7b-ex
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7b-ex. Combined Loading Examples• Ex. 7b.1
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Example 7b.1
Given: Consider the road sign of Example 2b.5. The
forces, moments, and torque acting at a cross-section
near the base of the mast are shown and right (Cut A-A).
Req'd: Determine the stress states at the surface of the
mast, at Points A, B, C and D. Point :
• A is on the windward side (facing the wind),
• C is on the "leeward side" (back side),
• B is on the left side, and
• D is on the right side of the mast.
Draw 2-d stress elements as you look from the outside of
the mast inward.
Forces, Moments and Torqueacting at Cut A-A.
Road Sign
Sol'n:
Step 1. Consider the five different types of loads acting at the cross-section individually. Then,
determine the stresses that each load causes, and at what points the stresses act.
Each load causes the mast to act as a different type of member, e.g.:
Under the torque, the mast acts as a torsion member.
Because of the shear force, the mast acts as a beam.
The weight makes it act like an axial member.
Load Mast Acts as Causes Stress at Surface
Torque, T Shaft about z-axis
Shear Force, V (y-direction) Beam about x-axis
Moment, Mx Beam about x-axis
Moment, My Beam about y-axis
Axial Force, W=Ws+Wm(z)Axial Member
along z-axis
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Ix is the Moment of Inertia about the x-axis.
Iy is the Moment of Inertia about the y-axis.
Step 2. Consider how each of the loads affects Point A.
Loads Causing Stresses at Point A. Coordinates: x=0, y= –R
Load Mast Actsas
Stress Equation for Stress atSurface.
Does Pt. A "feel" thisstress?
Stress that actsat Point A
Torque, TShaft about
z-axis
Yes – entire cross-section
supports torque
Shear Force,
V
Beam
about
x-axis
No – shear stress is zero at the
"top and bottom" of a beam
(Points A&C) - the mast acts
as a beam bending against the
shear force caused by the wind
0
Moment, Mx
Beam
about
x-axis
Yes (tension) – bending
stress is maximum at "top
and bottom" of beam
Moment, My
Beam
about
y-axis
No – bending stress is zero atCentroidal Axis, about which
beam is bending (the y-axis for
My)
0
Axial Force,
W=Ws+Wm(z)
Axial
Member
Yes (compression) – entire
cross-section supports axial
load
Point A feels three stresses:
shear stress due to the torque;1.
normal stress (tensile) due to the bending moment
about the x-axis;
2.
normal stress (compressive) due to the weight.3.
What are the stresses at the other points?
Stress State at Pt. A
Step 3. By knowing the loads (forces, torques and moments) that occur at the cross-section, the
stresses that act on the other elements can also be found:
Loads Causing Stresses:
Load Mast Acts as Stress Equation Pt. A Pt. B Pt. C Pt. D
Torque, TTorsion Member
about z-axisYes Yes Yes Yes
Shear Force, VBeam about
x-axisNo Yes No
Yes;
opposite
stress of
torsion
Moment, MxBeam about
x-axisYes (+) No Yes (–) No
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Moment, MyBeam about
y-axisNo Yes (–) No Yes (+)
Axial Force,
W=Ws+Wm(z)Axial Member Yes (–) Yes (–) Yes(–) Yes (–)
Notes on Normal Stresses:
(+) means normal stress is tensile.
(–) means normal stress is compressive.
Ix and Iy are the moments of inertia about the x- and y-axes at the centroid of the cross-
section, respectively. Due to symmetry they are equal.
Notes on Shear Stresses:
At Point B, the Shear Stresses ADD as they are in the same direction (+y-direction);
At Point D, the Shear Stresses SUBTRACT - they are in opposite directions.
Below, Cs = (4/3)[(Ro2
+ RoRi + Ri2) / (Ro
2+ Ri
2)]
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Updated: 05/21/09 DJD
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