The three fracture modes.
Fracture mechanics is the field of mechanics concerned with the study of the propagation of cracks in materials. It uses methods of analytical solid mechanics to calculate the driving force on a crack and those of experimental solid mechanics to characterize the material's resistance to fracture.
In modern materials science, fracture mechanics is an important tool in improving the mechanical performance of mechanical components. It applies the physics of stress and strain, in particular the theories of elasticity and plasticity, to the microscopic crystallographic defects found in real materials in order to predict the macroscopic mechanical failure of bodies. Fractography is widely used with fracture mechanics to understand the causes of failures and also verify the theoretical failure predictions with real life failures. The prediction of crack growth is at the heart of the damage tolerance discipline.
There are three ways of applying a force to enable a crack to propagate:

Mode I fracture – Opening mode (a tensile stress normal to the plane of the crack),

Mode II fracture – Sliding mode (a shear stress acting parallel to the plane of the crack and perpendicular to the crack front), and

Mode III fracture – Tearing mode (a shear stress acting parallel to the plane of the crack and parallel to the crack front).
Contents

Linear elastic fracture mechanics 1

Griffith's criterion 1.1

Irwin's modification 1.2

Stress intensity factor 1.3

Strain energy release 1.4

Small scale yielding 1.5

Fracture toughness tests 1.6

Limitations 1.7

Elastic–plastic fracture mechanics 2

CTOD 2.1

Rcurve 2.2

Jintegral 2.3

Cohesive zone models 2.4

Transition flaw size 2.5

Cracktip constraint under large scale yielding 3

JQ Theory 3.1

Tterm effects 3.2

Engineering applications 4

Short summary 5

Appendix: mathematical relations 6

Griffith's criterion 6.1

Irwin's modifications 6.2

Elasticity and plasticity 6.3

Applications of fracture mechanics 7

See also 8

References 9

Notes 9.1

Bibliography 9.2

Further reading 10

External links 11
Linear elastic fracture mechanics
Griffith's criterion
An edge crack (flaw) of length a in a material
Fracture mechanics was developed during World War I by English aeronautical engineer, A. A. Griffith, to explain the failure of brittle materials.^{[1]} Griffith's work was motivated by two contradictory facts:

The stress needed to fracture bulk glass is around 100 MPa (15,000 psi).

The theoretical stress needed for breaking atomic bonds is approximately 10,000 MPa (1,500,000 psi).
A theory was needed to reconcile these conflicting observations. Also, experiments on glass fibers that Griffith himself conducted suggested that the fracture stress increases as the fiber diameter decreases. Hence the uniaxial tensile strength, which had been used extensively to predict material failure before Griffith, could not be a specimenindependent material property. Griffith suggested that the low fracture strength observed in experiments, as well as the sizedependence of strength, was due to the presence of microscopic flaws in the bulk material.
To verify the flaw hypothesis, Griffith introduced an artificial flaw in his experimental glass specimens. The artificial flaw was in the form of a surface crack which was much larger than other flaws in a specimen. The experiments showed that the product of the square root of the flaw length (a) and the stress at fracture (σ_{f}) was nearly constant, which is expressed by the equation:

\sigma_f\sqrt{a} \approx C
An explanation of this relation in terms of linear elasticity theory is problematic. Linear elasticity theory predicts that stress (and hence the strain) at the tip of a sharp flaw in a linear elastic material is infinite. To avoid that problem, Griffith developed a thermodynamic approach to explain the relation that he observed.
The growth of a crack requires the creation of two new surfaces and hence an increase in the surface energy. Griffith found an expression for the constant C in terms of the surface energy of the crack by solving the elasticity problem of a finite crack in an elastic plate. Briefly, the approach was:

Compute the potential energy stored in a perfect specimen under a uniaxial tensile load.

Fix the boundary so that the applied load does no work and then introduce a crack into the specimen. The crack relaxes the stress and hence reduces the elastic energy near the crack faces. On the other hand, the crack increases the total surface energy of the specimen.

