Issue 58
R.N. da Cunha et alii, Frattura ed Integrità Strutturale, 58 (2021) 21-32; DOI: 10.3221/IGF-ESIS.58.02
U
T
1 1 ...
i
j
n
u w
u w
u w
u w
...
...
(1)
i
i
j
j
n
n
1
P
T
P P P
P P P
P P P
P P P
1 ...
...
...
(2)
i
u
w
ui
wi
uj
wj
j
un
wn
n
1
1
where u 1 is the node 1 displacement parallel to the X-axis, w 1 is the node 1 displacement parallel to the Z-axis and θ 1 is the node 1 rotation on the XZ plane. Analogously, P un is the applied force on node n parallel to the X-axis, P wn is the applied force on node n parallel to the Z-axis and P θ n is the applied moment on node n on the XZ plane.
The structural equilibrium is given by:
b P B M 1 m T b
(3)
b
being [ B ] b the transformation matrix and { M } b the generalised stresses of a finite element b, both given as follows:
M
T
M M N
(4)
i
j
i
b
Frame element:
b
b
sin
cos
sin cos L L sin cos L L b b b
b
0 0 0 ...
1 ...
0 ... 0 0 0
L
L
b
b
b
b
b
sin
cos
B
b
0 0 0 ...
0 ...
1 ... 0 0 0
(5)
b
L
L
b
b
b
b
sin
0 0 0 ...
cos
0 ... cos
sin 0 ... 0 0 0
b
b
b
b
node
node i
node j
node n
1
Arch element:
node
node i
1
b
b
sin
cos
0 0 0 ...
1 ...
b
b
R
R
sin
sin
b
b
b
b
sin
cos
B
0 0 0 ...
0 ...
b
b
b
R
R
sin
sin
b
b
cos 1 sin sin b b
cos 1 cos sin b b
b
b
0 0 0 ... cos
sin
0 ...
b
b
sin
cos
sin b b b R sin b b
sin cos b b b b b R
cos
cos
sin
cos
b
b
b
b
...
0 ... 0 0 0
R
R
b
b
cos
cos
sin
cos
b
b
b
b
b
b
b
b
b
b
...
1 ... 0 0 0
b
b
R
R
R
R
sin
sin
b
b
b
b
(6)
cos 1 sin b
cos 1 cos b
b
b
b
b
...
cos
sin
0 ... 0 0 0
b
b
b
b
b
b
sin
sin
node j
node n
23
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