Crack growth equation

Figure 1 shows a typical plot of the rate of crack growth as a function of the alternating stress intensity or crack tip driving force ${\displaystyle \Delta K}$ plotted on log scales. The crack growth rate behaviour with respect to the alternating stress intensity can be explained in different regimes (see, figure 1) as follows

Regime A: At low growth rates, variations in microstructure, mean stress (or load ratio), and environment have significant effects on the crack propagation rates. It is observed at low load ratios that the growth rate is most sensitive to microstructure and in low strength materials it is most sensitive to load ratio.[13]

Regime B: At mid-range of growth rates, variations in microstructure, mean stress (or load ratio), thickness, and environment have no significant effects on the crack propagation rates.

Regime C: At high growth rates, crack propagation is highly sensitive to the variations in microstructure, mean stress (or load ratio), and thickness. Environmental effects have relatively very less influence.

Cycles with higher stress ratio ${\displaystyle R=K_{\text{min}}}/{K_{\text{max}}\equiv P_{\text{min}}/{P_{\text{max}}}}$ have an increased rate of crack growth.[14] This effect is often explained using the crack closure concept which describes the observation that the crack faces can remain in contact with each other at loads above zero. This reduces the effective stress intensity factor range and the fatigue crack growth rate.[15]

A ${\displaystyle da/dN}$ equation gives the rate of growth for a single cycle, but when the loading is not constant amplitude, changes in the loading can lead to temporary increases or decreases in the rate of growth. Additional equations have been developed to deal with some of these cases. The rate of growth is retarded when an overload occurs in a loading sequence. These loads generate are plastic zone that may delay the rate of growth. Two notable equations for modelling the delays occurring while the crack grows through the overload region are:[16]

The Wheeler model (1972)

${\displaystyle \left({\frac {da}{dN}}\right)_{\text{VA}}=\beta \left({\frac {da}{dN}}\right)_{\text{CA}}}$ with ${\displaystyle \beta =\left({\frac {r_{\text{pi}}}{r_{\text{max}}}}\right)^{k}}$

where ${\displaystyle r_{\text{pi}}}$ is the plastic zone corresponding to the ith cycle that occurs post the overload and ${\displaystyle r_{\text{max}}}$ is the distance between the crack and the extent of the plastic zone at the overload.

The Willenborg model

To predict the crack growth rate at the near threshold region, the following relation has been used[17]

${\displaystyle {da \over dN}=A\left(\Delta K-\Delta K_{\text{th}}\right)^{p}.}$

To predict the crack growth rate in the intermediate regime, the Paris–Erdoğan equation is used[2]

${\displaystyle {da \over dN}=C\left(\Delta K\right)^{m}.}$

In 1967, Forman proposed the following relation to account for the increased growth rates due to stress ratio and when approaching the fracture toughness ${\displaystyle K_{\text{c}}}$[18]

${\displaystyle {da \over dN}={\frac {C(\Delta K)^{n}}{(1-R)K_{\text{c}}-\Delta K}}}$

McEvily and Groeger[19] proposed the following power-law relationship which considers the effects of both high and low values of ${\displaystyle \Delta K}$

${\displaystyle {da \over dN}=A(\Delta K-\Delta K_{\text{th}})^{2}{\Big [}1+{\frac {\Delta K}{K_{\text{Ic}}-K_{\text{max}}}}{\Big ]}}$.

The NASGRO equation is used in the crack growth programs AFGROW, FASTRAN and NASGRO software.[20] It is a general equation that covers the lower growth rate near the threshold ${\displaystyle \Delta K_{\text{th}}}$ and the increased growth rate approaching the fracture toughness ${\displaystyle K_{\text{crit}}}$, as well as allowing for the mean stress effect by including the stress ratio ${\displaystyle R}$. The NASGRO equation is

${\displaystyle {\frac {da}{dN}}=C\left[\left({\frac {1-f}{1-R}}\right)\Delta K\right]^{n}{\left(1-{\frac {\Delta K_{\text{th}}}{\Delta K}}\right)^{p} \over \left(1-{\frac {K_{\max }}{K_{\text{crit}}}}\right)^{q}}}$

where ${\displaystyle C}$, ${\displaystyle f}$, ${\displaystyle n}$, ${\displaystyle p}$, ${\displaystyle q}$, ${\displaystyle \Delta K_{\text{th}}}$ and ${\displaystyle K_{\text{crit}}}$ are the equation coefficients.

