of Swift Delta

Major Stress

(psf) 1500. Fringe: LC=3.3-RES=1.1-P3/PATRAN R.1-{Major)-ABj\QUS-13-Aug-94 12:58:26

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 4 1400.

1300.

1200.

1100.

1000.

900.0

800.0

700.0

600.0

500.0

400.0

300.0

200.0

100.0

0. I-'

nolin1 p3.fil FIGURE 64: Model NONLINlP Static Step 4 Major Stress 0 O"\

Page 119: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PATRAN R.1-{Major)-ABA9US-13-Aug-94 14:04:20

SWIFT DELTA SOIL NAIL WALL FEM RESULTS MODEL NOLIN1P STATIC STEP 6

nolin1 p3.fil FIGURE 65: Model NONLINlP Static Step 6 Major Stress

Major Stress

1500.

1400.

1300.

1200.

1100.

1000.

900.0

800.0

700.0

600.0

500.0

400.0

300.0

200.0

100.0

0.

Page 120: Two Dimensional Finite Element Modeling of Swift Delta

0.05

0.045

0.04

..-.. 0.035 iE.. c 0.03 0

+=' 0.025 (.) Q)

;+::::: 0.02 Q)

0 0.015

0.01

0.005

0 0

,

Swift Delta FEM Results Lift #6 Excav Deflec vs Dist from Fae~

,,,'!< ...

;x'

... ... )(·-·---·:.<·-·-·-·-~·-·-·-·-·-><·-·-·-·-···-)(·-·-·-···-···-><·-·-·-·-·-·-·-·->< x--·-

................................................................................ _ .............. _ ............ __ ... _ .. ,_ ... ..

5 10 15 20 25 30 35 Distance From Wall Face

1--·•···- Horiz Disp ---~·-· Vert Disp

FIGURE 66: Soil Excavation Lift Displacement

108

40

Page 121: Two Dimensional Finite Element Modeling of Swift Delta

Swift Delta FEM Results Shotcrete Face Deflection vs Height

109

0.035--.----------------------.

+::" LL 0.03 - l~#al (

351 -

~

c 0 0.025 u ~ 0.02 -Q.)

0 0.015

~ O.D1 t • _. !Ex #1 I jnolin1n I, 1

,

1

I 0 005 7 I I I I I . 0 2 4 6 8 10 12 14 16 18 20

Distance Down Face (Ft)

----- Lift #1 -+- Lift #2 --*- Lift #3

-a- Lift #4 -x- Lift #5 __._ Lift #6

FIGURE 67: NONLINl Wall Face Deflection

Page 122: Two Dimensional Finite Element Modeling of Swift Delta

0.035

-:;:;-0.03 LL -c:

0 :.;::::::; 0.025 (.) CD CD - 0.02 CD

Cl CD (.)

0.015 ell LL

0.01 0

Swift Delta FEM Results Shotcrete Face Deflection vs Height

I Ex Level #2 j ~------'..c;:x Level #5 Ex Level #4 ,___ __ _

I Ex Level #3 j

I Ex Level #61

!Ex Level #1 I jnolin1p I

110

2 4 6 8 1 0 1 2 1 4 1 6 1 8 20 -· Distance Down Face (Ft)

-II- Lift # 1 -+- Lift #2 ---*-- Lift #3

-a- Lift #4 -x-- Lift #5 __.._ Lift #6

FIGURE 68: NONLINlP Wall Face Deflection

Page 123: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3. 7-RES=4.1-P3/PATRAN A.1-0/ ector-X)-ABAQUS-17-Sep-94 14:34:09 Horiz Disp

SWIFT DELTA-SOIL NAIL WALL FEM RESULTS .03511

MODEL NOLIN1P STATIC STEP 8 .03262

.03014

.02766

.02518

.02269

.02021

.01773

.01525

.01276

.01028

.007800

.005318

.002835

.0003526

nolin1 p3.fil FIGURE 69: Model NONLINlP Step 8.Horiz .. Disp. -.002130

~ . I-' . I-'

Page 124: Two Dimensional Finite Element Modeling of Swift Delta
Page 125: Two Dimensional Finite Element Modeling of Swift Delta

-;; a.

