Graphics Programs Reference
In-Depth Information
fori=j+1:n
L(i,j) = -dot(L(i,j:i-1), L(j:i-1,j)/L(i,i));
end
end
L(n,n) = 1/L(n,n); Linv = L;
EXAMPLE 9.1
40 MPa
30 MPa
3
0 MPa
80 MPa
60 MPa
The stress matrix (tensor)corresponding to the state of stress shown is
⎡
⎣
⎤
⎦
80 300
3040 0
0060
S
=
MPa
(each row of the matrix consists of the three stress components acting onacoordinate
plane). It can be shown that the eigenvalues of
S
are the
principal stresses
and the
eigenvectors are normal to the
principal planes
. (1) Determine the principalstresses
by diagonalizing
S
with a Jacobi rotation and (2)compute the eigenvectors.
Solution of Part (1)
To e l iminate
S
12
we must applyarotationinthe 1-2plane.With
k
=
1 and
=
2Eq. (9.15) is
S
11
−
S
22
2
S
12
80
40
2(30)
−
2
3
φ
=−
=−
=−
Equation (9.16a) thenyields
φ
−
sgn(
)
1
t
=
1
=
+
(2
1
=−
0
.
53518
2
/
/
3)
2
+
|
φ
| +
φ
+
2
3
According to Eqs. (9.18), the changes in
S
due to the rotationare
S
11
=
S
11
−
tS
12
=
80
−
(
−
0
.
53518)
(
30
)
=
96
.
055 MPa
S
22
=
S
22
+
tS
12
=
40
+
(
−
0
.
53518) (30)
=
23
.
945 MPa
S
12
=
S
21
=
0
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