Compute the change in the free energy (surface energy − elastic energy) as a function of the crack length. Failure occurs when the free energy attains a peak value at a critical crack length, beyond which the free energy decreases by increasing the crack length, i.e. by causing fracture. Using this procedure, Griffith found that

C = \sqrt{\cfrac{2E\gamma}{\pi}}
where E is the Young's modulus of the material and γ is the surface energy density of the material. Assuming E = 62 GPa and γ = 1 J/m^{2} gives excellent agreement of Griffith's predicted fracture stress with experimental results for glass.
Irwin's modification
The plastic zone around a crack tip in a ductile material
Griffith's work was largely ignored by the engineering community until the early 1950s. The reasons for this appear to be (a) in the actual structural materials the level of energy needed to cause fracture is orders of magnitude higher than the corresponding surface energy, and (b) in structural materials there are always some inelastic deformations around the crack front that would make the assumption of linear elastic medium with infinite stresses at the crack tip highly unrealistic. ^{[2]}
Griffith's theory provides excellent agreement with experimental data for brittle materials such as glass. For ductile materials such as steel, though the relation \sigma_y\sqrt{a} = C still holds, the surface energy (γ) predicted by Griffith's theory is usually unrealistically high. A group working under G. R. Irwin^{[3]} at the U.S. Naval Research Laboratory (NRL) during World War II realized that plasticity must play a significant role in the fracture of ductile materials.
In ductile materials (and even in materials that appear to be brittle^{[4]}), a plastic zone develops at the tip of the crack. As the applied load increases, the plastic zone increases in size until the crack grows and the material behind the crack tip unloads. The plastic loading and unloading cycle near the crack tip leads to the dissipation of energy as heat. Hence, a dissipative term has to be added to the energy balance relation devised by Griffith for brittle materials. In physical terms, additional energy is needed for crack growth in ductile materials when compared to brittle materials.
Irwin's strategy was to partition the energy into two parts:

the stored elastic strain energy which is released as a crack grows. This is the thermodynamic driving force for fracture.

the dissipated energy which includes plastic dissipation and the surface energy (and any other dissipative forces that may be at work). The dissipated energy provides the thermodynamic resistance to fracture. Then the total energy is

G = 2\gamma + G_p
where γ is the surface energy and G_{p} is the plastic dissipation (and dissipation from other sources) per unit area of crack growth.
The modified version of Griffith's energy criterion can then be written as

\sigma_f\sqrt{a} = \sqrt{\cfrac{E~G}{\pi}}.
For brittle materials such as glass, the surface energy term dominates and G \approx 2\gamma = 2 \,\, J/m^2. For ductile materials such as steel, the plastic dissipation term dominates and G \approx G_p = 1000 \,\, J/m^2. For polymers close to the glass transition temperature, we have intermediate values of G \approx 21000 \,\, J/m^2.
Stress intensity factor
Another significant achievement of Irwin and his colleagues was to find a method of calculating the amount of energy available for fracture in terms of the asymptotic stress and displacement fields around a crack front in a linear elastic solid.^{[3]} This asymptotic expression for the stress field around a crack tip is

\sigma_{ij} \approx \left(\cfrac{K}{\sqrt{2\pi r}}\right)~f_{ij}(\theta)
where σ_{ij} are the Cauchy stresses, r is the distance from the crack tip, θ is the angle with respect to the plane of the crack, and f_{ij} are functions that depend on the crack geometry and loading conditions. Irwin called the quantity K the stress intensity factor. Since the quantity f_{ij} is dimensionless, the stress intensity factor can be expressed in units of \text{MPa}\sqrt{\text{m}}.
When a rigid line inclusion is considered, a similar asymptotic expression for the stress fields is obtained.
Strain energy release
Irwin was the first to observe that if the size of the plastic zone around a crack is small compared to the size of the crack, the energy required to grow the crack will not be critically dependent on the state of stress at the crack tip.^{[2]} In other words, a purely elastic solution may be used to calculate the amount of energy available for fracture.
The energy release rate for crack growth or strain energy release rate may then be calculated as the change in elastic strain energy per unit area of crack growth, i.e.,

G := \left[\cfrac{\partial U}{\partial a}\right]_P = \left[\cfrac{\partial U}{\partial a}\right]_u
where U is the elastic energy of the system and a is the crack length. Either the load P or the displacement u can be kept fixed while evaluating the above expressions.
Irwin showed that for a mode I crack (opening mode) the strain energy release rate and the stress intensity factor are related by:

