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(1, 2)
3
300 psi
Y
1
(0, 0)
2
(1, 0)
X
100 psi
(a)
3
40
Y
2
1
20
10
10
X
(b)
Figure 9.4
(a) Distributed loads on a triangular element.
(b) Work-equivalent nodal forces.
Along edge 1-2, y
=
0 , p x
=
0 , p y
=−
100 psi; hence, Equation 9.39 becomes
1
x 0
x 0
0 0
0
0
100
t d S
f ( p ) =
x
S
0
x
0
0
1
x 0
x 0
0 0
0
0
0
0
10
10
0
0
100
d x =
1
= 0 . 2
lb
x
0
0
x
0
0
 
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