Issue 33
M. Cova et alii, Frattura ed Integrità Strutturale, 33 (2015) 390-396; DOI: 10.3221/IGF-ESIS.33.43
(14)
, n a , n m b
, , ,2 4
n a eq
1 2
1 2
T
T
, n n
n
n
max
V
V
V
V
1
2
1
2
1 2
1 2
T
T
T
n n
n n
b n
n
S
V
V
1
2
2
2
2
2
b
b
b
b
1
1
1
1
T
T
n
b
, n n
b
n
max
V
V
S
V
V
S
1
2
1
2
And the maximum value, by changing the direction n, is: , ,2 4 , , max 1 1 max a eq n n a eq b b eigvl b
(15)
2
2
b
b
1
1
eigvl
b
,
V
V
S
V
V
S
1
2
1
2
2
2
However, the relative amplitude between the extremes at t 2
and t 4
is only one of the possible critical amplitudes; the other . These two combination are similar to that and t 4
and t 2
and, finally, between t 1
possibilities are the differences between t 1
investigated in the single pulsating loading case. Then the relative equivalent amplitudes are: , , ,1 2 1 1 1 1 max , 2 2 n a eq V S V S b b eigvl b eigvl b
(16)
1
1
b eigvl
b eigvl
,
max
b
b
(17)
2
2
V
S
V
S
41, , ,
eqan
2
2
The researched equivalent amplitude is, finally, the maximum of each computed amplitude; hence the maximum eigenvalue of the suggested six tensors: 1 1 ; 2 1 ; 2 1 ; 2 1 2 1 ; 2 1 2 1 max 1 1 2 1 2 1 , , S V S V S V V S V V eqan b eigvl b eigvl b b eigvl b b eigvl b b b eigvl b b b eigvl (18)
;
;
b
b
2
2
V
S
V
S
2
2
Figure 3 : Stress distribution at minimum et maximum of fatigue loading.
394
Made with FlippingBook - professional solution for displaying marketing and sales documents online