Mercurial > repos > public > sbplib_julia
comparison src/SbpOperators/volumeops/laplace/laplace.jl @ 1673:f28c92ec843c refactor/grids/boundary_identifiers_1d
Address TODO in laplace.jl + minor fixes
| author | Vidar Stiernström <vidar.stiernstrom@gmail.com> |
|---|---|
| date | Sun, 07 Jul 2024 15:19:33 -0700 |
| parents | 1937be9502a7 |
| children | b5690ab5f0b8 |
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| 1672:3714a391545a | 1673:f28c92ec843c |
|---|---|
| 58 | 58 |
| 59 The operators required to construct the SAT for imposing a Dirichlet | 59 The operators required to construct the SAT for imposing a Dirichlet |
| 60 condition. `H_tuning` and `R_tuning` are used to specify the strength of the | 60 condition. `H_tuning` and `R_tuning` are used to specify the strength of the |
| 61 penalty. | 61 penalty. |
| 62 | 62 |
| 63 See also: [`sat`](@ref),[`DirichletCondition`](@ref), [`positivity_decomposition`](@ref). | 63 See also: [`sat`](@ref), [`DirichletCondition`](@ref), [`positivity_decomposition`](@ref). |
| 64 """ | 64 """ |
| 65 function sat_tensors(Δ::Laplace, g::Grid, bc::DirichletCondition; H_tuning = 1., R_tuning = 1.) | 65 function sat_tensors(Δ::Laplace, g::Grid, bc::DirichletCondition; H_tuning = 1., R_tuning = 1.) |
| 66 id = boundary(bc) | 66 id = boundary(bc) |
| 67 set = Δ.stencil_set | 67 set = Δ.stencil_set |
| 68 H⁻¹ = inverse_inner_product(g,set) | 68 H⁻¹ = inverse_inner_product(g,set) |
| 69 Hᵧ = inner_product(boundary_grid(g, id), set) | 69 Hᵧ = inner_product(boundary_grid(g, id), set) |
| 70 e = boundary_restriction(g, set, id) | 70 e = boundary_restriction(g, set, id) |
| 71 d = normal_derivative(g, set, id) | 71 d = normal_derivative(g, set, id) |
| 72 B = positivity_decomposition(Δ, g, bc; H_tuning, R_tuning) | 72 B = positivity_decomposition(Δ, g, boundary(bc); H_tuning, R_tuning) |
| 73 penalty_tensor = H⁻¹∘(d' - B*e')∘Hᵧ | 73 penalty_tensor = H⁻¹∘(d' - B*e')∘Hᵧ |
| 74 return penalty_tensor, e | 74 return penalty_tensor, e |
| 75 end | 75 end |
| 76 | 76 |
| 77 """ | 77 """ |
| 92 penalty_tensor = -H⁻¹∘e'∘Hᵧ | 92 penalty_tensor = -H⁻¹∘e'∘Hᵧ |
| 93 return penalty_tensor, d | 93 return penalty_tensor, d |
| 94 end | 94 end |
| 95 | 95 |
| 96 """ | 96 """ |
| 97 positivity_decomposition(Δ::Laplace, g::Grid, bc::DirichletCondition; H_tuning, R_tuning) | 97 positivity_decomposition(Δ::Laplace, g::Grid, b::BoundaryIdentifier; H_tuning, R_tuning) |
| 98 | 98 |
| 99 Constructs the scalar `B` such that `d' - 1/2*B*e'` is symmetric positive | 99 Constructs the scalar `B` such that `d' - 1/2*B*e'` is symmetric positive |
| 100 definite with respect to the boundary quadrature. Here `d` is the normal | 100 definite with respect to the boundary quadrature. Here `d` is the normal |
| 101 derivative and `e` is the boundary restriction operator. `B` can then be used | 101 derivative and `e` is the boundary restriction operator. `B` can then be used |
| 102 to form a symmetric and energy stable penalty for a Dirichlet condition. The | 102 to form a symmetric and energy stable penalty for a Dirichlet condition. The |
| 103 parameters `H_tuning` and `R_tuning` are used to specify the strength of the | 103 parameters `H_tuning` and `R_tuning` are used to specify the strength of the |
| 104 penalty and must be greater than 1. For details we refer to | 104 penalty and must be greater than 1. For details we refer to |
| 105 https://doi.org/10.1016/j.jcp.2020.109294 | 105 <https://doi.org/10.1016/j.jcp.2020.109294> |
| 106 """ | 106 """ |
| 107 function positivity_decomposition(Δ::Laplace, g::Grid, bc::DirichletCondition; H_tuning, R_tuning) | 107 function positivity_decomposition(Δ::Laplace, g::Grid, b::BoundaryIdentifier; H_tuning, R_tuning) |
| 108 @assert(H_tuning ≥ 1.) | 108 @assert(H_tuning ≥ 1.) |
| 109 @assert(R_tuning ≥ 1.) | 109 @assert(R_tuning ≥ 1.) |
| 110 Nτ_H, τ_R = positivity_limits(Δ,g,bc) | 110 Nτ_H, τ_R = positivity_limits(Δ,g,b) |
| 111 return H_tuning*Nτ_H + R_tuning*τ_R | 111 return H_tuning*Nτ_H + R_tuning*τ_R |
| 112 end | 112 end |
| 113 | 113 |
| 114 # TODO: We should consider implementing a proper BoundaryIdentifier for EquidistantGrid and then | 114 function positivity_limits(Δ::Laplace, g::EquidistantGrid, b::BoundaryIdentifier) |
| 115 # change bc::BoundaryCondition to id::BoundaryIdentifier | |
| 116 function positivity_limits(Δ::Laplace, g::EquidistantGrid, bc::DirichletCondition) | |
| 117 h = spacing(g) | 115 h = spacing(g) |
| 118 θ_H = parse_scalar(Δ.stencil_set["H"]["closure"][1]) | 116 θ_H = parse_scalar(Δ.stencil_set["H"]["closure"][1]) |
| 119 θ_R = parse_scalar(Δ.stencil_set["D2"]["positivity"]["theta_R"]) | 117 θ_R = parse_scalar(Δ.stencil_set["D2"]["positivity"]["theta_R"]) |
| 120 | 118 |
| 121 τ_H = 1/(h*θ_H) | 119 τ_H = one(eltype(Δ))/(h*θ_H) |
| 122 τ_R = 1/(h*θ_R) | 120 τ_R = one(eltype(Δ))/(h*θ_R) |
| 123 return τ_H, τ_R | 121 return τ_H, τ_R |
| 124 end | 122 end |
| 125 | 123 |
| 126 function positivity_limits(Δ::Laplace, g::TensorGrid, bc::DirichletCondition) | 124 function positivity_limits(Δ::Laplace, g::TensorGrid, b::BoundaryIdentifier) |
| 127 τ_H, τ_R = positivity_limits(Δ, g.grids[grid_id(boundary(bc))], bc) | 125 τ_H, τ_R = positivity_limits(Δ, g.grids[grid_id(b)], b) |
| 128 return τ_H*ndims(g), τ_R | 126 return τ_H*ndims(g), τ_R |
| 129 end | 127 end |
