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Definition of Crack Tip Opening Displacement

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Definition of Crack Tip Opening Displacement

There are two common definitions of the crack tip opening displacement (CTOD):




1. The opening displacement of the original crack tip.

2. The displacement at the intersection of a 90 vertex with the crack flanks.

These two definitions are equivalent if the crack blunts in a semicircle.

CTOD in Specimen

The crack tip opening displacement (CTOD) of a crack at the edge of a three-point bending specimen is shown below:

where CTODm is the measured crack tip opening displacement, usually near the edge of the specimen for ease of access, CTOD is the real crack tip opening displacement, a is the length of the crack, and b is the width of the rest of the specimen. Please note that the figure is for illustration purpose only and not to scale. From simple geometry of two similar triangles:

where rhois a dimensionless rotational factor used to locate the center of the hinge.

For simplicity, let's assume that the center of the hinge locates at the center of b, i.e., rho~ 1/2. The CTOD then becomes

The above hinge model may not be accurate when the displacement is mostly elastic. A more accurate approach is to separate the CTOD into an elastic part and a plastic part:

where S ysis the small scale yielding stress and m is a dimensionless constant that depends on the material properties and the stress states.

Relationship between J and CTOD

Consider a linear elastic body containing a crack, the J integral and the crack tip opening displacement (CTOD) have the following relationship

J vs. CTOD in LEFM

where S ysand m are defined in the previous section. For plane stress and nonhardening materials, m = 1. Hence, for a through crack in an infinite plate subjected to a remote tensile stress sigma(Mode I), the crack tip opening displacement is

Shih, C. F., 1981, took a step further and showed that a unique relationship exists between J and CTOD beyond the validity limits of LEFM. He introduced the 90 intercept definition of CTOD, as illustrated below.

The displacement field is



The CTOD is evaluated from ux and uy at r = r* and theta = pi:

Since

The CTOD becomes

Definition of J Integral

Consider a nonlinear elastic body containing a crack,

the J integral is defined as

J Integral

where is the strain energy density, is the traction vector, Gammais an arbitrary contour around the tip of the crack, n is the unit vector normal to Gamma; Stress, Strain, and u are the stress, strain, and displacement field, respectively.

Rice, J. R., 1968, showed that the J integral is a path-independent line integral and it represents the strain energy release rate of nonlinear elastic materials

J

where Pi=U-Wis the potential energy, the strain energy U stored in the body minus the work W done by external forces and A is the crack area.

The dimension of J is

J vs. Gand K

For linear elastic materials, the J integral J is in fact the strain energy release rate, G, and both are related to the stress intensity factor K in the following fashion:






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