Foundation Analysis LATERAL EARTH PRESSURE

Similar documents
Chapter 12: Lateral Earth Pressure

LATERAL EARTH PRESSURE AND RETAINING STRUCTURES

Chapter (7) Lateral Earth Pressure

UNIT V. The active earth pressure occurs when the wall moves away from the earth and reduces pressure.

LATERAL EARTH PRESSURE

GEOTECHNICAL ENGINEERING ECG 503 LECTURE NOTE ANALYSIS AND DESIGN OF RETAINING STRUCTURES

Lateral Earth Pressure

file:///d /suhasini/suha/office/html2pdf/ _editable/slides/module%202/lecture%206/6.1/1.html[3/9/2012 4:09:25 PM]

FOUNDATION ENGINEERING UNIT V

Objectives. In this section you will learn the following. Rankine s theory. Coulomb s theory. Method of horizontal slices given by Wang (2000)

Soil Mechanics Prof. B.V.S. Viswanathan Department of Civil Engineering Indian Institute of Technology, Bombay Lecture 51 Earth Pressure Theories II

EARTH PRESSURES ON RETAINING STRUCTURES

Earth Pressure Theory

Compute the lateral force per linear foot with sloping backfill and inclined wall. Use Equation No. 51, page 93. Press ENTER.

8.1. What is meant by the shear strength of soils? Solution 8.1 Shear strength of a soil is its internal resistance to shearing stresses.

Module 6 (Lecture 23) LATERAL EARTH PRESSURE

Active Earth Pressure on Retaining Wall Rotating About Top

Geotechnical Parameters for Retaining Wall Design

D1. A normally consolidated clay has the following void ratio e versus effective stress σ relationship obtained in an oedometer test.

Seismic Analysis of Retaining Structures. Nanjundaswamy P. Department of Civil Engineering S J College of Engineering, Mysore

Chapter 5 Shear Strength of Soil

Ch 4a Stress, Strain and Shearing

CE 4780 Hurricane Engineering II. Section on Flooding Protection: Earth Retaining Structures and Slope Stability. Table of Content

SHEAR STRENGTH OF SOIL

1.5 STRESS-PATH METHOD OF SETTLEMENT CALCULATION 1.5 STRESS-PATH METHOD OF SETTLEMENT CALCULATION

Reinforced Soil Structures Reinforced Soil Walls. Prof K. Rajagopal Department of Civil Engineering IIT Madras, Chennai

Theory of Shear Strength

Introduction to Soil Mechanics

DETERMINATION OF UPPER BOUND LIMIT ANALYSIS OF THE COEFFICIENT OF LATERAL PASSIVE EARTH PRESSURE IN THE CONDITION OF LINEAR MC CRITERIA

2017 Soil Mechanics II and Exercises Final Exam. 2017/7/26 (Wed) 10:00-12:00 Kyotsu 4 Lecture room

9/23/ S. Kenny, Ph.D., P.Eng. Lecture Goals. Reading List. Students will be able to: Lecture 09 Soil Retaining Structures

both an analytical approach and the pole method, determine: (a) the direction of the

Project: Cantilever Steel SheetPile Retaining Wall Analysis & Design, Free Earth Support In accordance Eurocode 7.

Theory of Shear Strength

Following are the results of four drained direct shear tests on an overconsolidated clay: Diameter of specimen 50 mm Height of specimen 25 mm

Module 6 (Lecture 22) LATERAL EARTH PRESSURE

SHEAR STRENGTH I YULVI ZAIKA

SHEET PILE WALLS. Mehdi Mokhberi Islamic Azad University

EAS 664/4 Principle Structural Design

Soil strength. the strength depends on the applied stress. water pressures are required

(Refer Slide Time: 01:15)

The theories to estimate lateral earth pressure due to a strip surcharge loading will

Active Thrust on an Inclined Wall under the Combined Effect of Surcharge and Self- Weight

Active static and seismic earth pressure for c φ soils

PRINCIPLES OF GEOTECHNICAL ENGINEERING

Objectives. In this section you will learn the following. Development of Bearing Capacity Theory. Terzaghi's Bearing Capacity Theory

Module 7 (Lecture 25) RETAINING WALLS

Laboratory Testing Total & Effective Stress Analysis

SHEAR STRENGTH OF SOIL. Chapter 10: Sections Chapter 12: All sections except

Page 1 of 10. PROFESSIONAL ENGINEERS ONTARIO NATIONAL EXAMINATIONS Mav CIV-A4 GEOTECHNICAL MATERIALS AND ANALYSIS 3 HOURS DURATION

Estimation of the Passive Earth Pressure with Inclined Cohesive Backfills: the Effect of Intermediate Principal Stress is Considered

