Mechanical Engineering Principles

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FORCES ACTING AT A POINT 27

3.4 The resultant of two coplanar


forces


For two forces acting at a point, there are three
possibilities.

(a) For forces acting in the same direction and
having the same line of action, the single force
having the same effect as both of the forces,
called theresultant forceor just theresultant,
is the arithmetic sum of the separate forces.
Forces ofF 1 andF 2 acting at pointP, as shown
in Figure 3.5(a), have exactly the same effect
on pointPas forceFshown in Figure 3.5(b),
where F = F 1 +F 2 and acts in the same
direction asF 1 andF 2. ThusFis the resultant
ofF 1 andF 2

P

P

F 2

F

F 1

(F 1 +F 2 )

(a)

(b)

Figure 3.5

(b) For forces acting in opposite directions along
the same line of action, the resultant force is the
arithmetic difference between the two forces.
Forces ofF 1 andF 2 acting at pointPas shown
in Figure 3.6(a) have exactly the same effect
on pointPas forceFshown in Figure 3.6(b),
whereF =F 2 −F 1 and acts in the direction
ofF 2 ,sinceF 2 is greater thanF 1.


ThusFis the resultant ofF 1 andF 2

P

P

F 1

F

F 2

(F 2 – F 1 )

(a)

(b)

Figure 3.6

(c) When two forces do not have the same line
of action, the magnitude and direction of the

resultant force may be found by a procedure
called vector addition of forces. There are two
graphical methods of performingvector addi-
tion, known as thetriangle of forcesmethod
(see Section 3.5) and theparallelogram of
forcesmethod (see Section 3.6)

Problem 1. Determine the resultant force of
two forces of 5 kN and 8 kN,

(a) acting in the same direction and having
the same line of action,

(b) acting in opposite directions but having
the same line of action.

P

P

8 kN

8 kN

5 kN

0

Scale
5 10 kN (force)

(a)

(b)

5 kN

Figure 3.7

(a) The vector diagram of the two forces acting in
the same direction is shown in Figure 3.7(a),
which assumes that the line of action is hori-
zontal, although since it is not specified, could
be in any direction. From above, the resultant
forceFis given by:

F=F 1 +F 2 ,

i.e. F=( 5 + 8 )kN=13 kN

in the direction of the original forces.
(b) The vector diagram of the two forces acting in
opposite directions is shown in Figure 3.7(b),
again assuming that the line of action is in a
horizontal direction. From above, the resultant
forceFis given by:

F=F 2 −F 1 ,i.e.F=( 8 − 5 )kN

=3kN

in the direction of the 8 kN force.
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