G = G_I = \begin{cases} \cfrac{K_I^2}{E} & \text{plane stress} \\ \cfrac{(1\nu^2) K_I^2}{E} & \text{plane strain} \end{cases}
where E is the Young's modulus, ν is Poisson's ratio, and K_{I} is the stress intensity factor in mode I. Irwin also showed that the strain energy release rate of a planar crack in a linear elastic body can be expressed in terms of the mode I, mode II (sliding mode), and mode III (tearing mode) stress intensity factors for the most general loading conditions.
Next, Irwin adopted the additional assumption that the size and shape of the energy dissipation zone remains approximately constant during brittle fracture. This assumption suggests that the energy needed to create a unit fracture surface is a constant that depends only on the material. This new material property was given the name fracture toughness and designated G_{Ic}. Today, it is the critical stress intensity factor K_{Ic}, found in the plane strain condition, which is accepted as the defining property in linear elastic fracture mechanics.
Small scale yielding
When a macroscopic loading is applied to a structure with a crack, the stress near the vicinity of the crack approaches ∞ as r→0, where r is the distance from the crack tip. As the magnitude of the stress in a material is bounded by the yield stress, there exists a region near the crack tip, of size r_{p}, in which the material has deformed plastically. The maximum size of this plastic zone can be estimated from the stress intensity factor K_{C} and the yield stress σ_{Y}; and can be expressed as

r_p = \frac{K_{C}^2}{\sigma_Y^2}.
In this region, the equations of linear elasticity are not valid. Therefore, for linear elastic fracture mechanics to be applicable, 2.5 r_{p} should be much smaller than the relevant dimensions, such as the length, thickness and width of the structure. This condition, in which the plastic deformation of the structure is confined to a very small region near the crack tip, is commonly referred to as small scale yielding.
Fracture toughness tests
Limitations
But a problem arose for the NRL researchers because naval materials, e.g., shipplate steel, are not perfectly elastic but undergo significant plastic deformation at the tip of a crack. One basic assumption in Irwin's linear elastic fracture mechanics is small scale yielding, the condition that the size of the plastic zone is small compared to the crack length. However, this assumption is quite restrictive for certain types of failure in structural steels though such steels can be prone to brittle fracture, which has led to a number of catastrophic failures.
Linearelastic fracture mechanics is of limited practical use for structural steels and Fracture toughness testing can be expensive.
Elastic–plastic fracture mechanics
Most engineering materials show some nonlinear elastic and inelastic behavior under operating conditions that involve large loads. In such materials the assumptions of linear elastic fracture mechanics may not hold, that is,

the plastic zone at a crack tip may have a size of the same order of magnitude as the crack size

the size and shape of the plastic zone may change as the applied load is increased and also as the crack length increases.
Therefore, a more general theory of crack growth is needed for elasticplastic materials that can account for:

the local conditions for initial crack growth which include the nucleation, growth, and coalescence of voids or decohesion at a crack tip.