Jaky s formula was often used to calculate the earth pressure at-rest behind a

In depth study of lateral earth pressure

Active Force on Retaining Wall Supporting Φ Backfill Considering Curvilinear Rupture Surface

Mohr s Circle of Stress

Tectonics. Lecture 12 Earthquake Faulting GNH7/GG09/GEOL4002 EARTHQUAKE SEISMOLOGY AND EARTHQUAKE HAZARD

SHEAR STRENGTH OF SOIL

pcf REQUIRED: Determine the shear strength parameters for use in a preliminary shallow foundation design. SOLUTION:

Landslide FE Stability Analysis

Reciprocal of the initial shear stiffness of the interface K si under initial loading; reciprocal of the initial tangent modulus E i of the soil

Shear Strength of Soils

Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay

7. STRESS ANALYSIS AND STRESS PATHS

Passive Force on Retaining Wall Supporting Φ Backfill Considering Curvilinear Rupture Surface

Chapter (11) Pile Foundations

Chapter (3) Ultimate Bearing Capacity of Shallow Foundations

CE 221: MECHANICS OF SOLIDS I CHAPTER 1: STRESS. Dr. Krisada Chaiyasarn Department of Civil Engineering, Faculty of Engineering Thammasat university

1.8 Unconfined Compression Test

BACKFILL AND INTERFACE CHARACTERISTICS

Study of Seismic Behaviour of Retaining Walls

DESIGN AND DETAILING OF COUNTERFORT RETAINING WALL

SOIL SHEAR STRENGTH. Prepared by: Dr. Hetty Muhammad Azril Fauziah Kassim Norafida

Prof. B V S Viswanadham, Department of Civil Engineering, IIT Bombay

SOIL MECHANICS Assignment #7: Shear Strength Solution.

Advanced model for soft soils. Modified Cam-Clay (MCC)

DESIGN AND ANALYSIS OF RETAINING WALLS

vulcanhammer.net This document downloaded from

GG 454 March 19, EFFECTIVE STRESS AND MOHR-COULOMB FAILURE (26)

Brittle Deformation. Earth Structure (2 nd Edition), 2004 W.W. Norton & Co, New York Slide show by Ben van der Pluijm

Chapter (12) Instructor : Dr. Jehad Hamad

NUMERICAL ANALYSIS OF PASSIVE EARTH PRESSURES WITH INTERFACES

Interslice force functions for computing active and passive earth force

However, the friction forces are limited in magnitude and will not prevent motion if sufficiently large forces are applied.

D : SOLID MECHANICS. Q. 1 Q. 9 carry one mark each.

MECHANICS OF MATERIALS. Prepared by Engr. John Paul Timola

YOUR HW MUST BE STAPLED YOU MUST USE A PENCIL (no pens)

J. Paul Guyer, P.E., R.A.

BOOK OF COURSE WORKS ON STRENGTH OF MATERIALS FOR THE 2 ND YEAR STUDENTS OF THE UACEG

Slope Stability. loader

(Refer Slide Time: 02:18)

D DAVID PUBLISHING. Port and Marine Structures Made of Sheet Piling with Staggered Toe. 1. Introduction. 2. Design Approach and Main Dependencies


Foundation Engineering Prof. Dr. N. K. Samadhiya Department of Civil Engineering Indian Institute of Technology Roorkee

Entrance exam Master Course

SN QUESTION YEAR MARK 1. State and prove the relationship between shearing stress and rate of change of bending moment at a section in a loaded beam.

Class Principles of Foundation Engineering CEE430/530

Chapter 4. Ultimate Bearing Capacity of Shallow Foundations. Omitted parts: Sections 4.7, 4.8, 4.13 Examples 4.8, 4.9, 4.

Equilibrium of Deformable Body

SOIL MODELS: SAFETY FACTORS AND SETTLEMENTS

INTI COLLEGE MALAYSIA

Transcription:

Foundation Analysis LATERAL EARTH PRESSURE

INTRODUCTION Vertical or near-vertical slopes of soil are supported by retaining walls, cantilever sheet-pile walls, sheet-pile bulkheads, braced cuts, and other similar structures. The proper design of these structures requires an estimation of lateral earth pressure, which is a function of several factors, such as a) the type and amount of wall movement, b) the shear strength parameters of the soil, c) the unit weight of the soil, and d) the drainage conditions in the backfill.

INTRODUCTION Lateral earth pressure is a function of wall movement (or relative lateral movement in the backfill soil).

LATERAL EARTH PRESSURE AT REST (No Lateral Movement) Consider a vertical wall of height H, as shown in Figure 7.3, retaining a soil having a unit weight of γ. A uniformly distributed load, q/unit area, is also applied at the ground surface.

