2001
DOI: 10.1785/0120000244
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Accuracy of the Explicit Planar Free-Surface Boundary Condition Implemented in a Fourth-Order Staggered-Grid Velocity-Stress Finite-Difference Scheme

Abstract: We compute the accuracy of two implementations of the explicit planar free-surface boundary condition for 3D fourth-order velocity-stress staggered-grid finite differences, 1/2 grid apart vertically, in a uniform half-space. Due to the staggered grid, the closest distance between the free surface and some wave-field components for both implementations is 1/2-grid spacing. Overall, the differences in accuracy of the two implementations are small. When compared to a reflectivity solution computed at the staggere… Show more

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Cited by 67 publications
(32 citation statements)
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“…For the numerical examples in this paper, source functions are bandpassed between 1 and 20 Hz, and the time interval is 0.3 ms. Synthetic ambient noise is generated by staggered-grid finite-difference simulations of the isotropic elastic wave equation (Virieux 1986) with a free-surface boundary condition (Gottschämmer & Olsen 2001).…”
Section: Ambient-noise Simulationmentioning
confidence: 99%
“…For the numerical examples in this paper, source functions are bandpassed between 1 and 20 Hz, and the time interval is 0.3 ms. Synthetic ambient noise is generated by staggered-grid finite-difference simulations of the isotropic elastic wave equation (Virieux 1986) with a free-surface boundary condition (Gottschämmer & Olsen 2001).…”
Section: Ambient-noise Simulationmentioning
confidence: 99%
“…The free surface matches the top side of the FD grid and the stress is forced to zero on the free surface (Gottschamer & Olsen, 2001). Alternatively, the method of image can be used to implement the free surface along a virtual plane located half a grid interval above the topside of the FD grid (Virieux, 1986).…”
Section: Free Surfacementioning
confidence: 99%
“…The Q values in the 3D velocity-density model are based on Q relations validated against data for the Northridge earthquake . Perfectly matched layers (Marcinkovich and Olsen, 2003) were used to implement absorbing boundary conditions on the sides and bottom of the grid, and a zerostress free-surface boundary condition was used at the top (Gottschämmer and Olsen, 2001). The code has been extensively validated for a wide range of problems, from simple point-sources in a half-space to complex ruptures on dipping faults in 3D crustal models (Day et al, 2008).…”
Section: Broadband Simulations For the 1994mentioning
confidence: 99%