14

12

10

;g 8 ~ 0 ..J

.iii z 6 iii ·x <

4

2

!Tensile Nail Loads During Construction, Section.·1, iRow 11 113

FIGURE 71: Instrument Section 1 Row 1 and 2 Nail Loads

Page 126: Two Dimensional Finite Element Modeling of Swift Delta

Tensile Nail Loads During Construction, Section (. Rbw 3 14

12

10

iii ~ ~ 8 IV 0 _,

"jij z ~ ><

<(

-;; a. a ,, IV 0 -' "jij z ii ·;;c <(

6

4

2

-- !?: ?:>'}. I .· I I d. I I I I I 0 I ~ I 20 0 10 15 25' 5

Nail length From Wall Face (feet)

--{)-- 12-27:90 -:.:- 1-2-91 -.--1-5-91 -+--1-10-91

-+-- 1-16-91 --<>-- 1-26-91 -x- 2-16-91 ---- 3-16-91

Tensile Nail Loads During Construction, Section 1, Row 4 14

'l 1 '(j' 111

12

10

8 .~x =---<>-----o.

6

4

2

0

0 5 10 15 20 25 Nail Length From Wall Face (feet)

--0- 1-16-91 --+- 1-26-91 --+-- 1-31-91 --<>--- 2-16-91 -x- 3-16-91

FIGURE 72: Instrument Section 1 Ro.w 3 and 4 Nail Loads

114

Page 127: Two Dimensional Finite Element Modeling of Swift Delta

115

Tensile Nail Loads During Construction, Section 1, Row 5 14

12

10

";;' a. ;g

8 i:i IV 0

...J

~ z 6 iii )(

<

4

2

o I 1v I I ~-------

0 5 10 15 20 25 Nail Length From Wall Face (feetl

-0-- 1-26-91 -~-1-28-91 2-16-91 --0--- 3-6-91 -x- 3-16-91

FIGURE 73: Instrument Section 1 Row 5 Nail Loads

Page 128: Two Dimensional Finite Element Modeling of Swift Delta

-;; a. ~ "O

I Ill 0

...J

~ z ii ")(

<

-;; a. ;g "O

"' 0 ...J

"iij z "iii ")(

<

14

12

10

a

6

4

2

0

0

14

12

10

8

6

4

2

0

0

Tensile Nail Loads During Construction, Section 2, Row 1

5 10 15

Nail length From Wall Face (feet)

-0-- 12-10-90 --0--- 12-13-90 --+-- 12-18-90

Tensile Nail Loads During Construction, Section 2, Row 2

5

--0-- 12-21-90

-x- 1-31-91

10 15

Nail length From Wall Face (feet)

*

12-27-90

2-27-91

• 1-2-91

20 25

1-16-91 -:t::- 3-16-91

20 25

~ 1-16-91

FIGuRE 74: Instrument Section 2 Row 1 And 2 Nail Loads

116

Page 129: Two Dimensional Finite Element Modeling of Swift Delta

Tensile Nail loads During Construction, Section 2, Row 3 117 14

12

10

;;; a. ;g

8 "O

"' 0 ...J

"ii z 6 ii )(

<

4

2

0

0 5 10 15 20 25

Nail Length From Wall Face (feet)

• 12-27-90 ---0-- 1-5-91 1-10-91 ----- 1-16-91

----0- 1-31-91 -x- 3-16-91

Tensile Nail loads During Construction, Section 2, Row 4 14

12

10

;;; a. ;g

8 "O

"' 0 ...J

"ii z 6 ii ·;:c <

4

2

0

0 5 10 15 20 25

Nail Length From Wall Face (feet)

-0-- 1-16-91 1-26-91 • 1-31-91 --0-- 2-16-91 -x- 3-16-91

FIGURE 75: Instrument Section 2 Row 3 And 4 Nail Loads

Page 130: Two Dimensional Finite Element Modeling of Swift Delta

118

Tensile Nail Loads During Construction, Section 2, Row 5 14

12

10

iii a. ~ 8 "O

"' 0 ..J

·n; z 6 ni ·;c <

4

2

0

0 5 10 15 20 25

Nail Length From Wall Face (feet)

--0-- 1·26-91 1 ·31-91 • 2·16-91 -x- 3·2·91 -tr-- 3-16-91

FIGURE 76: Instrument Section 2 Row 5 Nail Loads

Page 131: Two Dimensional Finite Element Modeling of Swift Delta

Swift Delta FEM Results 119

Nail #1 Stress vs Nail Length (nolin1 n)

7000

6000

c ~ 5000 en en

4000 (],) lo.. .....

