Package evaluation to test HyperFEM on Julia 1.14.0-DEV.3081 (21a70e450d*) started at 2026-09-02T11:14:34.135 ################################################################################ # Set-up # Installing PkgEval dependencies (TestEnv)... Activating project at `~/.julia/environments/v1.14` Set-up completed after 33.08s ################################################################################ # Installation # Installing HyperFEM... Resolving package versions... Installed CommonWorldInvalidations ───────── v1.2.0 Installed Libuuid_jll ────────────────────── v2.42.0+0 Installed ChunkCodecLibZstd ──────────────── v1.0.0 Installed Bzip2_jll ──────────────────────── v1.0.9+0 Installed MKL_jll ────────────────────────── v2025.2.0+0 Installed gmsh_jll ───────────────────────── v4.13.1+0 Installed SIMDTypes ──────────────────────── v0.1.0 Installed NearestNeighbors ───────────────── v0.4.29 Installed Cairo_jll ──────────────────────── v1.18.7+0 Installed MPIABI_jll ─────────────────────── v1.0.0+0 Installed Xorg_libpciaccess_jll ──────────── v0.19.0+0 Installed CpuId ──────────────────────────── v0.3.1 Installed Xorg_libXinerama_jll ───────────── v1.1.7+0 Installed Fontconfig_jll ─────────────────── v2.17.1+0 Installed FileIO ─────────────────────────── v1.20.0 Installed ArgCheck ───────────────────────── v2.5.0 Installed OrderedCollections ─────────────── v2.0.1 Installed PartitionedArrays ──────────────── v0.3.5 Installed NaNMath ────────────────────────── v1.1.4 Installed Distances ──────────────────────── v0.10.12 Installed BSON ───────────────────────────── v0.3.9 Installed LinearElasticity_jll ───────────── v5.0.0+0 Installed StaticArrayInterface ───────────── v1.10.0 Installed OpenSpecFun_jll ────────────────── v0.5.6+0 Installed QuadGK ─────────────────────────── v2.11.3 Installed HDF5_jll ───────────────────────── v1.14.3+3 Installed ScopedValues ───────────────────── v1.6.2 Installed LLVMOpenMP_jll ─────────────────── v22.1.7+0 Installed Static ─────────────────────────── v1.4.6 Installed Xorg_libxcb_jll ────────────────── v1.17.1+0 Installed NLSolversBase ──────────────────── v7.10.0 Installed Preferences ────────────────────── v1.5.2 Installed IterativeSolvers ───────────────── v0.9.4 Installed Reexport ───────────────────────── v1.2.2 Installed ADTypes ────────────────────────── v1.24.0 Installed DataStructures ─────────────────── v0.19.6 Installed Inflate ────────────────────────── v0.1.5 Installed FillArrays ─────────────────────── v1.17.0 Installed DiffResults ────────────────────── v1.1.0 Installed libaec_jll ─────────────────────── v1.1.7+0 Installed ManualMemory ───────────────────── v0.1.8 Installed MacroTools ─────────────────────── v0.5.16 Installed AbstractTrees ──────────────────── v0.4.5 Installed ArnoldiMethod ──────────────────── v0.4.0 Installed oneTBB_jll ─────────────────────── v2022.3.0+0 Installed HyperFEM ───────────────────────── v0.0.6 Installed CodecZlib ──────────────────────── v0.7.9 Installed SCOTCH_jll ─────────────────────── v6.1.3+0 Installed Xorg_libXau_jll ────────────────── v1.0.13+0 Installed Xorg_libXfixes_jll ─────────────── v6.0.2+0 Installed IntelOpenMP_jll ────────────────── v2025.2.0+0 Installed ArrayInterface ─────────────────── v7.30.1 Installed CEnum ──────────────────────────── v0.5.0 Installed CommonSubexpressions ───────────── v0.3.1 Installed LayoutPointers ─────────────────── v0.1.17 Installed Expat_jll ──────────────────────── v2.8.3+0 Installed StructUtils ────────────────────── v2.8.5 Installed SimpleTraits ───────────────────── v0.9.6 Installed Libffi_jll ─────────────────────── v3.4.7+0 Installed Pixman_jll ─────────────────────── v0.46.4+0 Installed IrrationalConstants ────────────── v0.2.6 Installed libpng_jll ─────────────────────── v1.6.58+0 Installed ArrayLayouts ───────────────────── v1.12.2 Installed Hwloc_jll ──────────────────────── v2.14.0+0 Installed SparseMatricesCSR ──────────────── v0.6.12 Installed OpenMPI_jll ────────────────────── v4.1.9+0 Installed MMG_jll ────────────────────────── v5.6.0+0 Installed BlockArrays ────────────────────── v1.10.0 Installed ForwardDiff ────────────────────── v1.4.5 Installed WriteVTK ───────────────────────── v1.22.0 Installed Setfield ───────────────────────── v1.1.2 Installed CircularArrays ─────────────────── v1.5.0 Installed LightXML ───────────────────────── v0.9.3 Installed PkgVersion ─────────────────────── v0.3.3 Installed DocStringExtensions ────────────── v0.9.5 Installed DifferentiationInterface ───────── v0.7.21 Installed SimpleUnPack ───────────────────── v1.1.0 