Difference between revisions of "Crack Settings"
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where R = K<sub>II</sub>/K<sub>I</sub>. The second term is negative or positive depending on K<sub>II</sub> being positive or negative. In the limit of K<sub>I</sub> to zero, cos θ = 1/3 for crack direction of -70.5 (or +70.5) degrees. This method requires K<sub>I</sub> and K<sub>II</sub> which can only be done for isotropic (and subclasses), mooney, heisotropic (and subclass), and viscoelastic. All use initial, low strain modulus to calculate stress intensity factors. | where R = K<sub>II</sub>/K<sub>I</sub>. The second term is negative or positive depending on K<sub>II</sub> being positive or negative. In the limit of K<sub>I</sub> to zero, cos θ = 1/3 for crack direction of -70.5 (or +70.5) degrees. This method requires K<sub>I</sub> and K<sub>II</sub> which can only be done for isotropic (and subclasses), mooney, heisotropic (and subclass), and viscoelastic. All use initial, low strain modulus to calculate stress intensity factors. | ||
Above is same as | |||
| |||
<math>\tan {\theta\over 2} = {1\over 4}\left({1\over R} \mp \sqrt{{1\over R^2} + 8}\right)</math> | |||
where negative of positive is determined by sign of K<sub>II</sub>. | |||
in cod hoop direction, the code uses the max energy release rate method, but assumes R = δ<sub>t</sub>/δ<sub>n</sub> or ratio of the sliding and opening crack opening displacements. This method can be used for any material. | in cod hoop direction, the code uses the max energy release rate method, but assumes R = δ<sub>t</sub>/δ<sub>n</sub> or ratio of the sliding and opening crack opening displacements. This method can be used for any material. |
Revision as of 16:56, 27 September 2013
This section needs writing. Below are some items that will be used or moved else where.
Commands (temp)
Scripted commands
AltPropagate ContactPosition Friction JContour ImperfectInterface MovePlane Propagate PropagateLength
In XML files
<Cracks> <Propagate criterion='1' direction='0' traction='0'/> <AltPropagate criterion='7' direction='4' traction='0'/> <PropagateLength>2.5</PropagateLength> <JContour type='1' size="2" terms="1"/> <Friction>0.3</Friction> <MovePlane type='avg' prevent='no'/> <ContactPosition>0.8</ContactPosition> </Cracks>
Crack Propagation Commands
In max energy release rate (or max hoop stress), the crack direction is at angle θ (which is ccw from self similar growth) and obeys
[math]\displaystyle{ \cos\theta = {3R^2 + \sqrt{1+8R^2} \over 1+9R^2} \quad {\rm and} \quad \sin\theta = \mp\sqrt{1-\cos^2\theta} = \mp\left | R(3\cos\theta - 1)\right| }[/math]
where R = KII/KI. The second term is negative or positive depending on KII being positive or negative. In the limit of KI to zero, cos θ = 1/3 for crack direction of -70.5 (or +70.5) degrees. This method requires KI and KII which can only be done for isotropic (and subclasses), mooney, heisotropic (and subclass), and viscoelastic. All use initial, low strain modulus to calculate stress intensity factors.
Above is same as
[math]\displaystyle{ \tan {\theta\over 2} = {1\over 4}\left({1\over R} \mp \sqrt{{1\over R^2} + 8}\right) }[/math]
where negative of positive is determined by sign of KII.
in cod hoop direction, the code uses the max energy release rate method, but assumes R = δt/δn or ratio of the sliding and opening crack opening displacements. This method can be used for any material.