Cf)

"ffi 3000 z

1000 I I I I I I I I I I 0 2 4 6 8 10 12 14 16 18

9000

8000

c 7000 en -3: 6000 en en

5000 ~ -Cf) 4000

·~

z 3000

2000

1000 0

Distance Along Nail (Ft)

---- Lift #1 --+--Lift #2 ~Lift #3

-a- Lift #4 ~ Lift #5 ......_ Lift #6

Nail #2 Stress vs Nail Length (nolin1 n)

2 I I

1'0 1'2 4 6 8 Distance Along Nail (Ft)

--+-- Lift #2 ~ Lift #3 -a- Lift #4

~ Lift #5 ......_ Lift #6

14 16

FIGURE 77: NONLINlN Nail 1 and 2 Stresses

18

Page 132: Two Dimensional Finite Element Modeling of Swift Delta

c CJ) Q. .__. CJ) CJ) Q) .....

U5 "Cij z

c CJ)

9000

8000

7000

Swift Delta FEM Results Nail #3 Stress vs Nail Length (nolin1 n)

s 6000 CJ) CJ)

5000 Q) ..... Ci5 "Cij 4000 z

3000-J s---8

2000-l~

1000 0 2 4 6 8 1 0 1 2 1 4 1 6 1 8 20

Distance AJong Nail (Ft)

I -?IE- Lift #3 -B- Lift #4 ~ Lift #5 --..-- Lift #6

Nail #4 Stress vs Nail Length (nolin1 n) 121~ I 11

10

<ii 9 -0 c 8 co CJ) :J 0 7 ..c c 6

31 I I I I I I - - I 0 -2 4 6 8 10 12 14 16 18 Distance Along Nail (Ft)

/ -s- Lift #4 ~ Lift #5 --..-- Lift #6

FIGURE 78: NONLINlN Nail 3 and 4 stresses

120

Page 133: Two Dimensional Finite Element Modeling of Swift Delta

c

25

20

(/) -a. en _. "O 15 (/) c (/) "' <D en ~ ::J

(j) _g 10 ·- f-ell -z

5

0

Swift Delta FEM Results Nail #5 Stress vs Nail Length (nolin1 n)

0 2 4 6 8 10 12 14 16 18 Distance Along Nail (Ft)

1--')E- Lift #5 __.__ Lift #6 I

FIGURE 79: NONLINlN Nail 5 Stress

121

Page 134: Two Dimensional Finite Element Modeling of Swift Delta

Swift Delta FEM Results 122

Nail #1 Stress vs Nail Length (nolin1 p) 7000

6000 c s 5000 en ~ 4000 +-' (/)

~ 3000 z

2000

1000" I I I

1'0 0 2 4 6 8 12 14 16 18

Distance Along Nail (Ft)

--- Lift #1 -+- Lift #2 ~ Lift #3

-e- Lift #4 --*-- Lift #5 ___.__ Lift #6

Nail #2 Stress vs Nail Length (nolin1 p) 7000

6000

~ 5000 s en 4000 en Q.) t....

Ci5 3000 ·ro

2000 z

1000

0 2 4 6 8 10 12 14 16 18

Distance Along Nail (Ft)

-+- Lift #2--"*- Lift #3 -e- Lift #4

--*-- Lift #5 __._ Lift #6

FIGURE 80: NONLINlP Nail 1 And 2 Stresses

Page 135: Two Dimensional Finite Element Modeling of Swift Delta

8000

7000

C' 6000 en s en 5000 en Q.) ,_ .... 4000 (f)

·~ z 3000

2000

1000 0

10000

Swift Delta FEM Results Nail #3 Stress vs Nail Length (nolin1 p)

2 4 6 8 1 0 1 2 1 4 1 6 1 8 20 Distance Along Nail (Ft)

I -71E- Lift #3 -a- Lift #4 ~ Lift #5 _...._ Lift #6

Nail #4 Stress vs Nail Length (nolin1 p)

9000

8000 C' en s 7000 en en

6000 ~ .... (f)

·~ 5000

z 4000

3000

2000 0 5 10 15 20 25

Distance Along Nail (Ft)

1-a-- Lift #4 ~ Lift #5 __.__ Lift #6

FIGURE 81: NONLINlP Nail 3 And 4 Stresses

123

Page 136: Two Dimensional Finite Element Modeling of Swift Delta

c-en -cn Q. - "O en c en ~ CJ) en ...... ::i (j) 0

..c '(ij t:.. z

20

18

16

14

12

10

8

6

4

2 0

Swift Delta FEM Results Nail #5 Stress vs Nail Length (nolin1 p)

2 4 6 8 10 12 14 16 18 Distance Along Nail (Ft)

/-x- Lift #5 __._ Lift #6

FIGURE 82: NONLINlP Nail 5 And 4 Stresses

124

Page 137: Two Dimensional Finite Element Modeling of Swift Delta

7000

6000 c s 5000 (/J (/J

4000 ~ (i)