In 1967, McClintock developed an equation for the upper limit of crack growth based on the cyclic crack tip opening displacement ${\displaystyle \Delta {\text{CTOD}}}$[21]

${\displaystyle {da \over dN}\propto \Delta {\text{CTOD}}\approx \beta {(\Delta K)^{2} \over {2\sigma _{0}E'}}}$

where ${\displaystyle \sigma _{0}}$ is the flow stress, ${\displaystyle E'}$ is the Young's modulus and ${\displaystyle \beta }$ is a constant typically in the range 0.1–0.5.

To account for the stress ratio effect, Walker suggested a modified form of the Paris–Erdogan equation[22]

${\displaystyle {da \over dN}=C{\Big (}{\overline {\Delta K}}{\Big )}^{m}=C{\bigg (}{\frac {\Delta K}{(1-R)^{1-\gamma }}}{\bigg )}^{m}=C{\big (}K_{\text{max}}(1-R)^{\gamma }{\big )}^{m}}$

where, ${\displaystyle \gamma }$ is a material parameter which represents the influence of stress ratio on the fatigue crack growth rate. Typically, ${\displaystyle \gamma }$ takes a value around ${\displaystyle 0.5}$, but can vary between ${\displaystyle 0.3-1.0}$. In general, it is assumed that compressive portion of the loading cycle ${\displaystyle {\big (}R<0{\big )}}$ has no effect on the crack growth by considering ${\displaystyle \gamma =0,}$ which gives ${\displaystyle {\overline {\Delta K}}=K_{\text{max}}.}$ This can be physically explained by considering that the crack closes at zero load and does not behave like a crack under compressive loads. In very ductile materials like Man-Ten steel compressive loading does contribute to the crack growth according to ${\displaystyle \gamma =0.22}$.[23]

Elber modified the Paris–Erdogan equation to allow for crack closure with the introduction of the opening stress intensity level ${\displaystyle K_{\text{op}}}$ at which contact occurs. Below this level there is no movement at the crack tip and hence no growth. This effect has been used to explain the stress ratio effect and the increased rate of growth observed with short cracks. Elber's equation is[16]

${\displaystyle \Delta K_{\text{eff}}=K_{\text{max}}-K_{\text{op}}}$

${\displaystyle {da \over dN}=C(\Delta K_{\text{eff}})^{m}}$

The general form of the fatigue-crack growth rate in ductile and brittle materials is given by[21]

${\displaystyle {da \over dN}\propto (K_{\text{max}})^{n}(\Delta K)^{p},}$

where, ${\displaystyle n}$ and ${\displaystyle p}$ are material parameters. Based on different crack-advance and crack-tip shielding mechanisms in metals, ceramics, and intermetallics, it is observed that the fatigue crack growth rate in metals is significantly dependent on ${\displaystyle \Delta K}$ term, in ceramics on ${\displaystyle K_{\text{max}}}$, and intermetallics have almost similar dependence on ${\displaystyle \Delta K}$ and ${\displaystyle K_{\text{max}}}$ terms.

There are many computer programs that implement crack growth equations such as Nasgro,[24] AFGROW and Fastran. In addition, there are also programs that implement a probabilistic approach to crack growth that calculate the probability of failure throughout the life of a component.[25][26]

Crack growth programs grow a crack from an initial flaw size until it exceeds the fracture toughness of a material and fails. Because the fracture toughness depends on the boundary conditions, the fracture toughness may change from plane strain conditions for a semi-circular surface crack to plane stress conditions for a through crack. The fracture toughness for plane stress conditions is typically twice as large as that for plane strain. However, because of the rapid rate of growth of a crack near the end of its life, variations in fracture toughness do not significantly alter the life of a component.

Crack growth programs typically provide a choice of:

• cycle counting methods to extract cycle extremes
• geometry factors that select for the shape of the crack and the applied loading
• crack growth equation
• acceleration/retardation models
• material properties such as yield strength and fracture toughness

The stress intensity factor is given by

${\displaystyle K=\beta \sigma {\sqrt {\pi a}},}$

where ${\displaystyle \sigma }$ is the applied uniform tensile stress acting on the specimen in the direction perpendicular to the crack plane, ${\displaystyle a}$ is the crack length and ${\displaystyle \beta }$ is a dimensionless parameter that depends on the geometry of the specimen. The alternating stress intensity becomes

${\displaystyle {\begin{aligned}\Delta K&={\begin{cases}\beta (\sigma _{\text{max}}-\sigma _{\text{min}}){\sqrt {\pi a}}=\beta \Delta \sigma {\sqrt {\pi a}},\qquad R\geq 0\\\beta \sigma _{\text{max}}{\sqrt {\pi a}},\qquad R<0\end{cases}},\end{aligned}}}$

where ${\displaystyle \Delta \sigma }$ is the range of the cyclic stress amplitude.

