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FIGURE 6.42
A triangular element.
stretching. The displacements in the x direction are approximated by
u x =
N u
,
η)
u x
(6.140)
with the linear expression
N u
=
[1
ξη
]
where
u x 3 ] T
contains the generalized displacements. The transformation to nodal displacement v x fol-
lows the procedure described in Section 6.4.1. Define v x =
=
u x 1
u x 2
u x
[
[ u x 1 u x 2 u x 3 ] T . Then substitute
the
ξ
,
η
coordinates of Fig. 6.42 into Eq. (6.140)
u x 1
u x 2
u x 3
101
100
110
u x 1
=
= N u
u x 2
or
v x
u x
u x 3
It follows that
= N u v x
u x
=
Gv x
with
010
0
G
=
11
1
10
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