CENE 437
Introduction
Locating the n.a.
Moment Capacity
Analysis Examples
Design



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 CENE 437: The Class: Masonry Beams: Bending: Introduction


Bending

Introduction to Masonry Beams

General Discussion | Behavior | Adapt to Reinforced Masonry Beams


  • A masonry beam is composed of solidly grouted units reinforced with steel.

  • It is often called a lintel when spanning over openings in walls.



  • The design method used here is Working Stress Design (WSD). Its relationship to other methods used in masonry is shown in the following stress-strain figure.



  • WSD assumptions:
    • Plane secions remain plane during and after bending.
    • s is proportional to e
    • e is proportional to the distance from n.a.
    • Masonry is cracked:
      • It carries no tensile stresses.
      • Reinforcing steel resists tension.
      • Masonry resists compressive stresses only
    • Design stresses within elastic range.
    • Perfect bond between steel and grout.

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Behavior in Bending - A Review



  • During the bending deformation of a simply-supported beam:
    • Upper fibers shorten due to axial compression
    • Lower fibers lengthen due to axial tension
    • Fiber at n.a. => No Deformation => No Strain

  • More Deformation => More Strain => More Stress

  • Generic distribution of stress across the cross section of a beam:
    • Stresses act normal to cross section.
    • These axial stresses are induced by bending that is quantified in terms of the internal bending moment, M.



    • M = Ca = Ta
      • Where M is the internal force couple (i.e. bending moment) that resists the externally generated M which is a function of span, support conditions, and loads.

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Adapt to Reinforced Masonry Beams
  • Reinforced masonry beams are orthotropic.

  • Recall the WSD assumptions: masonry resists compression and steel resists tension.
    • In effect, this means that we assume that the masonry beam is cracked below the n.a. and cannot resist any tension.
    • This really isn't true under working loads, and therefore results in a large safety margin.
    • But, the uncertainty of measuring tensile stress in masonry necessitates this.

  • The modified stress distribution for reinforced masonry bending member:




  • Because we assume a perfect bond between steel and grout:
    • Strain in steel = strain in grout at corresponding location.

  • With this assumption we can transform the masonry-steel section into a section of one material: masonry.

  • Transform the steel into an equivalent masonry area by multiplying As by n, the modular ratio.
    n = Es / Em
    where Es = 29 x 10 6 psi, and
    Em = 750 (f ` m) £ 3 x 10 6 for concrete unit masonry.




  • The resultant compressive force can be found from essentially a volume calculation:
    F = s A = 1/2 fm ( k d ) b = C

  • Likewise, the resultant tensile force is:
    F = s A = (fs / n) (n As) = As fs

  • The internal resisting bending moment is then:
    M = Ca = Ta, but a = j d for reinforced masonry beams, and
    M = 1/2 fm k j b d2 or M = As fs j d.

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Send Email to Deb Larson at Debra.Larson@nau.edu


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