LATERAL EARTH PRESSURE AT REST The shear strength of the soil is, (No Lateral Movement) τ = c + σ tan where, c is the cohesion σ is the effective normal stress ϕ is the effective angle of friction At any depth z below the ground surface, the vertical subsurface stress and lateral earth pressure are expressed as, σ 0 = q + γz σ h = K 0 σ 0 + u where, u is the pore water pressure K 0 is the coefficient of at-rest earth pressure

LATERAL EARTH PRESSURE AT REST (No Lateral Movement) For normally consolidated soil (Jaky, 1944) K 0 = 1 sin For overconsolidated soil (Mayne and Kulhawy, 1982) K 0 = (1 sin )OCR sin The total force, P 0, per unit length of the wall can now be obtained from the area of the pressure diagram as, P 0 = P 1 + P 2 = qk 0 H + 1 2 γh2 K 0 The location of the line of action of the resultant force, P 0, can be obtained by taking the moment about the bottom of the wall. Thus, z = P H 1 2 + P H 2 3 Note: If the surcharge q = 0 and the pore water pressure u = 0, the pressure diagram will be a triangle. P 0

LATERAL EARTH PRESSURE AT REST (No Lateral Movement) If the water table is located at a depth z < H, the at-rest pressure diagram will have to be somewhat modified.

PROBLEM SET 10 1. For the retaining wall shown in the figure below, determine the lateral earth force at rest per unit length of the wall. Also determine the location of the resultant force. Assume OCR = 1.

LATERAL EARTH PRESSURE ACTIVE AND PASSIVE Based on assumptions of the intervening forces and the failure mode, different theories have been developed. These theories differ only in terms of the coefficient of lateral earth pressure but operate with similar stress/pressure equations. The three widely-accepted theories are the following: 1. Rankine s 2. Coulomb s 3. Log-spiral

LATERAL EARTH PRESSURE ACTIVE AND PASSIVE Below are the comparison of the three theories and their applicability. Method Failure Mode Wall Friction Active Case Passive Case based on experimentation and actual failure observations Rankine planar no wall friction poor estimate poor estimate Coulomb planar considered good estimate (less) poor estimate Log-spiral curved considered better estimate better estimate

RANKINE S THEORY A Unit weight of soil = γ c' ' tan ' f σ' v σ' h z Assumptions: Vertical frictionless wall Dry homogeneous soil Horizontal backfill B

ACTIVE EARTH PRESSURE A Unit weight of soil = γ c' ' tan ' f σ' v σ' h z If wall AB is allowed to move away from the soil mass gradually, horizontal stress will decrease. Plastic equilibrium in soil refers to the condition where every point in a soil mass is on the verge of failure. B This is represented by Mohr s circle in the subsequent slide.

ACTIVE EARTH PRESSURE c' ' tan ' f ø' Based on the diagram: c' σ'a Koσ o σ o K a ' a ' ' ' ' a 2 0 tan ' 1- sin ' (45 - ) 2 1 sin ' 0 0 tan K a 2 ' ' (45 - ) - 2c' tan (45 - ) 2 2-2c' K a K a is the Rankine active earth pressure coefficient

ACTIVE EARTH PRESSURE

ACTIVE EARTH PRESSURE DISTRIBUTION - 2c' K a - 2c' K a z c 2c' K a z ' 0 K a ' 0 Ka - 2c' Ka

PASSIVE EARTH PRESSURE A B Unit weight of soil = γ c' ' tan ' f σ' v σ' h z If the wall is pushed into the soil mass, the principal stress σ h will increase. On the verge of failure the stress condition on the soil element can be expressed by Mohr s circle b. The lateral earth pressure, σ p, which is the major principal stress, is called Rankine s passive earth pressure.

Shear stress PASSIVE EARTH PRESSURE c' ' tan ' f D b A ' c' O K o σ o a σ o C σ' p Normal stress ' ' p ' p 2 K p tan 0 ' ' 0 0 K tan p 2 ' ' (45 ) 2c' tan (45 ) 2 2 2c' ' 1 sin ' (45 ) 2 1 sin ' K p D K p is the Rankine passive earth pressure coefficient

PASSIVE EARTH PRESSURE

PASSIVE EARTH PRESSURE DISTRIBUTION z For cohesionless soil, p v K p z K p 2c' K p z K p

SPECIAL CASES Submergence: Inclined backfill: Inclined but smooth back face of wall:

SPECIAL CASES Inclined backfill with c -ϕ soil:

ILLUSTRATIVE PROBLEM A frictionless retaining wall is shown in Figure 12.22a. Determine: a) The active force Pa after the tensile crack occurs. b) The passive force Pp. A q = 10 kn/m 2 γ = 15 kn/m 3 ø = 26 o c = 8 kn/m 2 z H = 4 m B Figure 12.22a Frictionless retaining wall AB

