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For a rigid body to be in equilibrium, the net force as well as the net moment about any arbitrary point O must be equal to zero.
Typology: Summaries
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Today’s Objectives
:
Students will be able to:a) Identify support reactions, and,b) Draw a free-body diagram.
Section 5.1)
In contrast to the forces on a particle, theforces on a rigid-body are not usuallyconcurrent and may cause rotation of thebody (due to the moments created by theforces).
For a rigid body to be in equilibrium, thenet force as well as the net momentabout any arbitrary point O must beequal to zero.
= 0 and
O
Forces on a particle Forces on a rigid body
(Section 5.2)
Draw an outlined shape. Imagine the body to be isolatedor cut
“free” from its constraints and draw its outlined
shape.
Show all the external forces and couple moments. Thesetypically include: a) applied loads, b) the weight of thebody,
and c) support reactions (can be difficult).
Idealized model
Free-body diagram
(continued)
Label loads and dimensions: All known forces andcouple moments should be labeled with theirmagnitudes and directions. For the unknown forcesand couple moments, use letters like A
x
y
A
, etc..
Indicate any necessary dimensions.
Idealized model
Free-body diagram
80 kg load at C. In a FBD of only the beam, there are how manyunknowns?1) 2 forces and 1 couple moment2) 3 forces and 1 couple moment3) 3 forces4) 4 forces
If the directions of the force and the couple moments arereversed, then what will happen to the beam?A)
The beam will lift from A.
B)
The beam will lift at B.
C)
The beam will be restrained.
D)
The beam will break.
A single bearing or hinge can prevent rotation by providing aresistive couple moment. However, it is usually preferred to usetwo or more properly aligned bearings or hinges. Thus, in thesecases, only force reactions are generated and there are nomoment reactions created.
H
y
W
Reaction
couple
H
y
W
T
H
x