Mercurial > repos > public > sbplib_julia
diff src/SbpOperators/volumeops/derivatives/second_derivative.jl @ 1395:bdcdbd4ea9cd feature/boundary_conditions
Merge with default. Comment out broken tests for boundary_conditions at sat
author | Vidar Stiernström <vidar.stiernstrom@it.uu.se> |
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date | Wed, 26 Jul 2023 21:35:50 +0200 |
parents | 08f06bfacd5c |
children |
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--- a/src/SbpOperators/volumeops/derivatives/second_derivative.jl Tue Feb 07 21:55:07 2023 +0100 +++ b/src/SbpOperators/volumeops/derivatives/second_derivative.jl Wed Jul 26 21:35:50 2023 +0200 @@ -1,46 +1,37 @@ """ - second_derivative(grid::EquidistantGrid, inner_stencil, closure_stencils, direction) + second_derivative(g::EquidistantGrid, stencil_set, direction) -Creates the second-derivative operator `D2` as a `LazyTensor` - -`D2` approximates the second-derivative d²/dξ² on `grid` along the coordinate dimension specified by -`direction`, using the stencil `inner_stencil` in the interior and a set of stencils `closure_stencils` -for the points in the closure regions. +Creates the second derivative operator `D2` as a `LazyTensor` -On a one-dimensional `grid`, `D2` is a `VolumeOperator`. On a multi-dimensional `grid`, `D2` is the outer product of the -one-dimensional operator with the `IdentityTensor`s in orthogonal coordinate dirrections. +`D2` approximates the second-derivative d²/dξ² on `g` along the coordinate +dimension specified by `direction`. -See also: [`volume_operator`](@ref). +See also: [`VolumeOperator`](@ref), [`LazyTensors.inflate`](@ref). """ -function second_derivative(grid::EquidistantGrid, inner_stencil, closure_stencils, direction) - h_inv = inverse_spacing(grid)[direction] - return SbpOperators.volume_operator(grid, scale(inner_stencil,h_inv^2), scale.(closure_stencils,h_inv^2), even, direction) +function second_derivative(g::TensorGrid, stencil_set, direction) + D₂ = second_derivative(g.grids[direction], stencil_set) + return LazyTensors.inflate(D₂, size(g), direction) end - """ - second_derivative(grid, inner_stencil, closure_stencils) + second_derivative(g::EquidistantGrid, stencil_set::::StencilSet) -Creates a `second_derivative` operator on a 1D `grid` given `inner_stencil` and `closure_stencils`. +The second derivative operator on an `EquidistantGrid`. +Uses the `D2` stencil in `stencil_set`. """ -second_derivative(grid::EquidistantGrid{1}, inner_stencil::Stencil, closure_stencils) = second_derivative(grid, inner_stencil, closure_stencils,1) - +function second_derivative(g::EquidistantGrid, stencil_set::StencilSet) + inner_stencil = parse_stencil(stencil_set["D2"]["inner_stencil"]) + closure_stencils = parse_stencil.(stencil_set["D2"]["closure_stencils"]) + return second_derivative(g, inner_stencil, closure_stencils) +end """ - second_derivative(grid, stencil_set, direction) + second_derivative(g::EquidistantGrid, inner_stencil::Stencil, closure_stencils) -Creates a `second_derivative` operator on `grid` along coordinate dimension `direction` given a `stencil_set`. +The second derivative operator on an `EquidistantGrid`, given `inner_stencil` and +`closure_stencils`. """ -function second_derivative(grid::EquidistantGrid, stencil_set::StencilSet, direction) - inner_stencil = parse_stencil(stencil_set["D2"]["inner_stencil"]) - closure_stencils = parse_stencil.(stencil_set["D2"]["closure_stencils"]) - second_derivative(grid,inner_stencil,closure_stencils,direction); +function second_derivative(g::EquidistantGrid, inner_stencil::Stencil, closure_stencils) + h⁻¹ = inverse_spacing(g) + return VolumeOperator(g, scale(inner_stencil,h⁻¹^2), scale.(closure_stencils,h⁻¹^2), even) end - - -""" - second_derivative(grid, stencil_set) - -Creates a `second_derivative` operator on a 1D `grid` given a `stencil_set`. -""" -second_derivative(grid::EquidistantGrid{1}, stencil_set::StencilSet) = second_derivative(grid, stencil_set, 1) \ No newline at end of file