SOLUTION a) The active force Pa after the tensile crack occurs. At z = 0 m; At z = 4 m; K a = 1 sinø 1 + sinø σ a = K a σ v 2c σ v = γ z σ v = q = 10 kn/m 2 = 1 si n( 26) 1 + si n( 26) K a = 0. 39 σ a = 0.39(10) 2(8)( 0.39) = 6. 09 kn/m 2 σ v = 10 + 15(4) = 60 kn/m 2 σ a = 0.39(60) 2(8)( 0.39) = 17. 31 kn/m 2

SOLUTION A q = 10 kn/m 2-6.09 kn/m 2 γ = 15 kn/m 3 ø = 26 o y = 1.04 m c = 8 kn/m 2 H = 4 m 4 y = 2.96 m B (a) (b) 17.32 kn/m 2 Figure 12.22 (a) Frictionless retaining wall AB, and (b) active pressure distribution diagram

SOLUTION From Figure 12.22b, -6.09 kn/m 2 6.09 y = 17.31 ; y = 1. 04 m, 4 y = 2. 96 m 4 y The active force Pa after the tensile crack occurs is equal to the area of the active pressure distribution diagram below point C, or P a = 1 2 17.31 2.96 = 25. 62 kn/m 4 y = 2.96 m C y = 1.04 m P a and the location is located at z=0.99 m z = 1 3 2.96 = 0. 99 m 17.32 kn/m 2 (b)

b) The passive force Pp. K p = 1 + sinø 1 sinø SOLUTION = 1 + si n( 26) 1 si n( 26) = 2. 56 σ p = K p σ v + 2c σ v = γ z K p At z = 0 m; σ v = q = 10 kn/m 2 σ p = 2.56(10) + 2(8)( 2.56) = 51. 2 kn/m 2 At z = 4 m; σ v = 10 + 15(4) = 60 kn/m 2 σ p = 2.56(60) + 2(8)( 2.56) = 204. 8 kn/m 2

SOLUTION A q = 10 kn/m 2 51.2 kn/m 2 γ = 15 kn/m 3 ø = 26 o c = 8 kn/m 2 H = 4 m B (a) 51.2 kn/m 2 153.6 kn/m 2 (c) Figure 12.22 (a) Frictionless retaining wall AB, and (c) passive pressure distribution diagram

From Figure 12.22c, SOLUTION The passive force Pp is equal to the area of the passive pressure distribution, or 51.2 kn/m 2 P p = 51.2 4 + 1 2 153.6 4 = 512 kn/m and the location is calculated by taking summation moment at the base, or z=1.6 m P p 512 z = 51.2 4 4 2 + 1 2 153.6 (4) 1 3 (4) z = 1. 6 m 51.2 kn/m 2 153.6 kn/m 2 (c)

FINAL ANSWERS a) The active force Pa after the tensile crack occurs has a magnitude of 25.62 kn per unit length of the frictionless retaining wall and is acting at 0.99 meters above the base. b) The passive force Pp has a magnitude of 512 kn per unit length of the frictionless retaining wall and is acting at 1.6 meters above the base.

PROBLEM SET 10 2. Assume that the retaining wall shown in the figure below can yield sufficiently to develop an active state. Determine the Rankine active force per unit length of the wall and the location of the resultant line of action.

PROBLEM SET 10 3. Assume that the retaining wall shown in the figure below can yield sufficiently to develop passive state. Determine the Rankine passive force per unit length of the wall.

COULOMB S LATERAL EARTH PRESSURE ACTIVE EARTH PRESSURE

COULOMB S LATERAL EARTH PRESSURE PASSIVE EARTH PRESSURE

COULOMB S LATERAL EARTH PRESSURE where, β is the angle the back face is inclined with the horizontal α is the inclination of backfill with the horizontal δ is the wall friction angle ϕ is the angle of internal friction

PROBLEM SET 10 4. A retaining wall shown below has a height of 4.5 m. The unit weight of soil is 16.5 kn/m 3. The angle of internal friction of soil is 36, the wall friction angle is 24, and soil cohesion is 0. The wall is supporting a horizontal backfill. 4.1 Compute the Coulomb s active earth pressure coefficient. 4.2 Compute the Coulomb s active force per unit length of wall. 4.3 Compute the location of the Coulomb s active force from the bottom of the wall.

PROBLEM SET 10 5. A vertical retaining wall has a height of 4 m and is supporting a horizontal backfill. The unit weight of soil is 16.5 kn/m 3. The angle of internal friction of soil is 35, the wall friction angle is 20, and soil cohesion is 0. 5.1 Compute the Coulomb s passive earth pressure coefficient. 5.2 Compute the Coulomb s passive force per unit length of wall perpendicular to the wall. 5.3 Compute the location of the Coulomb s passive force from the bottom of the wall.