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BIOE 3200 - Fall 2015
Galileo’s Beam
To read more about the history of beam theory, check this out:
https://newtonexcelbach.wordpress.com/2008/02/27/the-history-of-the-theory-of-beam-bending-part-1/
Normal and
Shear
Stresses in
Bending
Learning objective:
◦ Determine normal (σx) and shear (τxy)
stresses in beams in bending
BIOE 3200 - Fall 2015
Axial loads in long bones create
bending
BIOE 3200 - Fall 2015
Normal Stresses in Beams
BIOE 3200 - Fall 2015
From http://www.strucalc.com/engineering-
resources/normal-stress-bending-stress-shear-stress/
Normal stress in beam cross-
section in bending:
σx =
𝑀 𝑧
𝐼
𝑦 𝑑𝐴 =
𝑀 𝑧
𝑦
𝐼 𝑧
σx = Normal (flexural) stress
Mz= Bending moment
y = vertical distance from the neutral axis
Iz = Second moment of area
Definition of
normal stress:
Shear Stresses in Beams
BIOE 3200 - Fall 2015
Shear stress in beam cross-section in bending:
τxy =
𝑉 𝑥 𝑑𝑥
𝐼
𝑦 𝑑𝐴 =
𝑉(𝑥)𝑄
𝑡𝐼 𝑧
τxy = Shear stress
Q = first moment of the shaded area with respect to the neutral axis
V(x) = Calculated shear at specific section
y = vertical distance from the neutral axis
I = Second moment of area
t = Width of beam at depth of specific section
What is the first moment of area?
 Area: A = 𝐴
𝑑𝐴
 First moment of area
𝑄 𝑦 = 𝐴
𝑥 𝑑𝐴 ; 𝑄 𝑥 = 𝐴
𝑦 𝑑𝐴
◦ Qy=Axc , Qx=A yc ; Q=0 about centroid
axes
 Centroid:
◦ xc = Qy/A
◦ yc = Qx/A
 Second moment of area:
 𝐼x = 𝑦2
𝑑𝐴
◦ 𝐼 = 𝑏ℎ3
12
for rectangular cross sections
BIOE 3200 - Fall 2015
Calculating first moment of area Q(y) at
a point p in a rectangular cross-section:
 𝑦𝑝 : Distance from origin of z-y
coordinate (centroid of the rectangle)
to centroid of the shaded area
 y : Distance from origin of z-y
coordinate (centroid of the rectangle)
to bottom of the shaded area (where p
is located)
 𝐴 𝑝: Area value of the shaded area
 b = width of beam; h = height of beam
 Qx=𝐴 𝑝 𝑦𝑝
BIOE 3200 - Fall 2015

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7 bending stresses

  • 1. BIOE 3200 - Fall 2015 Galileo’s Beam To read more about the history of beam theory, check this out: https://newtonexcelbach.wordpress.com/2008/02/27/the-history-of-the-theory-of-beam-bending-part-1/ Normal and Shear Stresses in Bending
  • 2. Learning objective: ◦ Determine normal (σx) and shear (τxy) stresses in beams in bending BIOE 3200 - Fall 2015
  • 3. Axial loads in long bones create bending BIOE 3200 - Fall 2015
  • 4. Normal Stresses in Beams BIOE 3200 - Fall 2015 From http://www.strucalc.com/engineering- resources/normal-stress-bending-stress-shear-stress/ Normal stress in beam cross- section in bending: σx = 𝑀 𝑧 𝐼 𝑦 𝑑𝐴 = 𝑀 𝑧 𝑦 𝐼 𝑧 σx = Normal (flexural) stress Mz= Bending moment y = vertical distance from the neutral axis Iz = Second moment of area Definition of normal stress:
  • 5. Shear Stresses in Beams BIOE 3200 - Fall 2015 Shear stress in beam cross-section in bending: τxy = 𝑉 𝑥 𝑑𝑥 𝐼 𝑦 𝑑𝐴 = 𝑉(𝑥)𝑄 𝑡𝐼 𝑧 τxy = Shear stress Q = first moment of the shaded area with respect to the neutral axis V(x) = Calculated shear at specific section y = vertical distance from the neutral axis I = Second moment of area t = Width of beam at depth of specific section
  • 6. What is the first moment of area?  Area: A = 𝐴 𝑑𝐴  First moment of area 𝑄 𝑦 = 𝐴 𝑥 𝑑𝐴 ; 𝑄 𝑥 = 𝐴 𝑦 𝑑𝐴 ◦ Qy=Axc , Qx=A yc ; Q=0 about centroid axes  Centroid: ◦ xc = Qy/A ◦ yc = Qx/A  Second moment of area:  𝐼x = 𝑦2 𝑑𝐴 ◦ 𝐼 = 𝑏ℎ3 12 for rectangular cross sections BIOE 3200 - Fall 2015
  • 7. Calculating first moment of area Q(y) at a point p in a rectangular cross-section:  𝑦𝑝 : Distance from origin of z-y coordinate (centroid of the rectangle) to centroid of the shaded area  y : Distance from origin of z-y coordinate (centroid of the rectangle) to bottom of the shaded area (where p is located)  𝐴 𝑝: Area value of the shaded area  b = width of beam; h = height of beam  Qx=𝐴 𝑝 𝑦𝑝 BIOE 3200 - Fall 2015

Editor's Notes

  1. σx balances moment Mz across cross section of beam
  2. Shear stress balances shear force across cross section of beam
  3. Just as the moment of force is force times distance from an axis, the moment of area is area times the distance from an axis. The point at which mass is concentrated is called the center of gravity. The point at which area is concentrated is called the centroid. If area is a flat thin slice of a mass, the centroid is then at the same place as the center of gravity. This point is where you could balance the thin sheet on a sharp point and it would not tip off in any direction.
  4. Full explanation of how to calculate Q shown in text on pp. 218 – 219, Example 5.4.