Consider the crack problem shown for the anti-plane strain case with u = v = 0, w

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Consider the crack problem shown for the anti-plane strain case with u = v = 0, w = w(x,y). From Section 7.4, the governing equation for the unknown displacement component with zero body force was given by Laplace’s equation, which in polar coordinates reads.

7 aw 1 dw + r r dr 1 3 w ar  30 0

Use a separation of variables scheme with w = f (0), where is a parameter to be determined and f (0) is

Data from section 8.4.10

Consider the original wedge problem shown in Fig. 8.16 for the case where angle a is small and  is 2 - . This

0 B = 2-  X

while the identical conditions at 0=6=27- = 2 produce sin 2 (2  2) ^ 2 si -  sin 272C +[cos 2(2-2) - cos 2] =

Near the tip of the notch  0 and the stresses will be of order O(2), while the displacements are O(-1). At

Such relations play an important role in fracture mechanics by providing information on the nature of the

The remaining constants A and B are determined from the far-field boundary conditions. However, an important

Data from section 7.4

One additional plane theory of elasticity involves a formulation based on the existence of only out-of- plane

and written out in terms of the single displacement component, the equilibrium statement becomes Vw + F = 0or traction form: T = T(x,y) = tnx + t2ny (b) dw My 1.) the on dy =  w nx +. x on S (7.4.7) The solution to


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