a global energy balance criterion for further crack growth and unstable fracture.
CTOD
Historically, the first parameter for the determination of fracture toughness in the elastoplastic was the crack tip opening displacement (CTOD) or "opening at the apex of the crack" indicated. This parameter was determined by Wells during the studies of structural steels which, due to the high toughness could not be characterized with the linear elastic fracture mechanics. He noted that, before it happened the fracture, the walls of the crack were leaving and that the crack tip, after fracture, acute to rounded off is due to plastic deformation. In addition, the rounding of the apex was more pronounced in steels with superior toughness.
There are a number of alternative definitions of CTOD. The two most common definitions, CTOD is the displacement at the original crack tip and the 90 degree intercept. The latter definition was suggested by Rice and is commonly used to infer CTOD in finite element measurements. Note that these two definitions are equivalent if the crack blunts in a semicircle.
Most laboratory measurements of CTOD have been made on edgecracked specimens loaded in threepoint bending. Early experiments used a flat paddleshaped gage that was inserted into the crack; as the crack opened, the paddle gage rotated, and an electronic signal was sent to an xy plotter. This method was inaccurate, however, because it was difficult to reach the crack tip with the paddle gage. Today, the displacement V at the crack mouth is measured, and the CTOD is inferred by assuming the specimen halves are rigid and rotate about a hinge point.
Rcurve
An early attempt in the direction of elasticplastic fracture mechanics was Irwin's crack extension resistance curve, Crack growth resistance curve or Rcurve. This curve acknowledges the fact that the resistance to fracture increases with growing crack size in elasticplastic materials. The Rcurve is a plot of the total energy dissipation rate as a function of the crack size and can be used to examine the processes of slow stable crack growth and unstable fracture. However, the Rcurve was not widely used in applications until the early 1970s. The main reasons appear to be that the Rcurve depends on the geometry of the specimen and the crack driving force may be difficult to calculate.^{[2]}
Jintegral
In the mid1960s James R. Rice (then at Brown University) and G. P. Cherepanov independently developed a new toughness measure to describe the case where there is sufficient cracktip deformation that the part no longer obeys the linearelastic approximation. Rice's analysis, which assumes nonlinear elastic (or monotonic deformation theory plastic) deformation ahead of the crack tip, is designated the J integral.^{[5]} This analysis is limited to situations where plastic deformation at the crack tip does not extend to the furthest edge of the loaded part. It also demands that the assumed nonlinear elastic behavior of the material is a reasonable approximation in shape and magnitude to the real material's load response. The elasticplastic failure parameter is designated J_{Ic} and is conventionally converted to K_{Ic} using Equation (3.1) of the Appendix to this article. Also note that the J integral approach reduces to the Griffith theory for linearelastic behavior.
The mathematical definition of Jintegral is as follows:

J= \int_\Gamma( w \,dy  T_i \frac{\partial u_i}{\partial x}\,ds) \quad \text{with} \quad w=\int^{\varepsilon_{ij}}_0 \sigma_{ij} \,d\varepsilon_{ij}
where

\Gamma is an arbitrary path clockwise around the apex of the crack,

w is the density of strain energy,

T_i are the components of the vectors of traction,

u_i the components of the displacement vectors,

ds and an incremental length along the path \Gamma, an

\sigma_{ij} and \varepsilon_{ij} are the stress and strain tensors.
Cohesive zone models
When a significant region around a crack tip has undergone plastic deformation, other approaches can be used to determine the possibility of further crack extension and the direction of crack growth and branching. A simple technique that is easily incorporated into numerical calculations is the cohesive zone model method which is based on concepts proposed independently by Barenblatt^{[6]} and Dugdale^{[7]} in the early 1960s. The relationship between the DugdaleBarenblatt models and Griffith's theory was first discussed by Willis in 1967.^{[8]} The equivalence of the two approaches in the context of brittle fracture was shown by Rice in 1968.^{[5]} Interest in cohesive zone modeling of fracture has been reignited since 2000 following the pioneering work on dynamic fracture by Xu and Needleman,^{[9]} and Camacho and Ortiz.^{[10]}
Transition flaw size
Failure stress as a function of crack size
Let a material have a yield strength \sigma_Y and a fracture toughness in mode I K_{IC}. Based on fracture mechanics, the material will fail at stress \sigma_{fail}=K_{IC}/\sqrt{\pi a}. Based on plasticity, the material will yield when \sigma_{fail}=\sigma_Y. These curves intersect when a=K_{IC}^2/\pi\sigma_Y^2. This value of a is called as transition flaw size a_t., and depends on the material properties of the structure. When the a , the failure is governed by plastic yielding, and when a>a_t the failure is governed by fracture mechanics. The value of a_t for engineering alloys is 100 mm and for ceramics is 0.001 mm. If we assume that manufacturing processes can give rise to flaws in the order of micrometers, then, it can be seen that ceramics are more likely to fail by fracture, whereas engineering alloys would fail by plastic deformation.
Cracktip constraint under large scale yielding
Under smallscale yielding conditions, a single parameter (e.g., K, J, or CTOD) characterizes cracktip conditions and can be used as a geometryindependent fracture criterion. Singleparameter fracture mechanics breaks down in the presence of excessive plasticity, and the fracture toughness depends on the size and geometry of the test specimen. The theories used for large scale yielding is not very standardized. The following theories/ approaches are commonly used among researchers in this field
JQ Theory
By using FEM, one can establish a parameter Q to modify the stress field for a better solution when the plastic zone is growing. The new stress field is: \sigma_{ij}=(\sigma_{ij})+Q*\delta_{ij}*\sigma_{yield} where \delta_{ij}=1 for i=j and 0 if not. Q usually takes values from 3 to +2. A negative value greatly changes the geometry of the plastic zone.
The JQM theory includes another parameter, the mismatch parameter, which is used for welds to make up for the change in toughness of the weld metal (WM), base metal (BM) and heat affected zone (HAZ). This value is interpreted to the formula in a similar way as the Qparameter, and the two are usually assumed to be independent of each other.
Tterm effects
As an alternative to JQ theory, a parameter T can be used. This only changes the normal stress in the xdirection (and the zdirection in the case of plane strain). T does not require the use of FEM, but is derived from constraint. It can be argued that T is limited to LEFM, but as the plastic zone change due to T never reaches the actual crack surface (except on the tip), its validity holds true not only under small scale yielding. The parameter T also significantly influences on the fracture initiation in brittle materials using maximum tangential strain fracture criterion, as found by the researchers at Texas A & M University.^{[11]} It is found that both parameter T and Poisson's ratio of the material play important roles in prediction of the crack propagation angle and the mixed mode fracture toughness of the materials.
Engineering applications
The following information is needed for a fracture mechanics prediction of failure:

