5. Forces and equilibrium
From Mechanics
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Revision as of 15:47, 17 September 2009
Theory | Exercises |
5. Forces and Equilibrium
Key Points
If the resultant of the forces acting on a particle is zero we say that these forces are in equilibrium.
The diagram shows an object, of mass 300 kg, that is at rest and is supported by two cables. Find the tension in each cable.
Solution
The diagram shows the forces
acting on the object.
Resolving horizontally or using the horizontal components of the forces:
=T2cos60
T1=T2
Resolving vertically gives;
+T2sin60
=2940
Now solving the equations by substituting
+T2sin60
=29402T1sin60
=2940T1=29402sin60
=1700 N (to 3sf)
And also
A particle of mass 6 kg is suspended by two strings as shown in the diagram. Note that one string is horizontal. Find the tension in each string.
Solution
The diagram shows the forces acting on the particle.
Resolving vertically:
=58
8T1=58
8sin60
=67
9 N (to 3 sf)
Resolving horizontally:
=T2T2=58
8sin60
cos60
=33
9 N (to 3sf)
A lorry of mass 5000 kg drives up a slope inclined at
Solution
Model the lorry as a particle.
The diagram shows the forces acting on the lorry.
Resolving perpendicular to the slope gives:
=48800 N (to 3 sf)
Resolving parallel to the slope gives:
=4270 N (to 3sf)
A child, of mass 30kg, slides down a slide at a constant speed. Assume that there is no air resistance acting on the child. The slide makes an angle of
Solution
Model the child as a particle.
The diagram shows the forces acting on the child.
Resolving parallel to the slope gives.
=189 N (to 3sf)
Resolving perpendicular to the slope gives:
As the child is sliding
R
=
294cos40
=294sin40
294cos40
=tan40
=0
840 (to 3 sf)
Note – Angle of Friction
If a particle of mass
Then using
R
mgcos
sin
cos
tan
A crate of mass 200 kg is on a horizontal surface. The coefficient of friction between the crate and the surface is 0.4. The crate is pulled by a rope, as shown in the diagram, so that the crate moves at a constant speed in a straight line. Find the tension in the rope.
Solution
The diagram shows the forces
acting on the crate.
Resolving horizontally:
Resolving vertically:
=1960
or
As the crate is sliding we can use
R
4R
Using this equation with the horizontal and vertical equations gives:
=0
4
1960−Tsin20
Tcos20
=784−T
0
4sin20
Tcos20
+T
0
4sin20
=784T
cos20
+0
4sin20
=784T=784cos20
+0
4sin20
=728 N (to 3sf)