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10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr Definition, Importance and Causes of Deflections Derivation of Moment – Curvature Relation The Double Integration Method 1 3 2
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Definition Deflection is defined as the displacement of various points of the structure from their original positions including  ,[object Object],[object Object]
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Importance of Deflections ,[object Object],[object Object],[object Object],[object Object],■  All Codes and Standards specify limits of deflection  as excessive deflections lead to problems as:
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Importance of Deflections ■  In Addition the analysis of indeterminate structures requires the calculation of deflections as in advance  step
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Sources of Deflections ,[object Object],[object Object],[object Object]
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Factors Affecting Deflections ,[object Object],[object Object],[object Object],[object Object]
10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■  Methods to calculate Deflections 1.  The Double Integration Method. 5.  The Real Work Method. 2.  The Moment Area Method. 3.  The Elastic Load Method. 4.  The Conjugate Beam Method. 6.  The  Virtual Work Method.
10/15/11 ,[object Object],THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions
10/15/11 ,[object Object],THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions
10/15/11 3. The Depth – Span Ration is very small ( Slender Members) THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions Slender Beam Deep Beam
10/15/11 3. The Deflection is very – small compared to Span  (Small deflection) THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions
10/15/11 THE DIFFERENTIAL EQUATION OF  THE ELASTIC LINE
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves) Curvature of elastic line
THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves) To be in x, y
10/15/11 As    is so small THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
10/15/11 As Then THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
10/15/11 Lead to THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
10/15/11 For Very small values of deflection (y) Is the equation of radius of curvature of any curve and its simplification for very small values of y THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship Moment - Curvature  Relationship
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship Elongation at any fiber Strain can be defined as  From Hook’s Law
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship From the stress formula By Substitution From Is the differential equation of the elastic line subjected to moment
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Sign Convention Deflection Slope Curvature Is the rate of change of the displacement Is the rate of change of the slope Represents the displacement of the structure Investigating the moment – deflection sign
10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Sign Convention Positive Moment Slope decreased with x Negative Moment Slope Increased with x
10/15/11 Is 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 point Slope angel at any point Curvature at any point Moment at any point
10/15/11 THE DOUBLE INTEGRATION METHOD
10/15/11 The method is based on the direct application of the differential 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 position variable x  (M(x)) Apply the differential equation of elastic line and integrate twice  Apply the Boundary and Continuity conditions to obtain the integration constants Substitute with the integration constants into the deflection and slope equations
THE DOUBLE INTEGRATION METHOD Boundary Conditions At Roller support At Hinged support At Fixed support
THE DOUBLE INTEGRATION METHOD Continuity  Conditions At Any intermediate point
10/15/11 Standard Cases of Beam Deflection Tharwat Sakr
10/15/11 Standard Cases of Beam Deflection Tharwat Sakr

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[Ths]2012 defl-01

  • 1. 10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr Definition, Importance and Causes of Deflections Derivation of Moment – Curvature Relation The Double Integration Method 1 3 2
  • 2.
  • 3.
  • 4. 10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■ Importance of Deflections ■ In Addition the analysis of indeterminate structures requires the calculation of deflections as in advance step
  • 5.
  • 6.
  • 7. 10/15/11 DEFLECTIONS of STRUCTURES Tharwat Sakr ■ Methods to calculate Deflections 1. The Double Integration Method. 5. The Real Work Method. 2. The Moment Area Method. 3. The Elastic Load Method. 4. The Conjugate Beam Method. 6. The Virtual Work Method.
  • 8.
  • 9.
  • 10. 10/15/11 3. The Depth – Span Ration is very small ( Slender Members) THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions Slender Beam Deep Beam
  • 11. 10/15/11 3. The Deflection is very – small compared to Span (Small deflection) THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Main Assumptions
  • 12. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE
  • 13. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves) Curvature of elastic line
  • 14. THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
  • 15. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves) To be in x, y
  • 16. 10/15/11 As  is so small THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
  • 17. 10/15/11 As Then THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
  • 18. 10/15/11 Lead to THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
  • 19. 10/15/11 For Very small values of deflection (y) Is the equation of radius of curvature of any curve and its simplification for very small values of y THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Curvature of Elastic Line (Property of Curves)
  • 20. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship Moment - Curvature Relationship
  • 21. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship
  • 22. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship Elongation at any fiber Strain can be defined as From Hook’s Law
  • 23. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Moment-Curvature Relationship From the stress formula By Substitution From Is the differential equation of the elastic line subjected to moment
  • 24. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Sign Convention Deflection Slope Curvature Is the rate of change of the displacement Is the rate of change of the slope Represents the displacement of the structure Investigating the moment – deflection sign
  • 25. 10/15/11 THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Sign Convention Positive Moment Slope decreased with x Negative Moment Slope Increased with x
  • 26. 10/15/11 Is the Relation between Deflection and Moment THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Sign Convention
  • 27. THE DIFFERENTIAL EQUATION OF THE ELASTIC LINE Concepts Deflection at any point Slope angel at any point Curvature at any point Moment at any point
  • 28. 10/15/11 THE DOUBLE INTEGRATION METHOD
  • 29. 10/15/11 The method is based on the direct application of the differential equation of elastic line THE DOUBLE INTEGRATION METHOD Theoretical Bases
  • 30. THE DOUBLE INTEGRATION METHOD Basic Procedure Derive an Equation of the Moment M as function of position variable x (M(x)) Apply the differential equation of elastic line and integrate twice Apply the Boundary and Continuity conditions to obtain the integration constants Substitute with the integration constants into the deflection and slope equations
  • 31. THE DOUBLE INTEGRATION METHOD Boundary Conditions At Roller support At Hinged support At Fixed support
  • 32. THE DOUBLE INTEGRATION METHOD Continuity Conditions At Any intermediate point
  • 33. 10/15/11 Standard Cases of Beam Deflection Tharwat Sakr
  • 34. 10/15/11 Standard Cases of Beam Deflection Tharwat Sakr

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