Applied load

Residual stress

Size and shape of the part

Size, shape, location, and orientation of the crack
Usually not all of this information is available and conservative assumptions have to be made.
Occasionally postmortem fracturemechanics analyses are carried out. In the absence of an extreme overload, the causes are either insufficient toughness (K_{Ic}) or an excessively large crack that was not detected during routine inspection.
Short summary
Arising from the manufacturing process, interior and surface flaws are found in all metal structures. Not all such flaws are unstable under service conditions. Fracture mechanics is the analysis of flaws to discover those that are safe (that is, do not grow) and those that are liable to propagate as cracks and so cause failure of the flawed structure. Ensuring safe operation of structure despite these inherent flaws is achieved through damage tolerance analysis. Fracture mechanics as a subject for critical study has barely been around for a century and thus is relatively new. There is a high demand for engineers with fracture mechanics expertise—particularly in this day and age where engineering failure is considered 'shocking' amongst the general public.
Appendix: mathematical relations
Griffith's criterion
For the simple case of a thin rectangular plate with a crack perpendicular to the load Griffith’s theory becomes:

G = \frac{\pi \sigma^2 a}{E}\, (1.1)
where G is the strain energy release rate, \sigma is the applied stress, a is half the crack length, and E is the Young’s modulus, which for the case of plane strain should be divided by the plate stiffness factor (1ν^2). The strain energy release rate can otherwise be understood as: the rate at which energy is absorbed by growth of the crack.
However, we also have that:

G_c = \frac{\pi \sigma_f^2 a}{E}\, (1.2)
If G ≥ G_c, this is the criterion for which the crack will begin to propagate.
Irwin's modifications
Eventually a modification of Griffith’s solids theory emerged from this work; a term called stress intensity replaced strain energy release rate and a term called fracture toughness replaced surface weakness energy. Both of these terms are simply related to the energy terms that Griffith used:

K_I = \sigma \sqrt{\pi a}\, (2.1)
and

K_c = \sqrt{E G_c}\, (for plane stress) (2.2)

K_c = \sqrt{\frac{E G_c}{1  \nu^2}}\, (for plane strain) (2.3)
where K_{I} is the stress intensity, K_{c} the fracture toughness, and \nu is Poisson’s ratio. It is important to recognize the fact that fracture parameter K_{c} has different values when measured under plane stress and plane strain
Fracture occurs when K_I \geq K_c. For the special case of plane strain deformation, K_c becomes K_{Ic} and is considered a material property. The subscript I arises because of the different ways of loading a material to enable a crack to propagate. It refers to socalled "mode I" loading as opposed to mode II or III:
We must note that the expression for K_I in equation 2.1 will be different for geometries other than the centercracked infinite plate, as discussed in the article on the stress intensity factor. Consequently, it is necessary to introduce a dimensionless correction factor, Y, in order to characterize the geometry. We thus have:

