An implicit staggered grid finite-difference elastic wave numerical simulation method and device
A staggered grid and finite difference technology, applied in the field of seismic wave exploration, can solve problems such as poor accuracy, achieve the effects of improving numerical solution accuracy, improving calculation efficiency, and reducing calculation time
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Embodiment 1
[0075] This embodiment provides an implicit staggered grid finite difference elastic wave numerical simulation method, Figure 4 is a flow chart of an implicit staggered grid finite difference elastic wave numerical simulation method according to an embodiment of the present invention, as shown in Figure 4 As shown, the method includes the following steps (step S401-step S405):
[0076] Step S401, based on the implicit staggered grid finite difference scheme (ie the above formula 2) and the plane wave theoretical formula (ie the above formula 5), the dispersion relation expression (ie the above formula 8) is obtained:
[0077] where, β=kh / 2, k is the wave number, h is the grid size, b is a constant, M is the order, a m are implicit staggered grid finite difference coefficients, m=1,2,...,M.
[0078] Step S402, performing a sampling approximation method on the dispersion relation expression to obtain a linear algebraic equation system.
[0079] Specifically: uniformly t...
Embodiment approach
[0087] In the first step, the implicit staggered grid finite difference coefficient a m and the constant b are substituted into the implicit staggered grid finite difference scheme to solve the spatial partial derivatives in the elastic wave equation;
[0088] This step specifically includes: the implicit staggered grid finite difference coefficient a m and the constant b are substituted into the implicit staggered grid finite difference scheme, and the implicit staggered grid finite difference scheme is applied to each grid point, and the difference equations on all grid points are simultaneously established (the implicit staggered grid finite difference equation is obtained through the above-mentioned implicit staggered grid finite-difference format conversion), and the tridiagonal matrix equation is obtained; the spatial partial derivatives in the elastic wave equation are obtained by solving the tridiagonal matrix equation.
[0089] In the second step, the spatial partial...
Embodiment 2
[0094] This embodiment introduces the complete flow of the implicit staggered grid finite-difference elastic wave numerical simulation method.
[0095] In a homogeneous isotropic medium, the two-dimensional elastic wave equation (Equation 1) is expressed as:
[0096]
[0097] Among them, t represents time, x and z represent space coordinates, (v x ,v z ) is the velocity vector, (τ xx ,τ zz ,τ xz ) is the stress tensor, ρ is the density, and λ and μ are the Lame constants. The time derivative term in the elastic wave equation (formula 1) (that is, the items on the left side of the equal sign in formula 1) is solved by the second-order difference scheme, and in order to improve the solution accuracy, the spatial derivative term (that is, the items on the right side of the equal sign in formula (1)) Solved by the implicit staggered-grid finite-difference scheme (Equation 2) described below.
[0098] The spatial first derivative of the function p(x) is expanded into an im...
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