"ffi 3000 z

2000

1000 0

9000

8000

c 7000 (/J

s 6000 (/J (/J

5000 Q) ..... +-' (/)

4000 "ffi z 3000

2000

1000'

Swift Delta FEM Results Nail #1 Stress vs Nail Length (nolin2n)

2 4 6 8 10 12 14 16 Distance Along Nail (Ft)

--- Lift #1 --+-- Lift #2 ~ Lift #3

-a- Lift #4 ~ Lift #5 __,._ Lift #6

Nail #2 Stress vs Nail Length (nolin2n)

0 2 4 6 8 10 12 14 16 Distance Along Nail (Ft)

--+-- Lift #2 ---*-- Lift #3 -Er- Lift #4

~ Lift #5 __,._ Lift #6

FIGURE 83: NONLIN2N Nail 1 And 2 Stresses

125

18

18

Page 138: Two Dimensional Finite Element Modeling of Swift Delta

c (/J

9000

8000

7000

Swift Delta FEM Results Nail #3 Stress vs Nail Length (noli2n)

·S 6000 (/J (/J

5000 Q) ~ ......

(/)

'Cij 4000 z

3000

2000

1000 0 2 4 6 8 10 12 14

Distance Along Nail (Ft) 16 18 20

/-s- Lift #4 --.><- Lift #5 __.__ Lift#~

12 Nail #4 Stress vs Nail Length (nolin2n)

11

10 c (/J en 9 0..

- "O (/J c (/J cu Q) (/J ~ :J ......

(/) 0 .c

'Cij I--z

8

7

6

5

4

31 I I I I I I - I I - j 0 ? A a "' ~- ·-, " 4 6 8 10 12 14 16 18

Distance Along Nail (Ft)

/ -a- Lift #4 ~ Lift #5 ......_ Lift #6

FIGURE 84: NONLIN2N Nail 3 And 4 Stresses

126

Page 139: Two Dimensional Finite Element Modeling of Swift Delta

22

20

c 18 (/J -Q. (/J - ~ (/J c: 16 (/J n1 CD C/J ._ :J

....... 0 14 (/) ..c ·- .._ n1 -z 12

10

8

Swift Delta FEM Results Nail #5 Stress vs Nail Length (nolin2n)

0 2 4 6 8 10 12 14 16 18 Distance Along Nail (Ft)

I ~ Lift #5 _..__ Lift #6

FIGURE 85: NONLIN2N Nail 5

127

Page 140: Two Dimensional Finite Element Modeling of Swift Delta

128

CONCLUSIONS AND FURTHER STUDY

At the time that this project was started no other FE codes

written specifically for soil nail walls was available. The

application of ABAQUS was not routine and the general purpose

FE code was not soil nail frMidly. Even with this good

comparison of modeled deflections to measured data (figure 86)

give some support to the validity of the ABAQUS models.

However, comparison of predicted nail stresses to measured did

not show particularly good agreement. This is in part due to

the difficulty in modeling soil nails which mainly lies with

the variability in grouting and nail/soil modulus

incompatibility. The results of this report indicate that the

presence of the pile within the nail zone results in lower

over all nail stresses. This is possibly due to soil arching

between piling. The nail zone was found to form a gravity

block. Within this block horizontal displacements were found

to be relatively uniform. This type of movement confirms what

has been suggested by others, and that is that soil nail walls

behave in a gravity block fashion. With this type of behavior

and considering the piling. The piling has to be deflecting

with the soil mass and under going new bending stresses.

Page 141: Two Dimensional Finite Element Modeling of Swift Delta

129

Further study in this area could include continued FEM

work with nails that more correctly model the initial stress

state. A time function should be considered to simulate

actual construction time. In addition more full scale studies

of pile supported bridge abutment/nail walls should be

performed. These studies should incorporate piling

instrumentation to accurately measure any nail wall induced

bending. The future modeling results and measurements should

be combined and used to form a design procedure for pile

supported abutments with nail walls in front of them.