Installed PolynomialBases ────────────────── v0.4.28 Installed MPICH_jll ──────────────────────── v5.0.1+0 Installed MicrosoftMPI_jll ───────────────── v10.1.4+3 (no artifacts on this platform) Installed Xorg_libXft_jll ────────────────── v2.3.9+0 Installed BitTwiddlingConvenienceFunctions ─ v0.1.6 Installed OCCT_jll ───────────────────────── v7.7.2+0 Installed HashArrayMappedTries ───────────── v0.2.0 Installed Combinatorics ──────────────────── v1.1.0 Installed RecipesBase ────────────────────── v1.3.4 Installed StaticArrays ───────────────────── v1.9.19 Installed FastGaussQuadrature ────────────── v1.3.0 Installed FLTK_jll ───────────────────────── v1.3.8+0 Installed StaticArraysCore ───────────────── v1.4.4 Installed Libglvnd_jll ───────────────────── v1.7.1+1 Installed AbstractFFTs ───────────────────── v1.5.0 Installed SciMLPublic ────────────────────── v1.3.0 Installed GridapSolvers ──────────────────── v0.7.1 Installed Gridap ─────────────────────────── v0.19.11 Installed Glib_jll ───────────────────────── v2.88.3+0 Installed LogExpFunctions ────────────────── v1.0.1 Installed DiffRules ──────────────────────── v1.16.0 Installed Parsers ────────────────────────── v2.8.7 Installed JSON ───────────────────────────── v1.7.1 Installed Gamma ──────────────────────────── v1.2.0 Installed FiniteDiff ─────────────────────── v2.33.0 Installed UnsafeAtomics ──────────────────── v0.3.2 Installed Requires ───────────────────────── v1.3.1 Installed AutoHashEquals ─────────────────── v2.2.0 Installed ChunkCodecCore ─────────────────── v1.0.2 Installed ThreadingUtilities ─────────────── v0.5.6 Installed CloseOpenIntervals ─────────────── v0.1.13 Installed JpegTurbo_jll ──────────────────── v3.2.0+1 Installed Xorg_libXdmcp_jll ──────────────── v1.1.6+0 Installed JLLWrappers ────────────────────── v1.8.0 Installed GLU_jll ────────────────────────── v9.0.1+0 Installed Polyester ──────────────────────── v0.7.19 Installed Xorg_xtrans_jll ────────────────── v1.6.0+0 Installed Graphs ─────────────────────────── v1.14.0 Installed Adapt ──────────────────────────── v4.7.0 Installed MPI ────────────────────────────── v0.20.27 Installed JLD2 ───────────────────────────── v0.6.6 Installed Libmount_jll ───────────────────── v2.42.0+0 Installed ConstructionBase ───────────────── v1.6.0 Installed Statistics ─────────────────────── v1.11.4 Installed Xorg_libX11_jll ────────────────── v1.8.13+0 Installed Compat ─────────────────────────── v4.18.1 Installed TranscodingStreams ─────────────── v0.11.3 Installed StrideArraysCore ───────────────── v0.5.9 Installed PrecompileTools ────────────────── v1.3.4 Installed ChunkCodecLibZlib ──────────────── v1.1.0 Installed StatsAPI ───────────────────────── v1.8.0 Installed Atomix ─────────────────────────── v1.1.3 Installed CPUSummary ─────────────────────── v0.2.7 Installed GettextRuntime_jll ─────────────── v0.22.4+0 Installed OffsetArrays ───────────────────── v1.17.0 Installed Metis ──────────────────────────── v1.5.0 Installed NLsolve ────────────────────────── v4.5.1 Installed SpecialFunctions ───────────────── v2.9.0 Installed Xorg_libXrender_jll ────────────── v0.9.12+0 Installed IfElse ─────────────────────────── v0.1.1 Installed XML2_jll ───────────────────────── v2.13.9+0 Installed FreeType2_jll ──────────────────── v2.14.3+1 Installed MPIPreferences ─────────────────── v0.1.12 Installed FFTW ───────────────────────────── v1.10.0 Installed FFTW_jll ───────────────────────── v3.3.12+0 Installed GridapDistributed ──────────────── v0.4.13 Installed Libiconv_jll ───────────────────── v1.18.0+0 Installed VTKBase ────────────────────────── v1.0.1 Installed MPItrampoline_jll ──────────────── v5.5.6+0 Installed METIS_jll ──────────────────────── v5.1.3+0 Installed Xorg_libXext_jll ───────────────── v1.3.8+0 Installed LineSearches ───────────────────── v7.5.1 Installed PolyesterWeave ─────────────────── v0.2.2 Installed GridapGmsh ─────────────────────── v0.7.4 Installing 42 artifacts Installed artifact libaec 31.0 KiB Installed artifact Xorg_libpciaccess 23.4 KiB Installed artifact Xorg_libXau 25.8 KiB Installed artifact Xorg_libXft 177.3 KiB Installed artifact METIS 393.1 KiB Installed artifact FreeType2 1.2 MiB Installed artifact Cairo 1.5 MiB Installed artifact GettextRuntime 345.6 KiB Installed artifact HDF5 3.8 MiB Installed artifact XML2 2.0 MiB Installed artifact Fontconfig 443.8 KiB Installed artifact Xorg_xtrans 39.5 KiB Installed artifact OpenSpecFun 105.4 KiB Installed artifact MMG 981.7 KiB Installed artifact Hwloc 3.0 MiB Installed artifact Libiconv 