14. Moments and equilibrium
From Mechanics
Theory | Exercises | Video |
Key Points
For a body in equilibrium:
• The resultant force on the body must be zero.
and
• The resultant moment of the forces on the body about all points must be zero.
Sometimes it is more convenient to solve a problem just using moments.
A uniform beam has length 8 m and mass 60 kg. It is suspended by two ropes, as shown in the diagram below.
Find the tension in each rope.
Solution
The diagram shows the forces acting on the beam.
Take moments about the point where T1 acts to give:
T2=3
588T2=53
588=352.8=353 N (to 3sf)
Take moments about the point where T2 acts to give:
T1=2
588T1=52
588=235.2=235 N (to 3sf)
Finally for vertical equilibrium we require
A beam, of mass 50 kg and length 5 m, rests on two supports as shown in the diagram. Find the magnitude of the reaction force exerted by each support.
Find the maximum mass that could be placed at either end of the beam if it is to remain in equilibrium.
Solution
The diagram shows the forces acting on the beam.
Taking moments about the point where R1 acts gives:
R2=1.5
490R2=21.5
490=367.5=368 N (to 3sf)
Taking moments about the point where R2 acts gives:
R1=0.5
490R1=20.5
490=122.5=123 N (to 3sf)
For vertical equilibrium we require
First consider the greatest mass that can be placed at the left hand end of the beam. The diagram below shows the extra force that must now be considered. When the maximum possible mass is used,
Taking moments about the point where R1 acts gives:
mg=1.5
490m=9.81.5
490=75 kg
Similarly for a mass placed at the right hand end of the beam:
mg=0.5
490m=2g0.5
490=12.5 kg
Hence the greatest mass that can be placed at either end of the beam is 12.5 kg.
A ladder, of length 3 m and mass 20 kg, leans against a smooth, vertical wall so that the angle between the horizontal ground and the ladder is 60
a) Find the magnitude of the friction and normal reaction forces that act on the ladder, if it is in equilibrium.
b) Find the minimum value of the coefficient of friction between the ladder and the ground.
Solution
The diagram shows the forces acting on the ladder
a) Considering the horizontal forces gives:
Considering the vertical forces gives:
Taking moment about the base of the ladder gives:
1.5cos60
=S
3sin60
S=3sin60
196
1.5cos60
=2sin60
196
cos60
=1962tan60
=56.6 N (to 3 sf)
But since
b) Using the friction inequality,
R
196
12tan60
0.289 (to 3sf)