stresses due to bending shear

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    Shear force and bendingShear force and bendingmoment diagrammoment diagram

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    Stresses due to bendingStresses due to bending

    Figure shows aFigure shows aslender memberslender member

    (beam) subjected to(beam) subjected toshear force andshear force andbending moment.bending moment.We will beWe will beconsidering onlyconsidering onlysymmetrical beams.symmetrical beams.

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    Concept of CurvatureConcept of Curvature

    The curvature of aThe curvature of aplane curve is definedplane curve is definedas the rate of changeas the rate of change

    of the slope angle ofof the slope angle ofthe curve with respectthe curve with respectto distance along theto distance along thecurve.curve.Curvature !Curvature ! "" ## $%$% ! ! $$ ss

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    GeometryGeometry

    of pureof purebendingbending

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    Geometry of pure bendingGeometry of pure bending

    From symmetry& we conclude thatFrom symmetry& we conclude thatin pure bending'in pure bending'

    ..lane sections remain plane.lane sections remain plane.

    .. Initially parallel sections have aInitially parallel sections have acommon intersection. The beamcommon intersection. The beambends into the arc of a circle.bends into the arc of a circle.

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    Geometry of pure bendingGeometry of pure bending

    Figure shows aFigure shows asegment of asegment of abeam beforebeam before

    deformation.deformation.The lines I* andThe lines I* and+, initially+, initiallye-ual in lengthe-ual in lengthdeform intodeform intoarcs of circles.arcs of circles.

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    Geometry of pure bendingGeometry of pure bending

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    Stresses obtained from stress-Stresses obtained from stress-strain relationsstrain relations

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    Equilibrium RequirementsEquilibrium Requirements

    -uilibrium re-uires that the resultant of-uilibrium re-uires that the resultant of

    the stress distribution over the crossthe stress distribution over the crosssection of the beam should e-ual thesection of the beam should e-ual thebending moment +bending moment + bb..

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    Equilibrium Requirements on anEquilibrium Requirements on anelemental areaelemental area A A

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    The transverse stressesThe transverse stresses // yy&&// 00 andand 11y0y0 are assumed to be 0eroare assumed to be 0ero

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    Equilibrium Requirements on anEquilibrium Requirements on anelemental areaelemental area A A

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    2r&2r& 3344## // 44 ! # 5y! ! # 5y! ""Which gives'Which gives' // 44 # 5 y!# 5 y! ""

    6ubstituting in the e-uilibrium6ubstituting in the e-uilibriume-uations'e-uations'

    77 88// 44 d8# 5d8# 5 77 88 y!y! "" d8 # 9d8 # 9Which implies 5 !Which implies 5 ! "" 77 88 y d8 # 9y d8 # 9

    Thus the neutral surface passes thruThus the neutral surface passes thruthe area centroid.the area centroid.

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    6ubstituting6ubstituting // 44 # 5 y!# 5 y! "" in the secondin the seconde-uilibrium e-uation gives'e-uilibrium e-uation gives'

    77 88// 44 0d8# 50d8# 5 77 88 y0!y0! "" d8 # 9d8 # 9Which implies 5 !Which implies 5 ! "" 77 88 y0 d8 # 9y0 d8 # 9

    This is automatically satisfied since theThis is automatically satisfied since thesection is symmetrical about y a4is.section is symmetrical about y a4is.

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    6ubstituting6ubstituting // 44 # 5 y!# 5 y! "" in the thirdin the thirde-uilibrium e-uation gives'e-uilibrium e-uation gives'

    5577 88// 44 yd8#yd8# 77 88 yy )) ! ! "" d8 # +d8 # + bbWhich implies !Which implies ! "" 77 88 yy )) d8 # +d8 # + bb

    :ut I:ut I 0000 ## 77 88 yy )) d8d82r& d2r& d %% !ds# ! !ds# ! "" # +# + bb ! I ! I 0000

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    6ubstitution in the stress and strain6ubstitution in the stress and straine4pressions gives'e4pressions gives'33

    44 # 5 +# 5 +

    bby! Iy! I

    0000

    8nd8nd// 44 # 5+# 5+ bby! Iy! I 0000

    Which e4press the strain and stressWhich e4press the strain and stressin terms of the applied bendingin terms of the applied bendingmoment.moment.

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    Stress-Strain relationsStress-Strain relations

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    Stress and Deformation in symmetricalStress and Deformation in symmetricalelastic beams sub ected to pure bendingelastic beams sub ected to pure bending

    6ubstituting e4pressions for stresses&6ubstituting e4pressions for stresses&we can obtain'we can obtain'33

    yy## ;; ++

    bby! Iy! I

    0000

    8nd8nd3300 ## ;; ++ bby! Iy! I 0000

    8lso8lso

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    Geometry of pure bendingGeometry of pure bending

    ffect offfect oftransversetransversestrains on thestrains on the

    deformeddeformedshape of ashape of arectangularrectangularbeambeam

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    Stresses in symmetrical beams transmittingStresses in symmetrical beams transmittingbending moment and shear forcebending moment and shear force

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    Stresses inStresses insymmetricalsymmetrical

    beamsbeams

    transmittingtransmitting

    bendingbendingmoment andmoment and

    shear forceshear force

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    Stresses in symmetrical beams transmittingStresses in symmetrical beams transmittingbending moment and shear forcebending moment and shear force

    The e-uilibrium e-uations for the segment is shown above.The e-uilibrium e-uations for the segment is shown above.6ubstituting stress5 moment relation in the above e-uation gives'6ubstituting stress5 moment relation in the above e-uation gives'

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    Stresses inStresses insymmetricalsymmetrical

    beamsbeams

    transmittingtransmittingbending momentbending momentand shear forceand shear force