1022.9 KiB Installed artifact Glib 4.2 MiB Installed artifact Expat 255.9 KiB Installed artifact JpegTurbo 713.4 KiB Installed artifact Xorg_libXdmcp 49.9 KiB Installed artifact Xorg_libXext 187.3 KiB Installed artifact Xorg_libXrender 174.0 KiB Installed artifact Xorg_libxcb 1.3 MiB Installed artifact Xorg_libXfixes 41.4 KiB Installed artifact Xorg_libXinerama 21.7 KiB Installed artifact MPICH 5.8 MiB Installed artifact Libuuid 1.9 MiB Installed artifact FLTK 1.3 MiB Installed artifact GLU 1.2 MiB Installed artifact Libffi 39.2 KiB Installed artifact LinearElasticity 257.2 KiB Installed artifact SCOTCH 357.1 KiB Installed artifact Libmount 3.4 MiB Installed artifact LLVMOpenMP 573.2 KiB Installed artifact Pixman 343.0 KiB Installed artifact Libglvnd 482.2 KiB Installed artifact Bzip2 152.8 KiB Installed artifact FFTW 1.8 MiB Installed artifact libpng 234.7 KiB Installed artifact Xorg_libX11 2.3 MiB Installed artifact gmsh 8.9 MiB Installed artifact OCCT 23.6 MiB Updating `~/.julia/environments/v1.14/Project.toml` [ddbf423a] + HyperFEM v0.0.6 Updating `~/.julia/environments/v1.14/Manifest.toml` [47edcb42] + ADTypes v1.24.0 [621f4979] + AbstractFFTs v1.5.0 [1520ce14] + AbstractTrees v0.4.5 [79e6a3ab] + Adapt v4.7.0 [dce04be8] + ArgCheck v2.5.0 [ec485272] + ArnoldiMethod v0.4.0 [4fba245c] + ArrayInterface v7.30.1 [4c555306] + ArrayLayouts v1.12.2 [a9b6321e] + Atomix v1.1.3 [15f4f7f2] + AutoHashEquals v2.2.0 [fbb218c0] + BSON v0.3.9 [62783981] + BitTwiddlingConvenienceFunctions v0.1.6 [8e7c35d0] + BlockArrays v1.10.0 [fa961155] + CEnum v0.5.0 [2a0fbf3d] + CPUSummary v0.2.7 [0b6fb165] + ChunkCodecCore v1.0.2 [4c0bbee4] + ChunkCodecLibZlib v1.1.0 [55437552] + ChunkCodecLibZstd v1.0.0 [7a955b69] + CircularArrays v1.5.0 [fb6a15b2] + CloseOpenIntervals v0.1.13 [944b1d66] + CodecZlib v0.7.9 [861a8166] + Combinatorics v1.1.0 [bbf7d656] + CommonSubexpressions v0.3.1 [f70d9fcc] + CommonWorldInvalidations v1.2.0 [34da2185] + Compat v4.18.1 [187b0558] + ConstructionBase v1.6.0 [adafc99b] + CpuId v0.3.1 [864edb3b] + DataStructures v0.19.6 [163ba53b] + DiffResults v1.1.0 [b552c78f] + DiffRules v1.16.0 [a0c0ee7d] + DifferentiationInterface v0.7.21 [b4f34e82] + Distances v0.10.12 [ffbed154] + DocStringExtensions v0.9.5 [7a1cc6ca] + FFTW v1.10.0 [442a2c76] + FastGaussQuadrature v1.3.0 [5789e2e9] + FileIO v1.20.0 [1a297f60] + FillArrays v1.17.0 [6a86dc24] + FiniteDiff v2.33.0 [f6369f11] + ForwardDiff v1.4.5 [a0844989] + Gamma v1.2.0 [86223c79] + Graphs v1.14.0 ⌅ [56d4f2e9] + Gridap v0.19.11 ⌃ [f9701e48] + GridapDistributed v0.4.13 [3025c34a] + GridapGmsh v0.7.4 [6d3209ee] + GridapSolvers v0.7.1 [076d061b] + HashArrayMappedTries v0.2.0 [ddbf423a] + HyperFEM v0.0.6 [615f187c] + IfElse v0.1.1 [d25df0c9] + Inflate v0.1.5 [92d709cd] + IrrationalConstants v0.2.6 [42fd0dbc] + IterativeSolvers v0.9.4 [033835bb] + JLD2 v0.6.6 [692b3bcd] + JLLWrappers v1.8.0 [682c06a0] + JSON v1.7.1 [10f19ff3] + LayoutPointers v0.1.17 [9c8b4983] + LightXML v0.9.3 ⌃ [d3d80556] + LineSearches v7.5.1 [2ab3a3ac] + LogExpFunctions v1.0.1 [da04e1cc] + MPI v0.20.27 [3da0fdf6] + MPIPreferences v0.1.12 [1914dd2f] + MacroTools v0.5.16 [d125e4d3] + ManualMemory v0.1.8 [2679e427] + Metis v1.5.0 ⌅ [d41bc354] + NLSolversBase v7.10.0 ⌅ [2774e3e8] + NLsolve v4.5.1 [77ba4419] + NaNMath v1.1.4 [b8a86587] + NearestNeighbors v0.4.29 [6fe1bfb0] + OffsetArrays v1.17.0 [bac558e1] + OrderedCollections v2.0.1 ⌅ [69de0a69] + Parsers v2.8.7 ⌅ [5a9dfac6] + PartitionedArrays v0.3.5 [eebad327] + PkgVersion v0.3.3 [f517fe37] + Polyester v0.7.19 [1d0040c9] + PolyesterWeave v0.2.2 [c74db56a] + PolynomialBases v0.4.28 [aea7be01] + PrecompileTools v1.3.4 [21216c6a] + Preferences v1.5.2 [1fd47b50] + QuadGK v2.11.3 [3cdcf5f2] + RecipesBase v1.3.4 [189a3867] + Reexport v1.2.2 [ae029012] + Requires v1.3.1 [94e857df] + SIMDTypes v0.1.0 [431bcebd] + SciMLPublic v1.3.0 [7e506255] + ScopedValues v1.6.2 [efcf1570] + Setfield v1.1.2 [699a6c99] + SimpleTraits v0.9.6 [ce78b400] + SimpleUnPack v1.1.0 [a0a7dd2c] + SparseMatricesCSR v0.6.12 [276daf66] + SpecialFunctions v2.9.0 [aedffcd0] + Static v1.4.6 [0d7ed370] + StaticArrayInterface v1.10.0 [90137ffa] + StaticArrays v1.9.19 [1e83bf80] + StaticArraysCore v1.4.4 [10745b16] + Statistics v1.11.4 [82ae8749] + StatsAPI v1.8.0 [7792a7ef] + StrideArraysCore v0.5.9 [ec057cc2] + StructUtils v2.8.5 [8290d209] + ThreadingUtilities v0.5.6 [3bb67fe8] + TranscodingStreams v0.11.3 [013be700] + UnsafeAtomics v0.3.2 [4004b06d] + VTKBase v1.0.1 [64499a7a] + WriteVTK v1.22.0 [6e34b625] + Bzip2_jll v1.0.9+0 [83423d85] + Cairo_jll v1.18.7+0 [2e619515] + Expat_jll