By assuming the initial crack size to be ${\displaystyle a_{0}}$, the critical crack size ${\displaystyle a_{c}}$ before the specimen fails can be computed using ${\displaystyle {\big (}K=K_{\text{max}}=K_{\text{Ic}}{\big )}}$ as

${\displaystyle {\begin{aligned}K_{\text{Ic}}&=\beta \sigma _{\text{max}}{\sqrt {\pi a_{c}}},\\\Rightarrow a_{c}&={\frac {1}{\pi }}{\bigg (}{\frac {K_{\text{Ic}}}{\beta \sigma _{\text{max}}}}{\bigg )}^{2}.\end{aligned}}}$

The above equation in ${\displaystyle a_{c}}$ is implicit in nature and can be solved numerically if necessary.

For ${\displaystyle R\geq 0.7,}$ crack closure has negligible effect on the crack growth rate[27] and the Paris–Erdogan equation can be used to compute the fatigue life of a specimen before it reaches the critical crack size ${\displaystyle a_{c}}$ as

${\displaystyle {\begin{aligned}{da \over dN}&=C(\Delta K)^{m}=C{\bigg (}\beta \Delta \sigma {\sqrt {\pi a}}{\bigg )}^{m},\\\Rightarrow N_{f}&={\frac {1}{({\sqrt {\pi }}\Delta \sigma )^{m}}}\int _{a_{0}}^{a_{c}}{\frac {da}{(C{\sqrt {a}}\beta )^{m}}}.\end{aligned}}}$

Figure 2: Geometrical representation of Center Cracked Tension test specimen

For the Griffith-Irwin crack growth model or center crack of length ${\displaystyle 2a}$ in an infinite sheet as shown in the figure 2, we have ${\displaystyle \beta =1}$ and is independent of the crack length. Also, ${\displaystyle C}$ can be considered to be independent of the crack length. By assuming ${\displaystyle \beta ={\text{constant}},}$ the above integral simplifies to

${\displaystyle N_{f}={\frac {1}{C({\sqrt {\pi }}\beta \Delta \sigma )^{m}}}\int _{a_{0}}^{a_{c}}{\frac {da}{({\sqrt {a}})^{m}}},}$

by integrating the above expression for ${\displaystyle m\neq 2}$ and ${\displaystyle m=2}$ cases, the total number of load cycles ${\displaystyle N_{f}}$ are given by

${\displaystyle {\begin{aligned}N_{f}&={\frac {2}{(m-2)C({\sqrt {\pi }}\beta \Delta \sigma )^{m}}}{\Bigg [}{\frac {1}{(a_{0})^{\frac {m-2}{2}}}}-{\frac {1}{(a_{c})^{\frac {m-2}{2}}}}{\Bigg ]},\qquad m\neq 2,\\N_{f}&={\frac {1}{\pi C(\beta \Delta \sigma )^{2}}}\ln {\frac {a_{c}}{a_{0}}},\qquad m=2.\end{aligned}}}$

Now, for ${\displaystyle m>2}$ and critical crack size to be very large in comparison to the initial crack size ${\displaystyle {\big (}a_{c}>>a_{0}{\big )}}$ will give

${\displaystyle N_{f}={\frac {2}{(m-2)C({\sqrt {\pi }}\Delta \sigma \beta )^{m}}}(a_{0})^{\frac {2-m}{2}}.}$

The above analytical expressions for the total number of load cycles to fracture ${\displaystyle {\big (}N_{f}{\big )}}$ are obtained by assuming ${\displaystyle Y={\text{constant}}}$. For the cases, where ${\displaystyle \beta }$ is dependent on the crack size such as the Single Edge Notch Tension (SENT), Center Cracked Tension (CCT) geometries, numerical integration can be used to compute ${\displaystyle N_{f}}$.

For ${\displaystyle R<0.7,}$ crack closure phenomenon has an effect on the crack growth rate and we can invoke Walker equation to compute the fatigue life of a specimen before it reaches the critical crack size ${\displaystyle a_{c}}$ as

${\displaystyle {\begin{aligned}{da \over dN}&=C{\bigg (}{\frac {\Delta K}{(1-R)^{1-\gamma }}}{\bigg )}^{m}={\frac {C}{(1-R)^{m(1-\gamma )}}}{\bigg (}\beta \Delta \sigma {\sqrt {\pi a}}{\bigg )}^{m},\\\Rightarrow N_{f}&={\frac {(1-R)^{m(1-\gamma )}}{({\sqrt {\pi }}\Delta \sigma )^{m}}}\int _{a_{0}}^{a_{c}}{\frac {da}{(C{\sqrt {a}}\beta )^{m}}}.\end{aligned}}}$

