Computer Aided Engineering Design

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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
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