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Γ-CONVERGENCE FOR A FAULT MODEL WITH SLIP-WEAKENING FRICTION AND PERIODIC BARRIERS
We consider a three-dimensional elastic body with a plane fault under a slip-weakening friction. The fault has ∊-periodically distributed holes, called (smallscale) barriers. This problem arises in the modeling of the earthquake nucleation on a large-scale fault. In each ∊-square of the ∊-lattice on...
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Published in: | Quarterly of applied mathematics 2005-12, Vol.63 (4), p.747-778 |
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Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We consider a three-dimensional elastic body with a plane fault under a slip-weakening friction. The fault has ∊-periodically distributed holes, called (smallscale) barriers. This problem arises in the modeling of the earthquake nucleation on a large-scale fault. In each ∊-square of the ∊-lattice on the fault plane, the friction contact is considered outside an open set T∊ (small-scale barrier) of size r∊ < ∊, compactly inclosed in the ∊-square. The solution of each ∊-problem is found as local minima for an energy with both bulk and surface terms. The first eigenvalue of a symmetric and compact operator K∊ provides information about the stability of the solution. Using Γ-convergence techniques, we study the asymptotic behavior as ∊ tends to 0 for the friction contact problem. Depending on the values of c =: lim∊→0T→/∊² we obtain different limit problems. The asymptotic analysis for the associated spectral problem is performed using G convergence for the sequence of operators K→. The limits of the eigenvalue sequences and the associated eigenvectors are eigenvalues and respectively eigenvectors of a limit operator. From the physical point of view our result can be interpreted as follows: i) if the barriers are too large (i. e. c = ∞), then the fault is locked (no slip), ii) if c > 0, then the fault behaves as a fault under a slip-dependent friction. The slip weakening rate of the equivalent fault is smaller than the undisturbed fault. Since the limit slip-weakening rate may be negative, a slip-hardening effect can also be expected. iii) if the barriers are too small (i.e. c = 0), then the presence of the barriers does not affect the friction law on the limit fault. |
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ISSN: | 0033-569X 1552-4485 |
DOI: | 10.1090/S0033-569X-05-00981-7 |