324 COMPUTER AIDED ENGINEERING DESIGN
ui vi θi uj vj θj
k =
00– 00
0 12 6 0 – 12 6
06 4 0–6 2
–00 00
0 – 12 – 6 0 12 – 6
06 2 0–6 4
32 32
22
32 3 2
22
AE
l
AE
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
AE
l
AE
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
EI
l
⎡
⎣
⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢
⎤
⎦
⎥
⎥
⎥
⎥
⎥⎥
⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥
u
u
i i i j j j
v
v
θ
θ
(11.9h)
11.5.1 Frame Elements and Transformations
For a frame element to be oriented at an angle θ in the x-y plane (Figure 11.10), the displacements
along the x and y global coordinate axes, namely, uix,uiy for node i and ujx,ujy for node j can be
extracted using the following transformation. Note that the rotations θi and θj remain invariant.
ue
ix
iy
i
jx
jy
j
i
i
i
j
j
u
u
u
u
u
u
= =
cos – sin 0 0 0 0
sin cos 0 0 0 0
001000
0 0 0 cos – sin 0
0 0 0 sin cos 0
000001
θ
θ
θθ
θθ
θθ
θθ
θ
⎛
⎝
⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜
⎞
⎠
⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟
⎛
⎝
⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜
⎞
⎠
⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟
v
v
θθj
T
⎛
⎝
⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜
⎞
⎠
⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟
= u (11.9i)
The stiffness of the frame element for the displacements (and forces) along the x and y directions,
and rotations (moments) perpendicular to the plane containing the frame element is given similar to
the truss element as
ujy
uj
ujx
vj
θj
ξ
θ
uiy
ui
uix
vi
θi
y
x
Figure 11.10 A frame element oriented at an angle θθθθθ