Figure 3: Schematic representation of fatigue life prediction process[28]

This scheme is useful when ${\displaystyle \beta }$ is dependent on the crack size ${\displaystyle a}$. The initial crack size is considered to be ${\displaystyle a_{0}}$. The stress intensity factor at the current crack size ${\displaystyle a}$ is computed using the maximum applied stress as

${\displaystyle {\begin{aligned}K_{\text{max}}&=\beta \sigma _{\text{max}}{\sqrt {\pi a}}.\end{aligned}}}$
If ${\displaystyle K_{\text{max}}}$ is less than the fracture toughness ${\displaystyle K_{\text{Ic}}}$, the crack has not reached its critical size ${\displaystyle a_{c}}$ and the simulation is continued with the current crack size to calculate the alternating stress intensity as

${\displaystyle \Delta K=\beta \Delta \sigma {\sqrt {\pi a}}.}$

Now, by substituting the stress intensity factor in Paris–Erdogan equation, the increment in the crack size ${\displaystyle \Delta a}$ is computed as

${\displaystyle \Delta a=C(\Delta K)^{m}\Delta N,}$

where ${\displaystyle \Delta N}$ is cycle step size. The new crack size becomes

${\displaystyle a_{i+1}=a_{i}+\Delta a,}$

where index ${\displaystyle i}$ refers to the current iteration step. The new crack size is used to calculate the stress intensity at maximum applied stress for the next iteration. This iterative process is continued until

${\displaystyle K_{\text{max}}\geq K_{\text{Ic}}.}$

Once this failure criterion is met, the simulation is stopped.

The schematic representation of the fatigue life prediction process is shown in figure 3.

Figure 4: Geometrical representation of Single Edge Notch Tension test specimen

The stress intensity factor in a SENT specimen (see, figure 4) under fatigue crack growth is given by[5]

${\displaystyle {\begin{aligned}K_{I}&=\beta \sigma {\sqrt {\pi a}}=\sigma {\sqrt {\pi a}}{\Bigg [}0.265{\bigg [}1-{\frac {a}{W}}{\bigg ]}^{4}+{\frac {0.857+0.265{\frac {a}{W}}}{{\big [}1-{\frac {a}{W}}{\big ]}^{\frac {3}{2}}}}{\Bigg ]},\\\Delta K_{I}&=K_{\text{max}}-K_{\text{min}}=\beta \Delta \sigma {\sqrt {\pi a}}.\end{aligned}}}$

The following parameters are considered for the calculation

${\displaystyle a_{0}=5}$ mm, ${\displaystyle W=100}$ mm, ${\displaystyle h=200}$ mm, ${\displaystyle K_{\text{Ic}}=30{\text{ MPa}}{\sqrt {\text{m}}}}$, ${\displaystyle R={\frac {K_{\text{min}}}{K_{\text{max}}}}=0.7}$,

${\displaystyle \Delta \sigma =20}$MPa,${\displaystyle C=4.6774\times 10^{-11}{\frac {\text{m}}{\text{cycle}}}{\frac {1}{({\text{MPa}}{\sqrt {\text{m}}})^{m}}}}$, ${\displaystyle m=3.874}$.

The critical crack length, ${\displaystyle a=a_{c}}$, can be computed when ${\displaystyle K_{\text{max}}=K_{\text{Ic}}}$ as

${\displaystyle a_{c}={\frac {1}{\pi }}{\Bigg (}{\frac {0.45}{\beta }}{\Bigg )}^{2}.}$

By solving the above equation, the critical crack length is obtained as ${\displaystyle a_{c}=26.7{\text{mm}}}$.

Now, invoking the Paris–Erdogan equation gives

${\displaystyle N_{f}={\frac {1}{C(\Delta \sigma )^{m}({\sqrt {\pi }})^{m}}}\int _{a_{0}}^{a_{c}}{\frac {da}{a^{\frac {m}{2}}{\Bigg [}0.265{\bigg [}1-{\frac {a}{W}}{\bigg ]}^{4}+{\frac {0.857+0.265{\frac {a}{W}}}{{\big [}1-{\frac {a}{W}}{\big ]}^{\frac {3}{2}}}}{\Bigg ]}^{m}}}}$

By numerical integration of the above expression, the total number of load cycles to failure is obtained as ${\displaystyle N_{f}=1.2085\times 10^{6}{\text{ cycles}}}$.