Mechanical Engineering Principles

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46 MECHANICAL ENGINEERING PRINCIPLES

Now try the following exercise


Exercise 20 Further problems on a graph-
ical method
Determine the internal forces in the following
pin-jointed trusses using a graphical method:
1.

12

3

60 ° 30 °

R 1 R 2

4 kN

Figure 4.23





R 1 = 3 .0kN, R 2 = 1 .0kN,
1–2, 1.7 kN, 1–3,− 3 .5kN,
2–3,− 2 .0kN





2.

R (^1) R
2
60 ° 30 ° H 2
3
2
6 kN
1
Figure 4.24




R 1 =− 2 .6kN, R 2 = 2 .6kN,
H 2 = 6 .0 kN, 1–2,− 1 .5kN,
1–3, 3.0 kN, 2–3,− 5 .2kN




3.
R 1 R 2
H 11 45 °
3
2
4 kN
6 kN
45 °
Figure 4.25




R 1 = 5 .0kN, R 2 = 1 .0kN,
H 1 = 4 .0kN 1–2,1.0kN,
1–3,−7.1 kN, 2–3,−1.4 kN




4.
2 kN
4 kN
6 kN
3 5
2
4
(^130) ° 30 ° 30 ° 30 °
6
12 m
R 1 R 2
Figure 4.26
⎡ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣
R 1 = 5 .0kN, R 2 = 7 .0kN,
1–3,− 10 .0kN, 1–6,− 8 .7kN,
3–4,− 8 .0kN, 3–6,− 2 .0kN,
4–6, 4.0kN, 4–5,8.0kN,
5–6,− 6 .0kN, 5–2,− 14 .0kN,
6–2, 12.1kN
⎤ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦


4.4 Method of joints (a mathematical


method)


In this method, all unknown internal member forces
are initially assumed to be in tension. Next, an
imaginary cut is made around a joint that has two
or less unknown forces, so that a free body diagram
is obtained for this joint. Next, by resolving forces
in respective vertical and horizontal directions at
this joint, the unknown forces can be calculated.
To continue the analysis, another joint is selected
with two or less unknowns and the process repeated,
remembering that this may only be possible because
some of the unknown member forces have been
previously calculated. By selecting, in turn, other
joints where there are two or less unknown forces,
the entire framework can be analysed.
It must be remembered that if the calculated force
in a member isnegative, then that member is in
compression. Vice-versa is true for a member in
tension.
To demonstrate the method, some pin-jointed
trusses will now be analysed in Problems 8 to 10.
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