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96

10

1

10

2

10

-3

10

-2

10

-1

10

0

10

1

10

2

10

3

10

4

K

c

or K

Ic

final failure

Threshold

da/dN = C(

Δ

K)

n

Region 3:

Rapid

unstable

crack

growth

Region 2:

Power law

behaviour

Region 1:

Slow crack

growth

Δ

K

th

da/dN, nm/ciklus

Δ

K, MPa m

1/2

Figure 8. Asymptotic behaviour of

da

/

dN

vs.

ΔK

plot for 13 CrMo 4 4 steel at either end

and a linear portion in the central part /16/

Figure 9. The influence of

R

value on the fatigue

crack growth characteristics of a steel /17/

The crack length (

a

) increases with the number of fatigue cycles,

N

, when a

component or a specimen containing a crack is subjected to cyclic loading, if the load

amplitude (

ΔP

), load ratio (

R

), and cyclic frequency (

v

), are held constant. The crack

growth rate,

da

/

dN

, increases as the crack length increases during a given test and in

structure. The

da

/

dN

is higher at any given crack length at higher load amplitudes. Thus,

the following functional relationship can be derived from these observations:

(

)

R,

da

f P,a

dN

ν

⎛ ⎞ = Δ

⎜ ⎟

⎝ ⎠

(4)

where the function

f

is dependent on the geometry of the specimen or component, the

crack length, the loading configuration, and the cyclic load range. This general relation is

simplified with the use of the

ΔK

parameter as summarized below.

In 1963, Paris and Erdogan /18/ published an analysis with sufficient fatigue crack

growth rate (FCGR) data, deriving a correlation between

da

/

dN

and the cyclic stress

intensity parameter,

ΔK

. They argued that

ΔK

characterizes the magnitude of the fatigue

stresses in the crack tip region, characterizing the crack growth rate in agreement with the

relationships of Eq. (4). The parameter

ΔK

accounts for the magnitude of the load range

(

ΔP

) as well as the crack length

a

and geometry. Later studies /19/ has confirmed the

findings of Paris and Erdogan. The data for intermediate FCGR values can be represented

by the simple mathematical relationship, commonly known as the Paris equation:

(

)

n

I

da C K

dN

⎛ ⎞ = ⋅ Δ

⎜ ⎟

⎝ ⎠

(5)

where

C

and

n

are constants that can be obtained from the intercept and slope,

respectively, of the linear log

da

/

dN

versus log

ΔK

plot (Figs. 8 and 9).