Geoscience Reference
In-Depth Information
Figure 4.8 2-D local coordinate transformation.
and k = 1 ϕ k =
k
j
and satisfy
ϕ k
j ,
η
) = δ
1. They are written as
j
2
2
(ξξ k + ξ
)(ηη k + η
)/
4 k
=
1, 3, 7, 9
2
2
(ξξ k + ξ
)(
1
η
)/
2
k
=
4, 6
ϕ k =
(4.84)
2
2
(
1
ξ
)(ηη k + η
)/
2
k
=
2, 8
2
2
(
1
ξ
)(
1
η
)
k
=
5
Differentiating coordinate transformation (4.83) with respect to
ξ
and
η
leads to
x
∂ξ =
k = 1
9
x k ∂ϕ k
∂ξ
,
x
∂η =
k = 1
9
x k ∂ϕ k
∂η
,
(4.85)
k = 1
k = 1
y
∂ξ =
9
y k ∂ϕ k
∂ξ
y
∂η =
9
y k ∂ϕ k
∂η
,
,
and
9
9
9
2 x
∂ξ
2
2 x
∂ξ∂η =
2
2 x
∂η
2
x k
ϕ k
∂ξ
x k
ϕ k
∂ξ∂η
,
x k
ϕ k
∂η
=
,
=
,
2
2
2
2
k
=
1
k
=
1
k
=
1
(4.86)
9
9
9
2 y
∂ξ
2
2 y
∂ξ∂η =
2
2 y
∂η
2
y k
ϕ k
∂ξ
y k
ϕ k
∂ξ∂η
y k
ϕ k
∂η
=
,
,
=
.
2
2
2
2
k
=
1
k
=
1
k
=
1
The Jacobian determinant is Eq. (4.76). The first and second derivatives are given
by Eqs. (4.77), (4.78), and (4.80)-(4.82).
For a 3-D problem, the volume formed by twenty-seven points shown in Fig. 4.9
is adopted as the basic element. This irregular element is turned into a cube by the
following coordinate transformation between the physical domain ( x , y , z ) and the
logical domain (
ξ
,
η
,
ζ
):
27
27
27
x
=
x k ϕ k
,
η
,
ζ)
,
y
=
y k ϕ k
,
η
,
ζ)
,
z
=
z k ϕ k
,
η
,
ζ)
(4.87)
k
=
1
k
=
1
k
=
1
 
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