Chapter 8 Civil Engineering Part 2: Geotechnical Engineering

Slides:



Advertisements
Similar presentations
1 Soil mechanics Lateral earth pressure References: 1. Budhu, Muni, D. Soil Mechanics & Foundations. New York; John Wiley.
Advertisements

10. In-Situ Stress (Das, Chapter 9)
1 Soil mechanics Effective and total stresses References: 1. Budhu, Muni, D. Soil Mechanics & Foundations. New York; John.
Lecture (2). 1/39 2/39 3/39 4/39 5/39 6/39 7/39.
Foundation Engineering CE 483
Oil water Geometric Proof of Archimedes’ principal---From Pressure on a submerged surface Consider a submerged body in an oil-water layered system (shown.
CENTER OF GRAVITY, CENTER OF MASS AND CENTROID FOR A BODY
Fluid Mechanics Chapter 10.
Bearing Capacity Theory
EXTERNAL STABILITY The MSE wall system consists of three zones. They are: 1. The reinforced earth zone. 2. The backfill zone. 3. The foundation soil zone.
MECHANICS OF MATERIALS 7th Edition
Forces Due to Static Fluid
4. Phase Relations (Das, Chapter 3) Sections: All except 3.6
Session 15 – 16 SHEET PILE STRUCTURES
Lecture Notes Applied Hydrogeology
FLUID STATICS: Hydrostatic Force on Plane Surfaces slide 18.
Chapter 14 Fluids What is a Fluid? A fluid, in contrast to a solid, is a substance that can flow. Fluids conform to the boundaries of any container.
Physics Chapter 8 Fluid Mechanics
Lecture 14.2 Fluids II. HW #13 (Chapter 14) Read Sections 14-1 to 14.5 Problems: 14.4, 14.26, 14.35, 14.39, Due: Thursday May 8.
FLUID STATICS: Hydrostatic Force on Plane Surfaces slide 18.
9.6 Fluid Pressure According to Pascal’s law, a fluid at rest creates a pressure ρ at a point that is the same in all directions Magnitude of ρ measured.
GEO-MECHANICS (CE2204) Engineering Properties of Soils
Chapter 14 Fluids.
Chapter 2: Total Hydrostatic Force on Surfaces
Effective Stress Soil is a multi phase system
Fluid Statics.
Mecânica de Fluídos Ambiental 2015/2016
Soil Physics David Zumr room: b608 Lecture (and seminar) notes will be available: -
Civil Engineering Department College of Engineering Course: Soil and Rock Mechanics (CE 260) Lecturer: Dr. Frederick Owusu-Nimo.
Soil mechanics and foundation engineering-III (CE-434)
Direct Shear Test.
Course : CE 6405 – Soil Mechanic
Chapter Six Overview Applications of the Definite Integral in Geometry, Science, and Engineering.
Compaction Of Soil GANDHINAGAR INSTITUTE OF TECHNOLOGY Group Members
Chapter 15 (1) Slope Stability
FE: Geotechnical Engineering
CTC 450 Hydrostatics (water at rest).
Soil Mechanics-II STRESS DISTRIBUTION IN SOILS DUE TO SURFACE LOADS
11. In SITU STRESSES.
Chapter 1 Linear Equations and Linear Functions.
CE 3305 Engineering FLUID MECHANICS
For updated version, please click on
CHAPTER FOUR LATERAL EARTH PRESSURE. 3.1 Introduction 3.2 Definitions of Key Terms 3.2 Lateral Earth Pressure at Rest 3.3 Active and Passive Lateral Earth.
Shear in Straight Members Shear Formula Shear Stresses in Beams
FOUNDATION ENGINEERING
Consolidation Theories of Soils
Prediction of settlements of buildings, bridges, Embankments
GUIDED BY:- ANERI CHAvan.
5. WEIGHT VOLUME RELATIONSHIPS
Continuum Mechanics for Hillslopes: Part II
CHAPTER 4 SOIL STRESSES.
Soil Mechanics-II Soil Stabilization and Improvement
Chapter 8 Objectives Define a fluid. Distinguish a gas from a liquid.
GEOTECHNICAL ENGINEERING ECG 503 LECTURE NOTE 10 TOPIC : 3
Chapter 7: Solid and Fluids
Soil mechanics INTRODUCTION ABOUT THE SUBJECT? WHY WE ARE STUDY THIS SUBJECT? HISTORY OF THE SUBJECT?
CE 230-Engineering Fluid Mechanics
Groundwater Learning objectives
Problem-1 A two member frame is supported by the two pin supports at A and D as shown. The beam AB is subjected to a load of 4 kN at its free end. Draw.
ENGINEERING MECHANICS
γdry=110 Find: VTotal[ft3] of borrowed soil Fill VT=10,000 [ft3]
CENTER OF GRAVITY, CENTER OF MASS AND CENTROID FOR A BODY
Statics Course Code: CIVL211 FRICTION Dr. Aeid A. Abdulrazeg.
Po Shan Road, Hong Kong, 18 June 1972
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg
Structure I Course Code: ARCH 208 Dr. Aeid A. Abdulrazeg.
Asst. Prof. Dr. Hayder Mohammad Jaffal
3 Chapter Chapter 2 Graphing.
Civil Engineering Dept.
CENTER OF GRAVITY, CENTER OF MASS AND CENTROID FOR A BODY
Presentation transcript:

