Structural Equivalency Lecture 10. Subbase Thickness, inches LTE=10% DC-10 Gear k=100 Subbase E=1x10 6 psi h- Varies LTE=10% 0510152025 25 20 15 10 5.

Slides:



Advertisements
Similar presentations
Sample Problem 4.2 SOLUTION:
Advertisements

Definition I. Beams 1. Definition
FAA Airport Pavement Working Group Meeting, April Concrete Overlay Research Shelley Stoffels, D.E., P.E. Lin Yeh, PhD FAA Airport Pavement Working.
Composites Design and Analysis Stress-Strain Relationship Prof Zaffar M. Khan Institute of Space Technology Islamabad.
HW/Tutorial Week #10 WWWR Chapters 27, ID Chapter 14 Tutorial #10 WWWR # 27.6 & To be discussed on March 31, By either volunteer or class list.
Lecture 33 - Design of Two-Way Floor Slab System
Chapter 9 Extension, Torsion and Flexure of Elastic Cylinders
Pavement Design Session Matakuliah: S0753 – Teknik Jalan Raya Tahun: 2009.
Sample Problem 4.2 SOLUTION:
4 Pure Bending.
PH0101 UNIT 1 LECTURE 31 Bending of Beams Bending moment of a Beam Uniform Bending (Theory and Experiment) Worked Problem.
CUFSM Advanced Functions
ENGR-1100 Introduction to Engineering Analysis
Gordon F. Hayhoe FAA AAR-410
CHAPTER 7 TRANSVERSE SHEAR.
Lecture 5 FUNDAMENTALS Fundamentals of sandwich structure will be derived such as stress- strain, flexural rigidity, bending, torsion etc. Virtually the.
Joint Types and Behavior. Rigid Pavement Design Course Jointing Patterns.
Approaches to Design.
4 Pure Bending.
Subgrade Characterization For Concrete Pavement Design
Final Project1 3/19/2010 Isogrid Buckling With Varying Boundary Conditions Jeffrey Lavin RPI Masters Project.
R/W Rehabilitation. Pavement Condition North 3000 feet North 8000 feet.
THEORIES OF FAILURE THEORIES OF FAILURE FOR DUCTILE MATERIALS
Beams: Pure Bending ( ) MAE 314 – Solid Mechanics Yun Jing Beams: Pure Bending.
PCC Overlays of HMA Pavements
FWD BackCalculation of Existing Pavement Structure.
Subgrade Models for Rigid Pavements. Development of theories for analyzing rigid pavements include the choice of a subgrade model. When the chosen model.
Load Equivalency. Plate theory: solutions limited to a single tire print Prickett & Ray (1951) – provided a graphical extension of Westergaard theory.
Load Characterization. Rigid Pavement Design Course Traffic Load Considerations Load Groups Lane Wander Load Configuration.
Sample Problem 4.2 SOLUTION:
CHAPTER #3 SHEAR FORCE & BENDING MOMENT
MECHANICS OF MATERIALS
Distributed Forces: Moments of Inertia
External Flow: The Flat Plate in Parallel Flow
COLUMNS. COLUMNS Introduction According to ACI Code 2.1, a structural element with a ratio of height-to least lateral dimension exceeding three used.
BENDING MOMENTS AND SHEARING FORCES IN BEAMS
Perpetual Pavement Design Perpetual Pavement Open House Ashton, Iowa October 5, 2005.
CUFSM Advanced Functions
Extending Asphalt Pavement Life Using Thin Whitetopping Mustaque Hossain, Ph.D., P.E. Department of Civil Engineering Kansas State University.
Moment Area Theorems: Theorem 1:
Mechanics of Thin Structure Lecture 15 Wrapping Up the Course Shunji Kanie.
 2005 Pearson Education South Asia Pte Ltd 7. Transverse Shear 1 CHAPTER OBJECTIVES Develop a method for finding the shear stress in a beam having a prismatic.
3. Stresses in Machine Elements Lecture Number – 3.1 Prof. Dr. C. S. Pathak Department of Mechanical Engineering Sinhgad College of Engineering, Pune Strength.
Perpetual Pavement Design John D’Angelo Federal Highway Administration Washington, DC Canadian User Producer Group for Asphalt Saskatoon, Saskatchewan.
Buckling of Slender Columns ( )
IIT-Madras, Momentum Transfer: July 2005-Dec 2005 Perturbation: Background n Algebraic n Differential Equations.
Mechanics of Materials – MAE 243 (Section 002) Spring 2008 Dr. Konstantinos A. Sierros.
Chapter 4 Pure Bending Ch 2 – Axial Loading Ch 3 – Torsion
Structural Design for Cold Region Engineering Lecture 14 Thory of Plates Shunji Kanie.
ME 612 Metal Forming and Theory of Plasticity
Mechanical Properties of Materials
Theoretical Mechanics STATICS KINEMATICS
Unit-5. Torsion in Shafts and Buckling of Axially Loaded Columns Lecture Number-3 Mr. M.A.Mohite Mechanical Engineering S.I.T., Lonavala.
Chapter 4 Pure Bending Ch 2 – Axial Loading Ch 3 – Torsion Ch 4 – Bending -- for the designing of beams and girders.
Structure Analysis I. Lecture 7 Internal Loading Developed in Structural Members Ch.4 in text book.
2010 FAA Airport Technology Transfer Conference Some Key Findings from NAPTF Testing of Unbonded PCC Overlays IPRF Project 04-02: Improved Overlay Design.
External Flow: The Flat Plate in Parallel Flow
☻ ☻ ☻ ☻ 2.0 Bending of Beams sx 2.1 Revision – Bending Moments
1 - An AISI 1020 cold- rolled steel tube has an OD of 3.0 inch. The internal pressure in the tube is 6,840 psi. Determine the thickness of the tube using.
Lecture 1 Stress 16 July 2007 ENT 450 Mechanics of Materials Dr. Haftirman 1 ENT 450 MECHANICS OF MATERIALS (MoM) RC. Hibbler Lecture: DR. HAFTIRMAN Teaching.
DARWIN AC/AC Overlay Design. Course Materials Tables and Design Procedures for this manual.
Principal Stresses and Strain and Theories of Failure
BACKCALCULATION OF AIRFIELD PAVEMENT STRUCTURES BASED ON WAVE PROPAGATION THEORY Kunihito MATSUI (Tokyo Denki University) Yoshiaki OZAWA (Century-techno.
DEPARTMENT OF MECHANICAL AND MANUFACTURING ENGINEERING
Sample Problem 4.2 SOLUTION:
Shear in Straight Members Shear Formula Shear Stresses in Beams
Pure Bending.
Sample Problem 4.2 SOLUTION:
Chapter 6 Bending.
Pavement Structural Analysis
Presentation transcript:

Structural Equivalency Lecture 10

Subbase Thickness, inches LTE=10% DC-10 Gear k=100 Subbase E=1x10 6 psi h- Varies LTE=10% ” 21” 24” Subgrade Stress, psi

Conventional Plate Theory o Single Placed Layer 1) Regard the base as contributing exclusively to the stiffness of the subgrade  k composite o Based of PCA tests (1950’s) o Volumetric approach o Backcalculation- matching Defl. Basin Basin Area

h1E1h1E1 h2E2h2E2 11 k heEeheEe ee k

Slab Action:  - Value

Equivalent Thickness h e-p  Equivalent Thickness  m  Measured Value k b  Back-calculated E c  Based on Cores

Unbonded Layers No separation during bending

Bonded System

unbonded or bonded Tandem Dual Tridem Tied or Extended Shoulder DoDo W L slab  = 0 or f

Bending Moment

Bending Moment - with Subbase

Bending Stress - with Subbase

Partially Bonded System cc ee  e-p hchc h e-p Transformed Section

Summary

Westergaard Special Theory

Basis of b and a correction factors Ordinary Theory: plane sections remain plane Special Theory: where vertical distortion is accounted for. Stress under a point loads tends to infinity (a & b were provided as correction factors)

for interior load:

Equation for b - b is a fictitious radius in the stress equation which yields the same tensile stress as the solutions by Nadai Point Loada=1/4 h b=0.3254hb=0.3709h b=0.705hb=0.504h b=1.456h b=0.944h b=1.967h a=h/2 a=3h/4 a=h a=1.5h a=2h

Nadai examined the area close to the load a small portion of the slab impressed with a uniform pressure and subgrade reaction pressure Boundary conditions used by Nadai not clear. - Used simple support reaction Westergaard selected n=5 For n  5, the subgrade reaction is small in comparison to the load on the surface and can be neglected. c uniform press. Vicinity close to loaded area Nadai Subgrade reaction (empirical soln.)

Westergaard Recommended In plotting against the following expression for b resulted where a=1.724h is where a=b; but a=0.5h may be just as appropriate. a=1.724h appears to be arbitrary.

h (c=b) c/h Hyperbola Analytical results Figure 6-2. Relation among true radius b, slab thickness h (16).