[ths]2012 defl-01
TRANSCRIPT
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
Definition, Importance and Definition, Importance and Causes of DeflectionsCauses of Deflections
Derivation of Moment – Derivation of Moment – Curvature RelationCurvature Relation
The Double Integration The Double Integration MethodMethod
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3
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ DefinitionDefinitionDeflection is defined as the displacement of various points of the structure from their original positions including
linear deformations of points.
rotational deformations of lines (slopes) from their
original position.
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ Importance of DeflectionsImportance of Deflections
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Bad appearance and uncomforting of occupants
Cracking of plaster.
Drainage problems.
Damage of walls and non structural Elements.
■ ■ All Codes and Standards specify limits of deflection All Codes and Standards specify limits of deflection as excessive deflections lead to problems as:as excessive deflections lead to problems as:
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ Importance of DeflectionsImportance of Deflections
■ ■ In Addition the analysis of indeterminate In Addition the analysis of indeterminate structuresstructures requires the calculation of deflections as in advance requires the calculation of deflections as in advance stepstep
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ Sources of DeflectionsSources of Deflections
The external loads.
Temperature variation
Differential settlements between supports cause
various deformations.
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ Factors Affecting DeflectionsFactors Affecting Deflections
Span and Configuration
The Applied Loads
Material of the structure
Cross section of the Structure
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DEFLECTIONS of STRUCTURES
Tharwat Sakr
■ ■ Methods to calculate DeflectionsMethods to calculate Deflections
1. The Double Integration Method.1. The Double Integration Method.
5. The Real Work Method.5. The Real Work Method.
2. The Moment Area Method.2. The Moment Area Method.
3. The Elastic Load Method.3. The Elastic Load Method.
4. The Conjugate Beam Method.4. The Conjugate Beam Method.
6. The Virtual Work Method.6. The Virtual Work Method.
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1. Plane section before deformation remains plane after
deformations (Bernoulli's law )
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Main Assumptions
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2. Stress is Proportional to Strain (Elastic Material) (Hook’s Low)
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Main Assumptions
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3. The Depth – Span Ration is very small ( Slender Members)
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Main Assumptions
Slender BeamSlender Beam Deep BeamDeep Beam
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3. The Deflection is very – small compared to Span (Small deflection)
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Main Assumptions
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Curvature of elastic line Curvature of elastic line
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
d
R
R
1
2
ds
1 2
d 12
Y
X
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
To be in x, yTo be in x, y d R
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2
ds
1 2
d 12
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As As is so small is so small
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
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AsAs
ThenThen
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
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Lead toLead to
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
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For Very small values of For Very small values of deflection (y)deflection (y)
Is the equation of radius of curvature of any curve and Is the equation of radius of curvature of any curve and its simplification for very small values of yits simplification for very small values of y
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Curvature of Elastic Line (Property of Curves)
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Moment - Curvature Moment - Curvature RelationshipRelationship
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Moment-Curvature Relationship
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Moment-Curvature Relationship
MM
dh.
d
d
dh.
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1 1
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Moment-Curvature Relationship
Elongation at any fiberElongation at any fiber
Strain can be defined as Strain can be defined as
From Hook’s LawFrom Hook’s Law dh.
d
dh.
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1 1
1
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Moment-Curvature Relationship
From the stress formulaFrom the stress formula
By SubstitutionBy Substitution
FromFrom
Is the differential equation of the elastic line subjected Is the differential equation of the elastic line subjected to momentto moment
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Sign Convention
DeflectionDeflection
2
2
dxyd
dxdy
y
SlopeSlope
CurvatureCurvature
Is the rate of change of the displacementIs the rate of change of the displacement
Is the rate of change of the slopeIs the rate of change of the slope
Represents the displacement of the structureRepresents the displacement of the structure
Investigating the moment – deflection signInvestigating the moment – deflection sign
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THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Sign ConventionPositive MomentPositive Moment
Slope decreased with xSlope decreased with xNegative MomentNegative Moment
Slope Increased with xSlope Increased with x
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Is the Relation between Deflection and MomentIs the Relation between Deflection and Moment
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Sign Convention
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
Concepts
Deflection at any pointDeflection at any point
Slope angel at any pointSlope angel at any point
Curvature at any pointCurvature at any point
Moment at any pointMoment at any point
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The method is based on the direct application of the The method is based on the direct application of the differential equation of elastic linedifferential equation of elastic line
THE DOUBLE INTEGRATION METHOD
Theoretical Bases
THE DOUBLE INTEGRATION METHOD
Basic Procedure
Derive an Equation of the Moment M as function of Derive an Equation of the Moment M as function of position variable x position variable x (M(x))(M(x))
Apply the differential equation of elastic Apply the differential equation of elastic line and integrate twice line and integrate twice
Apply the Boundary and Continuity conditions to obtain the Apply the Boundary and Continuity conditions to obtain the integration constantsintegration constants
Substitute with the integration constants into the deflection Substitute with the integration constants into the deflection and slope equationsand slope equations
THE DOUBLE INTEGRATION METHOD
Boundary Conditions
At Roller supportAt Roller support
At Hinged supportAt Hinged support
At Fixed supportAt Fixed support
THE DOUBLE INTEGRATION METHOD
Continuity Conditions
At Any intermediate pointAt Any intermediate point
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Standard Cases of Beam Deflection
Tharwat Sakr
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Standard Cases of Beam Deflection
Tharwat Sakr