K_I = Y \sigma \sqrt{\pi a}\, (2.4)
where Y is a function of the crack length and width of sheet given by:

Y \left ( \frac{a}{W} \right ) = \sqrt{\sec\left ( \frac{\pi a}{W} \right )}\, (2.5)
for a sheet of finite width W containing a throughthickness crack of length 2a, or

Y \left ( \frac{a}{W} \right ) = 1.12  \frac{0.41}{\sqrt \pi} \frac{a}{W} + \frac{18.7}{\sqrt \pi} \left ( \frac{a}{W} \right )^2  \cdots\, (2.6)
for a sheet of finite width W containing a throughthickness edge crack of length a
Elasticity and plasticity
Since engineers became accustomed to using K_{Ic} to characterise fracture toughness, a relation has been used to reduce J_{Ic} to it:

K_{Ic} = \sqrt{E^* J_{Ic}}\, where E^* = E for plane stress and E^* = \frac{E}{1  \nu^2} for plane strain (3.1)
The remainder of the mathematics employed in this approach is interesting, but is probably better summarised in external pages due to its complex nature.
Applications of fracture mechanics
The design process for a component consists of choosing the appropriate geometry, the necessary material strength as per the loading conditions (either cyclic or constant loading), the temperature of usage and structural analysis (Testing and FEM analysis), so that it does not fail under load. The methodologies followed in design criteria traditionally pick up the conventional materials based on standard data and as per the loading conditions proportioning the geometry of the components on basis of analysis. This method is not applicable for some new innovation like usage of new material in design. Another method followed is that as per the loading conditions, static analysis is done for the structure taking into account the forces acting on each component, material strength and geometry. The material strength is chosen keeping in mind the factor of safety, i.e. the ultimate stress (where it fails) is much higher than maximum stress in the component. The general assumptions in the design criteria are: lack of discontinuities, no defects or cracks in the material, and even in the presence of discontinuities the material is assumed to have sufficient ductility to yield locally so that redistribution of stress at discontinuities can occur. Investigations of failed components proved that crack growth started because of such discontinuities.
Fracture mechanics follows one of two design principles: either failsafe or safelife. In fail safe mode, even if a component fails, the entire structure is not at risk (failure of redundant members). According to the safe life principle throughout the life, no component of the structure may fail. Fracture mechanics estimated the maximum crack that a material can withstand before it fails through analysis taking into consideration the overall dimensions of the structure, the stress value where crack initiation takes place, notch toughness value (ability of a material to absorb energy in the presence of a crack for crack propagation), the behavior of materials under the action of stresses by finding out the stress intensity factor (K), fatigue crack growth and stress corrosion crack growth. As in basic solid mechanics analysis, stresses in the component should be lower than the yield stress; application of the same principle is means that the stress intensity factor should be less than the critical stress intensity factor. Major applications of fracture mechanics design are material selection, effect of defects, failure analysis and control/monitoring of components. Fracture analysis includes the usage of mathematical models such as linear elastic fracture mechanics (LEFM), crack opening displacement (COD) and Jintegral approaches by using finite element analysis (FEM).
The relationship used for estimating stress intensity factor is

K =c \sigma \sqrt{a}
where K is the critical fracture toughness value, c a constant that depends on crack and specimen dimensions, σ the applied stress, and a the flaw size.
The above relation is very general and as per the shape of the crack, relations available in standard data books or course books are to be used, any general crack can be approximated to standard shapes used in writing the relations.
For a given material the value of K is dependent on stresses acting and flaw size. Flaw size decreases as the stress increases. Thus a design engineer can dictate the life of a component by choosing appropriate values of K, a and σ. Even there are other parameters that estimate the life of a component like working temperature, loading rate (fatigue), residual stress and stress concentration. The higher the K value, the higher is the resistance to crack growth, and the material can resist higher stresses. Designers try to decrease the defects in the component arising in casting or manufacturing processes by following good fabrication processes and inspection, and estimate notchtoughness values of materials using methods like charpy Vnotch impact test, or drop weight tests. In many investigations it was proved that the material failed at a very much lower than the critical stress intensity factor because of defects in the material or micro cracks. Analysis proved that for any component there are two phases for crack development, i.e. crack initiation and second phase crack growth until failure. Of the two, the first phase covers a larger percentage of fatigue life, and under very large high cycle loading conditions second phase is instantaneous.
The factor (K/σ)² is used for estimating design of component because it estimates crack size, more the value better the resistance to the forces(Stress). But how large this factor has to be is decided by considering type of the structure, frequency of inspection, access to inspection, design life of the structure, consequences of failure, probability of over load, methods of fabrication, required quality, material cost in addition to the results obtained by fracture mechanics analysis.
See also
References
Notes

^ .