v2.8.3+0 [f5851436] + FFTW_jll v3.3.12+0 [4fce6fc7] + FLTK_jll v1.3.8+0 [a3f928ae] + Fontconfig_jll v2.17.1+0 [d7e528f0] + FreeType2_jll v2.14.3+1 [bd17208b] + GLU_jll v9.0.1+0 ⌅ [b0724c58] + GettextRuntime_jll v0.22.4+0 [7746bdde] + Glib_jll v2.88.3+0 ⌅ [0234f1f7] + HDF5_jll v1.14.3+3 [e33a78d0] + Hwloc_jll v2.14.0+0 [1d5cc7b8] + IntelOpenMP_jll v2025.2.0+0 [aacddb02] + JpegTurbo_jll v3.2.0+1 [1d63c593] + LLVMOpenMP_jll v22.1.7+0 ⌅ [e9f186c6] + Libffi_jll v3.4.7+0 [7e76a0d4] + Libglvnd_jll v1.7.1+1 [94ce4f54] + Libiconv_jll v1.18.0+0 [4b2f31a3] + Libmount_jll v2.42.0+0 [38a345b3] + Libuuid_jll v2.42.0+0 [18c40d15] + LinearElasticity_jll v5.0.0+0 [d00139f3] + METIS_jll v5.1.3+0 [856f044c] + MKL_jll v2025.2.0+0 [86086c02] + MMG_jll v5.6.0+0 [b5ada748] + MPIABI_jll v1.0.0+0 [7cb0a576] + MPICH_jll v5.0.1+0 [f1f71cc9] + MPItrampoline_jll v5.5.6+0 [9237b28f] + MicrosoftMPI_jll v10.1.4+3 ⌅ [baad4e97] + OCCT_jll v7.7.2+0 ⌅ [fe0851c0] + OpenMPI_jll v4.1.9+0 [efe28fd5] + OpenSpecFun_jll v0.5.6+0 [30392449] + Pixman_jll v0.46.4+0 ⌅ [a8d0f55d] + SCOTCH_jll v6.1.3+0 ⌅ [02c8fc9c] + XML2_jll v2.13.9+0 [4f6342f7] + Xorg_libX11_jll v1.8.13+0 [0c0b7dd1] + Xorg_libXau_jll v1.0.13+0 [a3789734] + Xorg_libXdmcp_jll v1.1.6+0 [1082639a] + Xorg_libXext_jll v1.3.8+0 [d091e8ba] + Xorg_libXfixes_jll v6.0.2+0 [2c808117] + Xorg_libXft_jll v2.3.9+0 [d1454406] + Xorg_libXinerama_jll v1.1.7+0 [ea2f1a96] + Xorg_libXrender_jll v0.9.12+0 [a65dc6b1] + Xorg_libpciaccess_jll v0.19.0+0 [c7cfdc94] + Xorg_libxcb_jll v1.17.1+0 [c5fb5394] + Xorg_xtrans_jll v1.6.0+0 ⌃ [630162c2] + gmsh_jll v4.13.1+0 [477f73a3] + libaec_jll v1.1.7+0 [b53b4c65] + libpng_jll v1.6.58+0 [1317d2d5] + oneTBB_jll v2022.3.0+0 [0dad84c5] + ArgTools v1.2.0 [56f22d72] + Artifacts v1.11.0 [2a0f44e3] + Base64 v1.11.0 [ade2ca70] + Dates v1.11.0 [8ba89e20] + Distributed v1.12.0 [f43a241f] + Downloads v1.7.0 [7b1f6079] + FileWatching v1.11.0 [9fa8497b] + Future v1.11.0 [b77e0a4c] + InteractiveUtils v1.11.0 [ac6e5ff7] + JuliaSyntaxHighlighting v1.13.0 [4af54fe1] + LazyArtifacts v1.11.0 [b27032c2] + LibCURL v1.0.0 [76f85450] + LibGit2 v1.11.0 [8f399da3] + Libdl v1.11.0 [37e2e46d] + LinearAlgebra v1.14.0 [56ddb016] + Logging v1.11.0 [d6f4376e] + Markdown v1.11.0 [a63ad114] + Mmap v1.11.0 [ca575930] + NetworkOptions v1.3.0 [44cfe95a] + Pkg v1.14.0 [de0858da] + Printf v1.11.0 [9a3f8284] + Random v1.11.0 [ea8e919c] + SHA v1.13.0 [9e88b42a] + Serialization v1.11.0 [6462fe0b] + Sockets v1.11.0 [2f01184e] + SparseArrays v1.13.0 [f489334b] + StyledStrings v1.13.0 [4607b0f0] + SuiteSparse [fa267f1f] + TOML v1.0.3 [a4e569a6] + Tar v1.10.0 [8dfed614] + Test v1.11.0 [cf7118a7] + UUIDs v1.11.0 [4ec0a83e] + Unicode v1.11.0 [e66e0078] + CompilerSupportLibraries_jll v1.5.7+0 [781609d7] + GMP_jll v6.3.0+4 [deac9b47] + LibCURL_jll v8.21.0+0 [e37daf67] + LibGit2_jll v1.9.7+0 [29816b5a] + LibSSH2_jll v1.11.104+0 [14a3606d] + MozillaCACerts_jll v2026.8.13 [4536629a] + OpenBLAS_jll v0.3.34+0 [05823500] + OpenLibm_jll v0.8.7+0 [458c3c95] + OpenSSL_jll v3.5.8+0 [efcefdf7] + PCRE2_jll v10.47.0+0 [bea87d4a] + SuiteSparse_jll v7.10.1+0 [83775a58] + Zlib_jll v1.3.2+0 [3161d3a3] + Zstd_jll v1.5.7+1 [8e850b90] + libblastrampoline_jll v5.15.0+0 [8e850ede] + nghttp2_jll v1.70.0+0 [3f19e933] + p7zip_jll v17.8.2+0 Info Packages marked with ⌃ and ⌅ have new versions available. Those with ⌃ may be upgradable, but those with ⌅ are restricted by compatibility constraints from upgrading. To see why use `status --outdated -m` Building GridapGmsh → `~/.julia/scratchspaces/44cfe95a-1eb2-52ea-b672-e2afdf69b78f/56bcd88698c92c1bacbca36aa82844de776c646e/build.log` Installation completed after 120.71s ################################################################################ # Precompilation # Precompiling PkgEval dependencies... Precompiling project... 4.1 s ✓ TestEnv 1 dependency successfully precompiled in 4 seconds. 27 already precompiled. Precompiling package dependencies... Precompiling project... 