Chapter 8 Civil Engineering Part 2: Geotechnical Engineering 4th Edition Chapter 8 Civil Engineering Part 2: Geotechnical Engineering

Part 2: Geotechnical Engineering The stability of a structure is no better than its foundations. Ask the people who built this  Exploring Engineering

Trouble in the Basement … Exploring Engineering

Properties of Soils Exploring Engineering

sat = (Ws + Wp)/V = dry + n w Wet Soil The mechanical properties of soils depend how much the soil’s pores are water filled sat = (Ws + Wp)/V = dry + n w where Ws and Wp are the weight of dry soil and the weight of water in the pores. The corresponding weight densities are dry and w. V is the volume of the soil. The term, n, is the volume fraction of the pores in the soil. Exploring Engineering

Dry Weight Densities of Different Soils Wet Soils Dry Weight Densities of Different Soils Soil Type Dry Density (lbf/ft3) Porosity Wet density Lbf/ft3 Sand 94.8 0.375 118 Clay 74.9 0.550 109 Silt 79.9 0.425 106 Water 62.4 — Exploring Engineering

Effective Stress Principle Pressure Is What You Feel when Your Fingers Press with Force Fn on the Contact Patch of Area A Exploring Engineering

Effective Stress Principle Soil section in next slide being analyzed for stress on the horizontal plane (dashed line) at depth z. This force is actually distributed uniformly over the bottom face creating a constant pressure (or stress).

Effective Stress Principle ’ =  - pp = (sat - w)z is the stress at depth z FBD Effective stress on layer of wet soil Exploring Engineering

Example Two top layers of a soil sample taken from a potential building site are shown in the next figure. If the thicknesses of the layers are HA = 2.50 ft and HB = 2.00 ft, determine: (a) the effective stress at a depth of ZA = 2.00 ft in Layer A (b) The effective stress at a depth of ZB = 3.00 ft in Layer B. Assume both layers are fully saturated with weight densities of γA = 78.6 lbf/ft3 and γB = 91.2 lbf/ft3. The weight density of water is γw = 62.4 lbf/ft3.  Exploring Engineering

Example Continued Need: Find the values of effective stress at depths of 2.00 ft and 3.00 ft. Know: The depths of interest are ZA = 2.00 ft and ZB = 3.00 ft; the layer thicknesses are HA = 2.50 ft and HB = 2.00 ft; the weight densities of saturated soil and water are γA = 78.6 lbf/ft3, γB = 91.2 lbf/ft3, and γw = 62.4 lbf/ft3; both soil layers are fully saturated. Exploring Engineering

Example Continued Exploring Engineering

Example continued How: Since all of the soils above z = ZA are of a uniform compositions and fully saturated, use effective stress principle. With two layers of soil above z = ZB generalize the effective stress equation for the weights z = ZB in the free-body diagram. (1) draw the free-body diagram of the soil section, (2) find Fn from the summation of forces in the vertical direction, (3) substitute Fn into the definition of pressure to get total stress, (4) subtract pore pressure from total stress to get effective stress. Exploring Engineering

Example continued Solve: a) ’ =  - pp = (sat - w)z = (78.6 – 62.4)(2.00) [lbf/ft3] [ft] = 32.4 lbf/ft2 Generalize the equation for the effective stress ’ = AHA + BHB - wz = (78.6)(2.50) + (91.2)(3.00 - 2.50) – (62.4)(3.00) [lbf/ft2] = 54.9 lbf/ft2

Summary of Part 2 Geotechnical Engineering Structures stand on soil whose properties are variable, particularly if wet Starting with a FBD, stress in wet soil can be estimated from the weight of dry soil and wet soil at any layer The effective stress equation allows the calculation of stress at any layer of wet soil knowing its porosity Exploring Engineering