Cleanup

Project.toml

@@ -5,7 +5,6 @@ version = "1.0.0-DEV"
 
 [deps]
 AbstractTrees = "1520ce14-60c1-5f80-bbc7-55ef81b5835c"
-AllocCheck = "9b6a8646-10ed-4001-bbdc-1d2f46dfbb1a"
 BlockArrays = "8e7c35d0-a365-5155-bbbb-fb81a777f24e"
 DrWatson = "634d3b9d-ee7a-5ddf-bec9-22491ea816e1"
 ForwardDiff = "f6369f11-7733-5829-9624-2563aa707210"
@@ -18,10 +17,8 @@ IterativeSolvers = "42fd0dbc-a981-5370-80f2-aaf504508153"
 JSON = "682c06a0-de6a-54ab-a142-c8b1cf79cde6"
 LinearAlgebra = "37e2e46d-f89d-539d-b4ee-838fcccc9c8e"
 PartitionedArrays = "5a9dfac6-5c52-46f7-8278-5e2210713be9"
-Plots = "91a5bcdd-55d7-5caf-9e0b-520d859cae80"
 Profile = "9abbd945-dff8-562f-b5e8-e1ebf5ef1b79"
 ProfileView = "c46f51b8-102a-5cf2-8d2c-8597cb0e0da7"
 Roots = "f2b01f46-fcfa-551c-844a-d8ac1e96c665"
 StaticArrays = "90137ffa-7385-5640-81b9-e52037218182"
-TimerOutputs = "a759f4b9-e2f1-59dc-863e-4aeb61b1ea8f"
 WriteVTK = "64499a7a-5c06-52f2-abe2-ccb03c286192"

src/ComputationalModels/ComputationalModels.jl

@@ -1,5 +1,4 @@
 module ComputationalModels
-using DrWatson
 using HyperFEM.PhysicalModels
 using HyperFEM.Solvers
 
@@ -13,7 +12,7 @@ import Gridap: solve!
 
 using BlockArrays
 using GridapPETSc, GridapPETSc.PETSC
-using GridapPETSc: PetscScalar, PetscInt, PETSC,  @check_error_code
+using GridapPETSc: PetscScalar, PetscInt, PETSC
 
 using GridapDistributed
 using GridapDistributed: DistributedDiscreteModel, DistributedTriangulation,
@@ -22,21 +21,18 @@ using GridapDistributed: DistributedDiscreteModel, DistributedTriangulation,
   DistributedMultiFieldFEBasis, BlockPMatrix, BlockPVector, change_ghost
 
 using PartitionedArrays
-using PartitionedArrays: getany, tuple_of_arrays, matching_ghost_indices
+using PartitionedArrays: getany
 
 using GridapSolvers
 using GridapSolvers.LinearSolvers, GridapSolvers.NonlinearSolvers, GridapSolvers.BlockSolvers
 using GridapSolvers.SolverInterfaces: SolverVerboseLevel, SOLVER_VERBOSE_NONE, SOLVER_VERBOSE_LOW, SOLVER_VERBOSE_HIGH
-# using GridapSolvers.SolverInterfaces: init!, update!, finalize!
 using GridapSolvers.SolverInterfaces: finished, print_message, converged
 
 using LinearAlgebra
 using WriteVTK
 
 using GridapGmsh 
 using GridapGmsh: GmshDiscreteModel
-using GridapGmsh:@check_if_loaded
-# using Gmsh: Gmsh, gmsh
 
 
 include("BoundaryConditions.jl")
@@ -71,7 +67,6 @@ export StaticNonlinearModel
 export DynamicNonlinearModel
 export StaticLinearModel
 export solve!
-# export evaluate!
 export dirichlet_preconditioning!
 export get_state
 export get_measure

src/ComputationalModels/GridapExtras.jl

@@ -1,32 +1,5 @@
 using Gridap.CellData
 
-# function Gridap.CellData.evaluate!(cache,f::CellState,x::CellPoint) 
-#   f.values
-# end
-
-# function GridapGmsh.GmshDiscreteModel(mshfile; terminal=1, renumber=true)
-
-#   @check_if_loaded
-#   if !isfile(mshfile)
-#     error("Msh file not found: $mshfile")
-#   end
-
-#   gmsh.initialize()
-#   gmsh.option.setNumber("General.Terminal", terminal)
-#   gmsh.option.setNumber("Mesh.SaveAll", 1)
-#   gmsh.option.setNumber("Mesh.MedImportGroupsOfNodes", 1)
-#   gmsh.open(mshfile)
-#   renumber && gmsh.model.mesh.renumberNodes()
-#   renumber && gmsh.model.mesh.renumberElements()
-#   model = GmshDiscreteModel(gmsh)
-#   gmsh.finalize()
-#   model
-# end
-
-# function Gridap.CellData.evaluate!(cache,f::CellState,x::CellPoint) 
-#   f.values
-# end
-
 
 function repeat_spaces(nblocks::Integer,U0::FESpace,V0::FESpace)
   U = MultiFieldFESpace([U0 for i in 1:nblocks];style=BlockMultiFieldStyle())

src/PhysicalModels/PhysicalModels.jl

@@ -3,8 +3,8 @@ module PhysicalModels
 using Gridap
 using Gridap.CellData
 using Gridap.Helpers
-using DrWatson
 
+using DrWatson
 using ForwardDiff
 using LinearAlgebra
 using ..TensorAlgebra

src/WeakForms/WeakForms.jl

@@ -422,48 +422,4 @@ function jacobian(physicalmodel::ThermoElectroMech_PINNs, kine::NTuple{2,Kinemat
 end
 
 
-
-
-
-
-
-# ===================
-# Time Integrators+
-# ===================
-
-# abstract type TimeIntegrator end
-
-# struct MidPoint <: TimeIntegrator
-# res::A
-# jac::B
-# params::A    
-# function MidPoint(res_,jac_, dΩ; αray = 0.4, ρ = 1.0, Δt = 5.0)
-
-#     res(u, v) =  mass_term(u, v, 2.0 * ρ / Δt^2, dΩ)-
-#                  0.5 * res_(u, v)+
-#                  0.5 * res_(u⁻, v)+
-
-
-#     res(t, u⁻, vh) = (u, v) -> mass_term(u, v, 2.0 * ρ / Δt^2, dΩ) -
-#     mass_term(u⁻, v, 2.0 * ρ / Δt^2, dΩ) -
-#     mass_term(vh, v, 2.0 * ρ / Δt, dΩ) +
-#     0.5 * res_(physmodel, u, v, dΩ) +
-#     0.5 * res_(physmodel, u⁻, v, dΩ) +
-#     mass_term(u, v, αray * ρ / Δt, dΩ) -
-#     mass_term(u⁻, v, αray * ρ / Δt, dΩ)
-
-
-#     params=(; αray = αray, ρ = ρ, Δt = Δt)
-#     A,B,C= typeof(res), typeof(jac), typeof(params)
-#     new{A,B,C}(res,jac,params)
-# end
-# end
-
-# Midpoint Integrator 
-# -------------------
-# function residual(, (u, φ), (v, vφ), dΩ)
-
-# end
-
-
 end