3.5 s ✓ MacroTools 0.6 s ✓ Reexport 0.7 s ✓ ConstructionBase 1.9 s ✓ IrrationalConstants 0.5 s ✓ DataValueInterfaces 0.6 s ✓ StatsAPI 0.6 s ✓ CEnum 1.8 s ✓ Combinatorics 0.7 s ✓ Inflate 0.6 s ✓ ArgCheck 0.9 s ✓ TranscodingStreams 0.6 s ✓ LaTeXStrings 0.7 s ✓ ChunkCodecCore 0.8 s ✓ Statistics 0.7 s ✓ StaticArraysCore 0.5 s ✓ IfElse 0.6 s ✓ AutoHashEquals 0.6 s ✓ ManualMemory 0.7 s ✓ Adapt 0.6 s ✓ DataAPI 2.9 s ✓ UnsafeAtomics 0.7 s ✓ VTKBase 0.9 s ✓ AbstractTrees 0.5 s ✓ SimpleUnPack 0.8 s ✓ AbstractFFTs 2.0 s ✓ FillArrays 0.6 s ✓ ExprTools 0.9 s ✓ OrderedCollections 0.6 s ✓ HashArrayMappedTries 0.8 s ✓ DocStringExtensions 1.1 s ✓ BSON 1.3 s ✓ OffsetArrays 0.5 s ✓ SIMDTypes 0.5 s ✓ IteratorInterfaceExtensions 1.8 s ✓ Crayons 0.7 s ✓ NaNMath 0.7 s ✓ Requires 1.8 s ✓ StructUtils 1.4 s ✓ CpuId 0.8 s ✓ Compat 1.2 s ✓ Preferences 4.3 s ✓ PkgVersion 0.9 s ✓ CommonSubexpressions 2.1 s ✓ SimpleTraits 0.5 s ✓ ConstructionBase → ConstructionBaseLinearAlgebraExt 0.7 s ✓ CodecZlib 0.7 s ✓ ChunkCodecLibZlib 0.7 s ✓ ChunkCodecLibZstd 1.5 s ✓ Statistics → SparseArraysExt 1.2 s ✓ Distances 0.6 s ✓ DiffResults 1.1 s ✓ ThreadingUtilities 0.8 s ✓ ArrayInterface 1.4 s ✓ Adapt → AdaptSparseArraysExt 0.7 s ✓ Atomix 3.2 s ✓ AbstractFFTs → AbstractFFTsTestExt 1.8 s ✓ FillArrays → FillArraysSparseArraysExt 0.9 s ✓ FillArrays → FillArraysStatisticsExt 3.3 s ✓ DataStructures 0.6 s ✓ ScopedValues 1.1 s ✓ LogExpFunctions 0.6 s ✓ OffsetArrays → OffsetArraysAdaptExt 0.6 s ✓ CircularArrays 0.5 s ✓ TableTraits 7.9 s ✓ FileIO 0.8 s ✓ StructUtils → StructUtilsStaticArraysCoreExt 0.5 s ✓ Compat → CompatLinearAlgebraExt 1.2 s ✓ PrecompileTools 1.1 s ✓ JLLWrappers 1.5 s ✓ MPIPreferences 1.6 s ✓ Setfield 1.5 s ✓ Distances → DistancesSparseArraysExt 0.8 s ✓ ArrayInterface → ArrayInterfaceFillArraysExt 0.5 s ✓ ArrayInterface → ArrayInterfaceStaticArraysCoreExt 1.5 s ✓ ArrayInterface → ArrayInterfaceSparseArraysExt 1.8 s ✓ QuadGK 1.5 s ✓ Gamma 1.7 s ✓ Tables 5.8 s ✓ StringManipulation 12.8 s ✓ StaticArrays 1.5 s ✓ SciMLPublic 1.6 s ✓ CommonWorldInvalidations 2.8 s ✓ RecipesBase 1.8 s ✓ ADTypes 10.6 s ✓ Parsers 42.5 s ✓ JLD2 1.2 s ✓ Libffi_jll 1.1 s ✓ Bzip2_jll 0.7 s ✓ MicrosoftMPI_jll 1.2 s ✓ OpenSpecFun_jll 1.0 s ✓ Xorg_xtrans_jll 3.9 s ✓ IntelOpenMP_jll 1.0 s ✓ libpng_jll 1.0 s ✓ LinearElasticity_jll 3.8 s ✓ oneTBB_jll 1.0 s ✓ Libmount_jll 1.5 s ✓ Libuuid_jll 1.0 s ✓ SCOTCH_jll 1.0 s ✓ Xorg_libXau_jll 1.1 s ✓ FFTW_jll 1.3 s ✓ METIS_jll 1.4 s ✓ libaec_jll 1.1 s ✓ Xorg_libpciaccess_jll 1.1 s ✓ LLVMOpenMP_jll 1.1 s ✓ Libiconv_jll 1.0 s ✓ Xorg_libXdmcp_jll 1.1 s ✓ Expat_jll 1.2 s ✓ JpegTurbo_jll 4.6 s ✓ OpenMPI_jll 3.7 s ✓ MPItrampoline_jll 1.2 s ✓ FiniteDiff 0.9 s ✓ StructUtils → StructUtilsTablesExt 39.5 s ✓ PrettyTables 2.9 s ✓ ArnoldiMethod 1.3 s ✓ StaticArrays → StaticArraysStatisticsExt 1.3 s ✓ ConstructionBase → ConstructionBaseStaticArraysExt 1.3 s ✓ Adapt → AdaptStaticArraysExt 1.8 s ✓ FillArrays → FillArraysStaticArraysExt 1.9 s ✓ Static 3.9 s ✓ IterativeSolvers 0.8 s ✓ ADTypes → ADTypesConstructionBaseExt 1.8 s ✓ DifferentiationInterface 8.3 s ✓ JSON 1.0 s ✓ FreeType2_jll 5.0 s ✓ SpecialFunctions Downloading artifact: IntelOpenMP Downloading artifact: oneTBB 8.2 s ✓ MKL_jll 1.5 s ✓ MMG_jll 2.6 s ✓ Metis 1.0 s ✓ Pixman_jll 1.1 s ✓ XML2_jll 1.1 s ✓ GettextRuntime_jll 1.2 s ✓ Xorg_libxcb_jll 1.3 s ✓ FiniteDiff → FiniteDiffStaticArraysExt 1.4 s ✓ FiniteDiff → FiniteDiffSparseArraysExt 13.9 s ✓ TimerOutputs 7.1 s ✓ NearestNeighbors 9.1 s ✓ Graphs 23.6 s ✓ ArrayLayouts 0.9 s ✓ BitTwiddlingConvenienceFunctions 2.6 s ✓ CPUSummary 2.8 s ✓ StaticArrayInterface 1.0 s ✓ DifferentiationInterface → DifferentiationInterfaceFiniteDiffExt 1.3 s ✓ DifferentiationInterface → DifferentiationInterfaceStaticArraysExt 1.7 s ✓ DifferentiationInterface → DifferentiationInterfaceSparseArraysExt 1.4 s ✓ Fontconfig_jll 3.7 s ✓ FastGaussQuadrature 1.1 s ✓ DiffRules 2.7 s ✓ FFTW 1.0 s ✓ LightXML 1.3 s ✓ Hwloc_jll 1.4 s ✓ Glib_jll 1.3 s ✓ Xorg_libX11_jll 3.2 s ✓ Metis → MetisGraphs 4.4 s ✓ ArrayLayouts → ArrayLayoutsSparseArraysExt 5.5 s ✓ BlockArrays 1.6 s ✓ PolyesterWeave 1.0 s ✓ StaticArrayInterface → StaticArrayInterfaceOffsetArraysExt 1.6 s ✓ StaticArrayInterface → StaticArrayInterfaceStaticArraysExt 1.0 s ✓ CloseOpenIntervals 1.4 s ✓ LayoutPointers 7.4 s ✓ ForwardDiff 3.9 s ✓ PolynomialBases 2.0 s ✓ WriteVTK 1.3 s ✓ MPICH_jll 4.2 s ✓ MPIABI_jll 1.1 s ✓ Xorg_libXfixes_jll 1.1 s ✓ Xorg_libXrender_jll 1.1 s ✓ Xorg_libXext_jll 3.9 s ✓ BlockArrays → BlockArraysAdaptExt 1.8 s ✓ StrideArraysCore 1.7 s ✓ ForwardDiff → ForwardDiffStaticArraysExt 1.4 s ✓ DifferentiationInterface → DifferentiationInterfaceForwardDiffExt 5.2 s ✓ HDF5_jll 11.6 s ✓ MPI 1.3 s ✓ Xorg_libXft_jll 1.2 s ✓ Xorg_libXinerama_jll 1.2 s ✓ Cairo_jll 1.3 s ✓ Libglvnd_jll 2.0 s ✓ Polyester 3.3 s ✓ NLSolversBase 1.1 s ✓ GLU_jll 1.2 s ✓ OCCT_jll 1.4 s ✓ FLTK_jll 3.6 s ✓ SparseMatricesCSR 2.8 s ✓ LineSearches 4.4 s ✓ gmsh_jll 8.4 s ✓ PartitionedArrays 3.2 s ✓ NLsolve 55.5 s ✓ Gridap 20.5 s ✓ GridapDistributed 19.6 s ✓ GridapGmsh 19.7 s ✓ GridapSolvers 17.6 s ✓ GridapSolvers → IterativeSolversExt 24.0 s ✓ HyperFEM 194 dependencies successfully precompiled in 643 seconds. 41 already precompiled. 