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AIDJEX Bulletin #40 - Polar Science Center - University of Washington

AIDJEX Bulletin #40 - Polar Science Center - University of Washington

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considered and it might alter the results, perhaps by eliminating all charac-<br />

teristic directions. Thus, we do not consider seriously the cases where<br />

0 n/2 for which DI < 0. We do note that for the assumed yield surface<br />

(Figure 4) we require a confining stress to obtain uniaxial contracting.<br />

In Figure 5c a combined stretching <strong>of</strong> shearing and closing is presented.<br />

In this case, the shearing exceeds the closing and DII/DI = -6. The stress<br />

state is similar to that which induces uniaxial contracting, but the differ-<br />

ences are large enough to change the characteristics. For 8 = 2~13 we have<br />

two real characteristic directions oriented symmetrically about principal<br />

directions at angles k27.4 degrees.<br />

In Figure 5d the case <strong>of</strong> pure shearing is sketched. Since no area<br />

changes occur we have 8 = T/2 and two characteristic directions <strong>of</strong> ?45<br />

degrees.<br />

This is the classical result that occurs with a von Mises yield<br />

surface. In our case it occurs only at the point <strong>of</strong> maximum shear stress.<br />

We can imagine velocity discontinuities across these lines associated with<br />

shearing across leads.<br />

In Figure 5e we present the case <strong>of</strong> shearing and opening. We see that<br />

for the particular yield surface chosen this stretching requires a uniaxial<br />

stress state. The stretching is similar to that in Figure 5c but the sign<br />

<strong>of</strong> DI has been changed from negative to positive.<br />

also similar but the pressure 01 is different.<br />

The stress deviator is<br />

We again have two character-<br />

istic directions but in this case they are oriented at 262.6 degrees from<br />

the larger principal stretching. Thus, although this characteristic pattern<br />

could be obtained by rotating the material 90 degrees as in Figure 5c, the<br />

stress and stretching are not the same. Therefore, we must exercise care<br />

when attempting to determine what state exists. Again, in this case we can<br />

visualize leads that are shearing and opening along characteristic directions.<br />

Finally, in Figure 5f we present uniaxial opening. For the yield sur-<br />

face presented the material may support a small amount <strong>of</strong> tensile stress,<br />

but there is nothing critical about this property. One real characteristic<br />

occurs at 90 degrees, which is orthogonal to the direction <strong>of</strong> maximum open-<br />

ing.<br />

It is easy to visualize leads opening along this characteristic<br />

direction for the uniaxial opening case.<br />

135

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