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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