Civil Engineering Reference
In-Depth Information
(
)
ˆ
Δ
is the distance between points i and j , and where
Ss
,
where
Δ
ω
,
ij
pp
ij
uv
, or
w
, is the reduced cross spectral density between flow component p at point
i and itself at point j (i.e. the cross spectral density between
=
p
uv
, or
w at ends 1 or 2 of
w at ends 1 or 2 of element m ). As shown in Eq. 2.88, ˆ pp
element n and
uv
, or
S
may be expressed by the product of the reduced single point spectra at points i and j
and the reduced co spectrum between the same points, i.e.
ˆ
(
)
ˆ
ˆ
ˆ
(
)
()
()
Ss
,
S
S
o
s
,
Δ
ω
=
ω
ω
Δ
ω
(9.118)
pp
ij
p
p
pp
ij
i
j
E.g., adopting a Kaimal type of auto spectrum and simple exponential co-spectrum
decay, then (see Eqs. 3.25 and 3.41)
x f
()
()
S
ω
ALVZ
ˆ
p
u
()
p
p
i
i
S
ω
=
=
p i
2
5 3
σ
x f
()
p
v
w
=
11.5
ALVZ
p i
+
ω
p
p
i
()
()
()
x f
S
ω
ALVZ
p
p
p
j
ˆ
j
1
2
1
2
1
2
1
2
()
S
ω
=
=
n
p j
2
5 3
σ
x f
p j
11.5
+
ALVZ
ω
n
p
p
j
i
(9.119)
=
m
2
2
(
)
(
)
cXX
⎤ ⎡
cZZ
ω
+
px
i
j
⎦ ⎣
pz
i
j
m
(
)
ˆ
Co
Δ
s
,
ω
=
exp
pp
ij
V
n
ij
n
j
=
1
2
()
()
V
=
V Z
+
V Z
m
ij
i
j
m
and where indices n or m refers to element numbers and 1 or 2 refers to element end
numbers. By defining the reduced auto spectral density matrices associated with
elements n and m
ˆ
ˆ
ˆ
ˆ
ˆ
ˆ
ˆ
()
i g SSS SSS
S
ω
=
n
u
v
w
u
v
w
⎥ ⎪
1
1
1
2
2
2
n
n
n
n
n
n
(9.120)
ˆ
ˆ
ˆ
ˆ
ˆ
ˆ
ˆ
()
diag S
S
S
S
S
S
S
ω
=
m
u
v w u v w
mm m m m m
1
1
1
2
2
2
⎦⎭
and the reduced covariance matrix between corresponding element ends
Search WWH ::




Custom Search