Figure 2
The finite-difference model is decomposed into a set of discrete cells, indicated by the solid lines, each with uniform static sound speed c and ambient density ρo. The acoustic pressure and density perturbations are defined at the nodes at the centre of each cell, indicated by the filled circles. The horizontal particle velocity vx (triangles pointing right) and vertical particle velocity variables vz (triangles pointing up) nodes straddle the cell boundaries of the spatially staggered grid, shown in two dimensions.

The finite-difference model is decomposed into a set of discrete cells, indicated by the solid lines, each with uniform static sound speed c and ambient density ρo. The acoustic pressure and density perturbations are defined at the nodes at the centre of each cell, indicated by the filled circles. The horizontal particle velocity vx (triangles pointing right) and vertical particle velocity variables vz (triangles pointing up) nodes straddle the cell boundaries of the spatially staggered grid, shown in two dimensions.

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