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06/19/22 DEFLECTIONS of STRUCTURES Tharwat Sakr Definition, Definition, Importance and Importance and Causes of Causes of Deflections Deflections Derivation of Derivation of Moment – Curvature Moment – Curvature Relation Relation The Double The Double Integration Method Integration Method 1 3 2

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Page 1: [Ths]2012 defl-01

05/03/23

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

1

3

2

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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

3

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)

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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

1

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.

1

1 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.

1

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

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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

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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

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THE DOUBLE INTEGRATION METHOD

Boundary Conditions

At Roller supportAt Roller support

At Hinged supportAt Hinged support

At Fixed supportAt Fixed support

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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