Page 142: Two Dimensional Finite Element Modeling of Swift Delta

130

Swift Delta FEM Results Measured and Predicted Face Deflection

0.45

- 0.4 c :::=.. c

0.35 0 +:i (.) Q)

0.3 Q) I'+-

Q)

0 0.25 Q) (.) ctl

0.2 LL.

0.15 0 4 8 12 16 20

Distance Down Face (Ft)

/ ~ Measured Sl-130 --+- Predicted nolin2n

FIGURE 86: Measured and Predicted Wall Face Deflection

Page 143: Two Dimensional Finite Element Modeling of Swift Delta

S3::>I GN3:ddV

1£1

Page 144: Two Dimensional Finite Element Modeling of Swift Delta

NO I .L V .LN3:WmI.L SN I

Page 145: Two Dimensional Finite Element Modeling of Swift Delta

I TABLE A-I

Swift Delta Instrumentation

Instrument Type Manufacturer Model Readout Units

Vibrating Wire Geokon/RST VK4100 Micro Strain Strain Gages

Load Cell Carlson/RST SCA-100- Micro Strain 1.5x4.00

Pneumatic Earth SIN CO 51408200 psi Cell

Tiltmeter/Plates SIN CO 2(sin)theta 50304400/503 2300

Single Point RST EX-1 In Extesometer

Survey Tag Line Wild EDM T-16 Feet

Load Cell RST Micro E 350 Micro Read Out Strain

Strain Gage Geokon/RST GK-401 Micro Readout Strain

Earth Pressure SIN CO Cell Readout

LVDT RST EX-1 In Extensometers

Accuracy

+/-1 Micro E

.25%

1 in 10,000

.05 Ft

+/- 1

+/-1 psi

+/-1 psi

1 in 100

Qty

58

6

2

3

1

2

1

1

1

2

I

...... w w

.1

Page 146: Two Dimensional Finite Element Modeling of Swift Delta

~~Id iliildNI dN1NI~ON g XIQN~ddV

v£1

Page 147: Two Dimensional Finite Element Modeling of Swift Delta

-

*DENSITY 145.0 ** *INITIAL CONDITIONS, TYPE=STRESS, GEOSTATIC SOIL,0.0,35,-3500.0,0.0,1.0 **

135

**------ REMOVAL OF ELEMENTS TO BE INSTALLED DURRING CONSTRUCTION -----------­*STEP, AMPLITUDE=RAMP ** LOAD 1 REMOVAL OF ELEMENTS TO BE ADDED LATER. ** *STATIC *DLpAD *MODEL CHANGE, REMOVE PILE *MODEL qHANGE, REMOVE APlSC *MODEL CHANGE, REMOVE AP2SC *MODEL CHANGE, REMOVE AP3SC *MODEL CHANGE, REMOVE AP4SC *MODEL CHANGE, REMOVE AP5SC *MODEL CHANGE, REMOVE AP6SC *MODEL CHANGE, REMOVE NAILl *MODEL CHANGE, REMOVE NAIL2 *MODEL CHANGE, REMOVE NAIL3 *MODEL CHANGE, REMOVE NAIL4 *MODEL CHANGE, REMOVE NAILS ** *END STEP ** ** *STEP, AMPLITUDE=RAMP **-----------------GRAVITY CONDITIONS--------------------------------------**------------------------------------------------------------------------** ** **-----------------GRAVITY LOAD-------------------------------------­**-------------------------------------------------------------------** LOAD 2 APPLICATION OF GEOSTATIC STRSS *GEOSTATIC *DLOAD, OP=NEW SOIL,BY,-102.0 ** ** ** **------------------BOUNDARY CONDITIONS---------------------------------** *BOUNDARY,

1, 2' 4, 6, 8,

10, 12,

OP=NEW 1,' 0. 0 1, I 0 • 0 1,' o. 0 1,' 0. 0 1,' 0. 0 1,' o. 0 l, I 0 • 0

Page 148: Two Dimensional Finite Element Modeling of Swift Delta

465, 6, I o.o 475, 1, I 0.0 475, 3 It o.o 475, 4 t I 0.0 475, 5,, 0.0 475, 6 It 0.0 478, 1,, 0.0 478, 3, t 0.0 478, 4 t I 0.0 478, 5,' 0.0 478, 6, I 0.0 485, 1,' 0.0

l 485, 3 It 0.0 485, 4 I I 0.0 485, 5, I o.o 485, 6, I 0.0 487, 1,, 0.0 487, 3 I I 0.0 487, 4,, 0.0 487, 5,' 0.0 487, 6,' 0.0 491, 1, I 0.0 491, 3,, 0.0 491, 4,' 0.0 491, 5,, 0.0 491, 6,, 0.0 492, 1·, I 0.0 492, 3,, 0.0 492, 4 I I 0.0 492, 5,, 0.0

"492, 6, I 0.0 493, 1,, 0.0 493, 3 t I 0.0 493, 4 t I 0.0 493, 5, I 0.0 493, 6, t 0.0

