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()
()
()
x
φ
φ
y
N
mod
(
)
()
( ) ()
r
x t
,
x
t
Φη (4.7)
x
t
=
η
=
z
i
i
1
=
x
φ
θ
i
where N mod is the number of modes that has been deemed necessary for a sufficiently
accurate or representative solution.
Fig. 4.3 Mode shapes
()
()
Φ and the vector
η that contains the so-called gener-
The mode shape matrix
alised coordinates are defined by
()
()
()
()
x
x
...
x
...
x
Φφ
=
φ
φ
1
i
N
mod
(4.8)
T
()
()
()
()
η
t
t
.....
t
.....
t
=
η
η
η
1
i
N
mod
The introduction of Eq. 4.7 into the equilibrium equations, followed by consecutive
weighing with each (orthogonal) mode shape and span-wise integration will then render
N
equivalent modal equilibrium conditions
mod
M η C η K η Q
⋅+
⋅+
⋅=
(4.9)
0
0
0
tot
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