Dynamic Problems of Mode Ⅱ Cracks in 2D Octagonal Quasicrystals

MA Qing; WANG Guixia; LI Lianhe

doi:10.21656/1000-0887.380272

Volume 39 Issue 10

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MA Qing, WANG Guixia, LI Lianhe. Dynamic Problems of Mode Ⅱ Cracks in 2D Octagonal Quasicrystals[J]. Applied Mathematics and Mechanics, 2018, 39(10): 1180-1188. doi: 10.21656/1000-0887.380272

Citation:

MA Qing, WANG Guixia, LI Lianhe. Dynamic Problems of Mode Ⅱ Cracks in 2D Octagonal Quasicrystals[J]. Applied Mathematics and Mechanics, 2018, 39(10): 1180-1188. doi: 10.21656/1000-0887.380272

Citation:

MA Qing, WANG Guixia, LI Lianhe. Dynamic Problems of Mode Ⅱ Cracks in 2D Octagonal Quasicrystals[J]. Applied Mathematics and Mechanics, 2018, 39(10): 1180-1188. doi: 10.21656/1000-0887.380272

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Dynamic Problems of Mode Ⅱ Cracks in 2D Octagonal Quasicrystals

doi: 10.21656/1000-0887.380272

College of Mathematics Science, Inner Mongolia Normal University, Hohhot 010022, P.R.China

Funds: The National Key R&D Program of China(2017YFC1405600)；The National Natural Science Foundation of China(11462020；11361039)

Received Date: 2017-10-27
Rev Recd Date: 2018-02-26
Publish Date: 2018-10-01

Abstract

Abstract

Based on the elasto-hydrodynamic model, the dynamic problems of mode Ⅱ cracks in octagonal 2D quasicrystals were investigated with the finite difference scheme. The dynamic responses of stress intensity factors to different loading periods and different specimen sizes were analyzed, respectively. Then the influence of different phonon-phason coupling elastic constants on the displacement component of the phason field was demonstrated. The results indicate that, the stress intensity factor increases with the loading period, while the curve approaches the curve under the step load. The wider the specimen size is, the longer the time will be for the stress wave to reach the crack tip, and the smaller the stress intensity factor will be. The crack loading is different from the board loading, for the change of the stress intensity factor under the former is greater than that under the latter. With the increasing phonon-phason coupling constant, the displacement component of the phason field rises. Because of the influence of the phonon and phonon-phason coupling effect, the displacement component of the phason field equals zero when the phonon-phason coupling constant is zero.
- elasto-hydrodynamic model,
- finite difference method,
- mode Ⅱ crack,
- stress intensity factor

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References(22)

References

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