** ** *EL FI~E, s

POSITION=CENTROIDAL

SINV ·E

EE ** *NODE FILE, GLOBAL= YES u *EL PR+NT, ELSET=NAILl ,POSITION=CENTRODIAL s SINV E EE *EL PRINT, ELSET=NAIL2, POSITION=CENTRODIAL s SINV E EE ** *END STEP ** **-----------------------PILE INSTALATION------------------------------­*STEP, AMPLITUDE=RAMP *STATIC *DLOAD **----------------------Remove Pile Soil Elements---------------------­*MODEL CHANGE, REMOVE PI LEX

136

Page 149: Two Dimensional Finite Element Modeling of Swift Delta

**--------------------- Add Pile Elements------------------------------­*MODEL CHANGE, INCLUDE PILE *EL FILE, POSITION=CENTRODIAL s E SINV EE *END STEP ** **-----------------------EXCAVATION LIFT #1------------------------------**-----------------------------------------------------------------------** *STEP, AMPLITUDE=RAMP LOAD 3 Excavation of soil lift and the instalation of Nail#l *STATIC *DLOAD **---------------- Remove Soil Slope for Lift #1 --------------------­*MODEL CHANGE, REMOVE EXlS **--------------- Add Shotcrete to newly cut soil face --------------­*MODEL CHANGE, INCLUDE APlSC **---------------Remove Soil in nail location (drill)--------------­*MODEL CHANGE, REMOVE SNELl **---------------- Install soil nail in wall *MODEL CHANGE, INCLUDE NAILl ** *EL FILE, POSITION=CENTRODIAL s E SINV EE *NODE FILE, GLOBAL=YES u . *EL PRINT, ELSET=PNAILl, POSITION=CENTRODIAL s SINV E EE * * I

*NODE PRINT, NSET=FACEl u ** *NODE PRINT, NSET=Hl u '• * *END STEP **

, I ------------------------

137

**---------------------- EXCAVATION LIFT #2 -------------------------------­*STEP, AMPLITUDE=RAMP LOAD 4 Excavation of soil lift #2 and the installation of Nail#2 *STATIC *DLOAD **--------------- Remove Soil Slope for Lift #2 --------------------------­*MODEL CHANGE, REMOVE EX2S **----------------- Add Shotcrete to Newly Cut Soil Face ----------------­*MODEL CHANGE, INCLUDE AP2SC **----------------- Remove Soil in Nail Location -------------------------­*MODEL CHANGE, REMOVE SNEL2 **----------------- Install Soil Nail in Wall -----------------------------

Page 150: Two Dimensional Finite Element Modeling of Swift Delta

*MODEL CHANGE, INCLUDE NAIL2 ** *EL FILE, POSITION=CENTRODIAL s E SINV EE ** *NODE FILE, GLOBAL=YES u ** *EL PRINT, ELSET=PNAIL2, POSITION=CENTRODIAL s E ** *NODE PRINT, NSET=FACEl u ** *NODE PRINT, NSET=H2 u ** *END STEP ** **---------------------- EXCAVATION LIFT #3 -------------------------------­*STEP, AMPLITUDE=RAMP LOAD 5 Excavation of soil lift #3 and the installation of Nail#3 ~STATIC

*DLOAD **--------------- Remove Soil Slope for Lift #3 ---------------------------*MODEL CHANGE, REMOVE . EX3S **-------------~--- Add Shotcrete to Newly Cut Soil Face ----------------­*MODEL CHANGE, INCLUDE AP3SC **----------------- Remove Soil in Nail Location --------------------------*MODEL CHANGE, REMOVE SNEL3

~

**----------------- Install *MODEL CHANGE, INCLUDE NAIL3

Soil Nail in Wall -----------------------------

** *EL FILE, POSITION=CENTRODIAL s E SINV EE *NODE FILE, GLOBAL=YES u *EL PRINT, ELSET=PNAIL3, POSITION=CENTRODIAL s E ** *NODE PRINT, NSET=H3 u ** *NODE PRINT, NSET=FACEl u ** *END STEP ** **---------------------- EXCAVATION LIFT #4 -------------------------------­*STEP, AMPLITUDE=RAMP LOAD 6 Excavation of soil lift #4 and the installation of Nail#4 *STATIC *DLOAD

