80 2. RELIABILITY OF A COMPONENT UNDER CYCLIC LOAD
where L is the number of different cyclic loading levels and m is a material fatigue property and
is the slope of the traditional S-N curve. m is determined per Equation (2.74). K
f
is the fatigue
stress concentration factor on the component critical section, which has been discussed and can
be calculated per Equations (2.22)–(2.25) in Section 2.6. n
Li
is the number of cycles of the ith
cyclic loading stress level
ai
.
ai
is an equivalent fully reversed cyclic stress amplitude and can
be calculated by the following equation:
ai
D
8
ˆ
ˆ
ˆ
ˆ
<
ˆ
ˆ
ˆ
ˆ
:
a
for a fully reversed cyclic stress
a
m
0 of non-zero mean cyclic stress
a
S
u
.
S
u
m
/
m
> 0 of non-zero mean cyclic stress;
(2.83)
where .
a
;
m
/ are the stress amplitude and the mean stress of cyclic stress. S
u
is the ultimate
material strength. Equation (2.83) is based on the modified Goodman approach for the consid-
eration of the effect of mean stress in cyclic stress.
n
Li
or
ai
can be a constant value or a distributed random variable, which is defined by the
provided cyclic loading spectrum.
Following are the equations for calculating component fatigue damage per given cyclic
spectrum.
For model #1, model #2, and model #3 cyclic loading spectrum .
a
; n
L
/, the component
fatigue damage due to the cyclic loading spectrums is:
D D n
L
K
f
a
m
; (2.84)
where K
f
and m have the same meaning as those in Equation (2.82). For model #1, n
L
is
a constant number of cycles and
a
is the fully reversed constant cyclic stress amplitude. For
the model #2, n
L
is a distributed number of cycles and
a
is the fully reversed constant cyclic
stress amplitude. For model #3, n
L
is a constant number of cycles and
a
is the fully reversed
distributed cyclic stress amplitude.
For model #4, model #5, and model #6 cyclic loading spectrum .
ai
; n
Li
; i D 1; 2; : : : ; L/,
the component fatigue damage due to the cyclic loading spectrums is calculated per Equa-
tion (2.82) and repeated here as Equation (2.85):
D D
L
X
iD1
n
Li
K
f
ai
m
; (2.85)
where K
f
, m, and L have the same meaning as those in Equation (2.82). For model #4, n
Li
is a
constant number of cycles and
ai
is the fully reversed constant cyclic stress amplitude at the i th
cyclic stress level. For model #5, n
Li
is a distributed number of cycles and
ai
is the fully reversed
constant cyclic stress amplitude at the ith cyclic stress level. For model #6, n
Li
is a constant
number of cycles and
ai
is a distributed fully reversed constant cyclic stress amplitude at the ith
cyclic stress level.