Information Technology Reference
In-Depth Information
TABLE 4.3
Transfer Matrix for a Beam Elements, Part a: ( Continued )
Note: The column 5 definitions of Part b along with case 6 or 7 of Part c of this table apply for
any magnitude of
. However, usually the transfer matrix elements will then be complex
quantities, and the computer calculations may be quite difficult.
To use this general transfer matrix, follow the steps:
λ
,
ζ
,
η
1.
Calculate the three parameters
λ
,
ζ
, and
η
. If shear deformation is not to be considered, set
1
/
k s GA
=
0
2.
Compare the magnitude of these parameters and look up the appropriate e i functions in Parts
b and c of this table.
3.
Substitute these e i expressions in the general transfer matrix above.
A second general, viable technique for deriving transfer matrices is based on the use
of the Laplace transform. The homogeneous form of Eq. (4.94) can be combined into a
single fourth-order equation
d 4
w
dx 4 + η)
d 2
w
dx 2 + ζη)w =
0
(4.109)
where
k )/
ζ = (
N
EI,
η =
k
/(
k s GA
)
,
λ =
k
/
EI
The Laplace transform of Eq. (4.109) is
[ s 4
s 2
w(
s
)
+ η)
+ ζη)
]
s 3
s 2
w (
w (
) + w (
) + η)w (
=
w(
0
) +
0
) +
s
0
0
0
) + η)
s
w(
0
)
(4.110)
where s is the transform variable. The inverse transform gives
w(
) =
[ e 1 (
) + η)
e 3 (
)
w(
) +
[ e 2 (
) + η)
e 4 (
)
w (
)
x
x
x
]
0
x
x
]
0
)w (
)w (
+
e 3 (
) +
e 4 (
)
x
0
x
0
(4.111)
where
L 1
s 4 i
e i (
x
) =
(4.112)
s 4
+ η)
s 2
+ λ ζη
The quantity L 1 indicates the inverse Laplace transform. It follows from Eq. (4.112) that
several useful identities hold:
d
dx e i + 1 (
e i (
x
) =
x
)
i
=−
2 ,
1 , 0 , 1 , 2 , 3
(4.113)
x
e i + 1 (
x
) =
e i (
u
)
du
i
=
4 , 5 , 6
0
Take the first three derivatives of
w(
x
)
and arrange the results as
w(
x
)
e 1 + η)
e 3
e 2 + η)
e 4
e 3
e 4
w(
0
)
=
w (
x
)
e 0 + η)
e 2
e 1 + η)
e 3
e 2
e 3
w (
0
)
(4.114)
w (
w (
x
)
e 1 + η)
e 1
e 0 + η)
e 2
e 1
e 2
0
)
w (
w (
x
)
e 2 + η)
e 0
e 1 + η)
e 1
e 0
e 1
0
)
w
(
x
) =
Q
(
x
)
w
(
0
)
Search WWH ::




Custom Search