138

Page 151: Two Dimensional Finite Element Modeling of Swift Delta

**--------------- Remove Soil Slope for Lift #4 --------------------------- 139 *MODEL CHANGE, REMOVE EX4S **----------------- Add Shotcrete to Newly Cut Soil Face ----------------­*MODEL CHANGE, INCLUDE AP4SC **----------------- Remove Soil in Nail Location -------------------------­*MODEL CHANGE, REMOVE SNEL4 **----------------- Install Soil Nail in Wall ----------------------------­*MODEL CHANGE, INCLUDE NAIL4 ** *EL FILE, POSITION=CENTRODIAL s E *NODE FILE, GLOBAL=YES u ** *EL PRINT, ELSET:PNAIL4, POSITION=CENTRODIAL s E ** *NODE PRINT, NSET=H4 u ** *NODE PRINT, NSET=FACEl u ** *END STEP ** **---------------------- EXCAVATION LIFT #5 --------------------------------*STEP, AMPLITUDE=RAMP LOAD 7 Excavation of soil lift #5 and the installation of Nail#S *STATIC *DLOAD

~ **--------------- Remove Soil Slope for Lift #5 *MODEL CHANGE, REMOVE

---------------------------EXSS **----~------------ Add Shotcrete to Newly Cut Soil Face ----------------­*MODEL CHANGE, INCLUDE AP SSC **---------~------- Remove Soil in Nail Location -------------------------­*MODEL CHANGE, REMOVE SNELS **----------------- Install Soil Nail in Wall ----------------------------­*MODEL CHANGE, INCLUDE NAILS ** *EL FILE, POSITION=CENTRODIAL s E SINV EE ** *NODE FILE, GLOBAL=YES u ** *EL PRINT, ELSET=PNAILS, POSITION=CENTRODIAL s E ** *NODE PRINT, NSET=HS u ** *NODE PRINT, NSET=FACEl

Page 152: Two Dimensional Finite Element Modeling of Swift Delta

u ** *END STEP ** **---------------------- EXCAVATION LIFT #6 -------------------------------­*STEP, AMPLITUDE=RAMP LOAD 8 Excavation of soil lift #6 and the installation of Nail#6 *STATIC *DLOAD **--------------- Remove Soil Slope for Lift #6 --------------------------­*MODEL CHANGE, REMOVE EX6S **----------------- Add Shotcrete to Newly Cut Soil Face ----------------­*MODEL CHANGE, INCLUDE ~PGSC ** *EL FILE, POSITION=CENTRODIAL s E *NODE FILE, GLOBAL=YES u ** *EL PRINT,ELSET=PNAILS, POSITION=CENTRODIAL s E *NODE PRINT, NSET=H6 u ** *NODE PRINT, NSET=FACEl u ** *END STEP ** *STEP, AMPLITUDE=RAMP **-----~---------- Activate Shootcrete WEIGHT ------------------------­*GEOSTATIC *DLOAD SHOT,BY,-145.0 ** *EL FILE, POSITION=CENTRODIAL s E *NODE FILE, GLOBAL=YES

\ u ** *EL PRINT, ELSET=PNAILS, POSITION=CENTRODIAL s E ** *NODE PRINT, NSET=H6 u ** *NODE PRINT, NSET=FACEl u ** *FILE FORMAT, ASCII *END STEP

140

Page 153: Two Dimensional Finite Element Modeling of Swift Delta

::> XION3:ddV

i:vi:

Page 154: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.4-RES=1.1-P3/PATRAN R.1-(Tensor-YY)-ABAQUS-05-Mar-9415:10:12

SWIFT DELTA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 5 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. ~I-'

.i::.. N

Page 155: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES=1.1-P3/PA TRAN R.1 :-(T ensor-YY)-~BAQUS-05-Mar-94 15:28:51

SWIFT DEL TA FINITE ELEMENT MESH 0.

LIN1N MODEL STEP 6 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. - ........ ~ w

Page 156: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3. 7-RES=4.1-P3/PA TRAN R.1-0/ ector-Y)-ABAQUS-18-Mar-94 13:59:4 7

SWIFT DELTA FINITE ELEMENT MESH .05416

Deflection (Ft) LIN1 N MODEL STEP 8 .05012

.04608

.04203

.03799

.03395

.02991

.02587

.02182

.01778

.01374

.009699

.005657

.001615

-.002427 I I

I-'

-.006469 LJ t

Page 157: Two Dimensional Finite Element Modeling of Swift Delta

S~O~d NVCI~Vd ~VaNI~-NON

0 XIGN:a'.ddV

Sv1

Page 158: Two Dimensional Finite Element Modeling of Swift Delta

Vert Stress (psf)

0.

Fringe: LC=2.1-RES=1.1-P3/PATRAN R'.1-(T ensor-YY)-ABAQUS-31-Aug-94 09:42:57

SWIFT DEL TA-SOIL NAIL FEM RESULTS MODEL NOLIN1N GEOSTATIC STEP 2 -233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

nolin 1 n3.fil -3267.