^ ^{a} ^{b} ^{c} E. Erdogan (2000) Fracture Mechanics, International Journal of Solids and Structures, 37, pp. 171–183.

^ ^{a} ^{b} Irwin G (1957), Analysis of stresses and strains near the end of a crack traversing a plate, Journal of Applied Mechanics 24, 361–364.

^ Orowan, E., 1948. Fracture and strength of solids. Reports on Progress in Physics XII, 185–232.

^ ^{a} ^{b} .

^ Barenblatt, G. I. (1962), "The mathematical theory of equilibrium cracks in brittle fracture", Advances in applied mechanics 7: 55–129,

^ Dugdale, D. S. (1960), "Yielding of steel sheets containing slits", Journal of the Mechanics and Physics of Solids 8 (2): 100–104,

^ Willis, J. R. (1967), "A comparison of the fracture criteria of Griffith and Barenblatt", Journal of the Mechanics and Physics of Solids 15 (3): 151–162, .

^ Xu, X.P. and Needleman, A. (1994), "Numerical simulations of fast crack growth in brittle solids", Journal of the Mechanics and Physics of Solids 42 (9): 1397–1434,

^ Camacho, G. T. and Ortiz, M. (1996), "Computational modelling of impact damage in brittle materials", International Journal of Solids and Structures 33 (2022): 2899–2938,

^ Mirsayar, M. M., Mixed mode fracture analysis using extended maximum tangential strain criterion, "Materials & Design," 2015, doi:10.1016/j.matdes.2015.07.135.
Bibliography

C. P. Buckley, "Material Failure", Lecture Notes (2005), University of Oxford.

T. L. Anderson, "Fracture Mechanics: Fundamentals and Applications" (1995) CRC Press.
Further reading

Davidge, R.W., Mechanical Behavior of Ceramics, Cambridge Solid State Science Series, (1979)

Demaid, Adrian, Fail Safe, Open University (2004)

Green, D., An Introduction to the Mechanical Properties of Ceramics, Cambridge Solid State Science Series, Eds. Clarke, D.R., Suresh, S., Ward, I.M. (1998)

Lawn, B.R., Fracture of Brittle Solids, Cambridge Solid State Science Series, 2nd Edn. (1993)

Farahmand, B., Bockrath, G., and Glassco, J. (1997) Fatigue and Fracture Mechanics of HighRisk Parts, Chapman & Hall.

Chen, X., Mai, Y.W., Fracture Mechanics of Electromagnetic Materials: Nonlinear Field Theory and Applications, Imperial College Press, (2012)

Fracture mechanics fundamentals and applications by Anderson.

Chapter 10 – Strength of Elastomers, A.N. Gent, W.V. Mars, In: James E. Mark, Burak Erman and Mike Roland, Editor(s), The Science and Technology of Rubber (Fourth Edition), Academic Press, Boston, 2013, Pages 473516, ISBN 9780123945846, 10.1016/B9780123945846.000108
External links

Fracture Mechanics on eFunda site

Fracture Mechanics by Prof. Alan Zehnder, Cornell University

Fracture Mechanics for Engineers

Nonlinear Fracture Mechanics Notes by Prof. John Hutchinson, Harvard University

Notes on Fracture of Thin Films and Multilayers by Prof. John Hutchinson, Harvard University

Fracture Mechanics by Prof. Piet Schreurs, TU Eindhoven, Netherlands

Fracturemechanics.org by Dr. Bob McGinty, Mercer University

Fracture mechanics course notes by Prof. Rui Huang, Univ. of Texas

Application of Fracture Mechanics on keytometals.com
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