-3500. _ .....

.i:::. (j'\

Page 159: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.3-RES=1.1-P3/PATRAN R..1-(T ensor-XX)-ABAQUS-31-Aug-94 10:22:40

SWIFT DEL TA SOIL NAIL FEM RESULTS

MODEL NOLIN1N STATIC STEP 4

no I in 1 n3.f ii

Horiz Stress (psf)

0.

-233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. .i::. ....J

Page 160: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.5-RES= 1.1-P3/P A TRAN R.1-(T ensor-XX)-ABAQUS-31-Aug-94 11 :23: 11

SWIFT DEL TA SOIL NAIL FEM RESULTS

MODEL NOLIN 1 N STATIC STEP 6

nolin 1 n3.fil

Horiz Stress (psf)

0.

-233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. ~ ~ 00

Page 161: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.2-RES=3.1-P3/PATRAN R.1-(T ensor-YY)-ABAQUS-13-May-94 16:58:23 Vert Strain

SWIFT DELTA SOIL NAIL WALL FEM RESULTS .001649

MODEL NOLIN1P STATIC STEP 3 .001304

.0009592

.0006144

.0002696

-.00007518

-.0004200

-.0007647

-.001110

-.001454

-.001799

-.002144

-.002489

-.002833

-.003178

nolin1 p3.fil -.003523 L--1 I-' ~ l.O

Page 162: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.2-RES=4.1-P31PATRAN R.1-0/ector-X)-A~AQUS-21-May-94 13:54:32 Horiz Disp

SWIFT DELTA SOIL NAIL WALL FEM RESULTS .008571

MODEL NOLIN1P STATIC STEP 4 .007918

.007265

.006612

.005959

.005306

.004653

.004000

.003347

.002694

.002041

.001388

.0007344

.00008136

-.0005717

nolin1 p3.fil -.001225 L_J I-' lJ1 0

Page 163: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=3.7-RES=2.1-P3/PATRAN R.1~(Major)-ABAQUS-17-Sep-9414:52:41

. SWIFT DELTA SOIL NAIL WALL FEM RESULTS

MODEL NOLIN1 P STATIC STEP 8

Major Strain

.007492

.006993

.006493

.005994

.005494

.004995

.004495

.003996

.003496

.002997

.002497

.001998

.001498

.0009990

.0004995

nolin1 p3.fil -.000000001000 -1--' U1 1--'

Page 164: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.1-RES= 1.1-P3/P A TRAN R.1-(T ensor-XX)-t\BAQUS-31-Aug-94 09:22:06

SWIFT DELTA SOIL NAIL FEM RESULTS

MODEL NOLIN1N GEOSTATIC STEP 2

nolin 1 n3.fil

Horiz Stress (psf)

0.

-233.3

-466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2567.

-2800.

-3033.

-3267.

-3500. I-' U1 N

Page 165: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.H-AES=1.1-P31PATAAN R.1-(Tensor-YY}-~AQUS-23-Juf-9416:41 :55 VERT STRESS

0.

SWIFT DELTA SOIL NAIL WALL FEM RESULTS -233.3

MODEL NOUN2N STATIC STEP 8 -466.7

-700.0

-933.3

-1167.

-1400.

-1633.

-1867.

-2100.

-2333.

-2B67.

-2800.

-3033.

-3267.

nolin2n 1.fil -3500. LJ .,

U1 w

Page 166: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.17-AES=1.1-P3/PATRAN R.1.-(Von-Mises)-ABAQUS-23-Juf-94 ·16:51:12 VON MISES

25785.

SWIFT DELTA SOIL NAIL WALL FEM RESULTS 24066.

MODEL NOUN2N STATIC STEP 8 22347.

20628.

18909_

17190.

15471.

13752.

12033.

·10314.

8595~

6876.

5157.

3438..

1719.

nolin2n 1. fil -.002197

- I-' lJl ~

Page 167: Two Dimensional Finite Element Modeling of Swift Delta

Fringe: LC=2.17-RES=2.1-P31PATRAN R.1-(Major)-,ABAQUS-23-Jul-9416:57:47

SWIFT DELTA SOIL NAIL WALL FEM .RESULTS _005174

.004830 MODEL NOUN2N STATIC STEP 8

.004485

.004140

.003795

.003450

.003105

.002760

.002415

.002070

.001725

.001380

.001035

.0006899

.0003450 nolin2n1 .fil

-.0000000000000 ....... lJ1 lJ1