1 dependency had output during precompilation: ┌ MKL_jll │ Downloading artifact: IntelOpenMP │ Downloading artifact: oneTBB └ Precompilation completed after 687.26s ################################################################################ # Testing # Testing HyperFEM Status `/tmp/jl_ugM6Lh/Project.toml` [f6369f11] ForwardDiff v1.4.5 ⌅ [56d4f2e9] Gridap v0.19.11 [6d3209ee] GridapSolvers v0.7.1 [ddbf423a] HyperFEM v0.0.6 [682c06a0] JSON v1.7.1 [90137ffa] StaticArrays v1.9.19 [a759f4b9] TimerOutputs v1.2.0 [8dfed614] Test v1.11.0 Status `/tmp/jl_ugM6Lh/Manifest.toml` [47edcb42] ADTypes v1.24.0 [621f4979] AbstractFFTs v1.5.0 [1520ce14] AbstractTrees v0.4.5 [79e6a3ab] Adapt v4.7.0 [dce04be8] ArgCheck v2.5.0 [ec485272] ArnoldiMethod v0.4.0 [4fba245c] 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[e66e0078] CompilerSupportLibraries_jll v1.5.7+0 [781609d7] GMP_jll v6.3.0+4 [deac9b47] LibCURL_jll v8.21.0+0 [e37daf67] LibGit2_jll v1.9.7+0 [29816b5a] LibSSH2_jll v1.11.104+0 [14a3606d] MozillaCACerts_jll v2026.8.13 [4536629a] OpenBLAS_jll v0.3.34+0 [05823500] OpenLibm_jll v0.8.7+0 [458c3c95] OpenSSL_jll v3.5.8+0 [efcefdf7] PCRE2_jll v10.47.0+0 [bea87d4a] SuiteSparse_jll v7.10.1+0 [83775a58] Zlib_jll v1.3.2+0 [3161d3a3] Zstd_jll v1.5.7+1 [8e850b90] libblastrampoline_jll v5.15.0+0 [8e850ede] nghttp2_jll v1.70.0+0 [3f19e933] p7zip_jll v17.8.2+0 Info Packages marked with ⌃ and ⌅ have new versions available. Those with ⌃ may be upgradable, but those with ⌅ are restricted by compatibility constraints from upgrading. Testing Running tests... ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:632 Expression: norm(∂ΨE(F(∇u), E(∇φ), θt)) == 3.890788259241063 Evaluated: 3.8907882592410625 == 3.890788259241063 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:632 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:633 Expression: ∂Ψθ(F(∇u), E(∇φ), θt) == -0.1756808680132173 Evaluated: -0.1756808680132174 == -0.1756808680132173 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:633 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:634 Expression: norm(∂ΨFF(F(∇u), E(∇φ), θt)) == 41.75134321258517 Evaluated: 41.751343212585176 == 41.75134321258517 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:634 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:635 Expression: norm(∂ΨEE(F(∇u), E(∇φ), θt)) == 1.9388101847663917 Evaluated: 1.9388101847663914 == 1.9388101847663917 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:635 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:636 Expression: norm(∂Ψθθ(F(∇u), E(∇φ), θt)) == 0.05854786347086507 Evaluated: 0.05854786347086505 == 0.05854786347086507 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:636 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:637 Expression: norm(∂ΨEF(F(∇u), E(∇φ), θt)) == 10.455220025096452 Evaluated: 10.455220025096454 == 10.455220025096452 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:637 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:638 Expression: norm(∂ΨFθ(F(∇u), E(∇φ), θt)) == 0.059252287541736004 Evaluated: 0.059252287541736025 == 0.059252287541736004 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:638 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] ThermoElectroMech_PINNS: Test Failed at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:639 Expression: norm(∂ΨEθ(F(∇u), E(∇φ), θt)) == 0.023111702806623537 Evaluated: 0.02311170280662355 == 0.023111702806623537 Stacktrace: [1] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:591 [2] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [3] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/PhysicalModelTests.jl:639 [inlined] [4] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:784 [inlined] 807.309442 seconds (183.72 M allocations: 11.619 GiB, 1.27% gc time, 99.87% compilation time) ViscousIncompressible: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:83 Test threw exception Expression: isapprox(∂Ψuu(F, Fn, Avn), tangent, rtol = rtolH) ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [inlined] [10] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:781 [inlined] [11] test_viscous_derivatives_numerical(model::ViscousIncompressible; rtolP::Float64, rtolH::Float64) @ Main ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:83 ViscousIncompressible2: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:143 Test threw exception Expression: isapprox(norm(∂Ψuu(F, Fn, Avn)), 4.847586088299776, rtol = 1.0e-10) ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [10] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:133 [11] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [12] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:143 [inlined] [13] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:781 [inlined] GeneralizedMaxwell NeoHookean 1-branch: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:83 Test threw exception Expression: isapprox(∂Ψuu(F, Fn, Avn), tangent, rtol = rtolH) ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [inlined] [10] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}})(∂ΨiFF::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, Ai::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [11] (::Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}})(args::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base operators.jl:1381 [inlined] [12] (::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}})(acc::TensorValue{9, 9, Float64, 81}, x::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base reduce.jl:98 [inlined] [13] _foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, init::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}) @ Base reduce.jl:56 [14] foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, nt::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}) @ Base reduce.jl:46 [inlined] [15] mapfoldl_impl(f::typeof(identity), op::typeof(+), nt::TensorValue{9, 9, Float64, 81}, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}) @ Base reduce.jl:42 [inlined] [16] mapfoldl(f::typeof(identity), op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; init::TensorValue{9, 9, Float64, 81}) @ Base reduce.jl:173 [inlined] [17] mapreduce(f::typeof(identity), op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:306 [inlined] [18] reduce(op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:498 [inlined] [19] mapreduce(f::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}, op::typeof(+), itr::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, itrs::Tuple{VectorValue{10, Float64}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:307 [inlined] [20] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [21] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:134 [22] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:781 [inlined] [23] test_viscous_derivatives_numerical(model::GeneralizedMaxwell{NeoHookean3D}; rtolP::Float64, rtolH::Float64) @ Main ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ViscousModelsTests.jl:83 568.793675 seconds (72.05 M allocations: 4.546 GiB, 0.71% gc time, 99.84% compilation time) ViscoElectricModel: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:138 Test threw exception Expression: norm(∂Ψuu(F(∇u), E(∇φ), F(∇un), Avn)) ≈ 3110.7607787445168 ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [inlined] [10] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}})(∂ΨiFF::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, Ai::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [11] (::Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}})(args::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base operators.jl:1381 [inlined] [12] (::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}})(acc::TensorValue{9, 9, Float64, 81}, x::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base reduce.jl:98 [inlined] [13] _foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, init::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}) @ Base reduce.jl:56 [14] foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, nt::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}) @ Base reduce.jl:46 [inlined] [15] mapfoldl_impl(f::typeof(identity), op::typeof(+), nt::TensorValue{9, 9, Float64, 81}, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}) @ Base reduce.jl:42 [inlined] [16] mapfoldl(f::typeof(identity), op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; init::TensorValue{9, 9, Float64, 81}) @ Base reduce.jl:173 [inlined] [17] mapreduce(f::typeof(identity), op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:306 [inlined] [18] reduce(op::typeof(+), itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:498 [inlined] [19] mapreduce(f::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}, op::typeof(+), itr::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, itrs::Tuple{VectorValue{10, Float64}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:307 [inlined] [20] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [21] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:134 [22] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##10"{HyperFEM.PhysicalModels.var"#∂Ψem∂FF#∂Ψem∂FF##0"{HyperFEM.PhysicalModels.var"#∂Ψem_JJ#∂Ψem_JJ##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HEHE#HEHE##0"{HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_HJ#∂Ψem_HJ##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_HH#∂Ψem_HH##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_∂J#∂Ψem_∂J##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HEHE#HEHE##0"{HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_∂H#∂Ψem_∂H##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}})(F::TensorValue{3, 3, Float64, 9}, E::VectorValue{3, Float64}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ElectroMechanicalModels.jl:53 [23] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:121 [24] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [25] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:138 [inlined] [26] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:781 [inlined] ViscoElectricModel 2-branch: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:161 Test threw exception Expression: norm(∂Ψuu(F(∇u), E(∇φ), F(∇un), Avn, Avn)) ≈ 3110.9722775475557 ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [inlined] [10] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}})(∂ΨiFF::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, Ai::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [11] (::Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}})(args::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base operators.jl:1381 [inlined] [12] (::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}})(acc::TensorValue{9, 9, Float64, 81}, x::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base reduce.jl:98 [inlined] [13] _foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, init::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}) @ Base reduce.jl:56 [14] foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, nt::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}) @ Base reduce.jl:46 [inlined] [15] mapfoldl_impl(f::typeof(identity), op::typeof(+), nt::TensorValue{9, 9, Float64, 81}, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}) @ Base reduce.jl:42 [16] mapfoldl(f::Function, op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; init::TensorValue{9, 9, Float64, 81}) @ Base reduce.jl:173 [17] mapreduce(f::typeof(identity), op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:306 [inlined] [18] reduce(op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:498 [inlined] [19] mapreduce(f::Function, op::Function, itr::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, itrs::Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:307 [20] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}})(::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::Vararg{VectorValue{10, Float64}}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [21] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}})(::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::Vararg{VectorValue{10, Float64}}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:134 [22] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##10"{HyperFEM.PhysicalModels.var"#∂Ψem∂FF#∂Ψem∂FF##0"{HyperFEM.PhysicalModels.var"#∂Ψem_JJ#∂Ψem_JJ##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HEHE#HEHE##0"{HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_HJ#∂Ψem_HJ##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_HH#∂Ψem_HH##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_∂J#∂Ψem_∂J##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HEHE#HEHE##0"{HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#∂Ψem_∂H#∂Ψem_∂H##0"{IdealDielectric, HyperFEM.PhysicalModels.var"#HE#HE##0"{HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#J#J##18"}, HyperFEM.PhysicalModels.var"#H#H##18"}, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}})(::TensorValue{3, 3, Float64, 9}, ::VectorValue{3, Float64}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::Vararg{VectorValue{10, Float64}}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ElectroMechanicalModels.jl:53 [23] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:143 [24] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [25] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/TestConstitutiveModels/ElectroMechanicalTests.jl:161 [inlined] [26] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:781 [inlined] 7.331506 seconds (4.45 M allocations: 278.447 MiB, 5.13% gc time, 86.96% compilation time) 2.186620 seconds (462.94 k allocations: 26.953 MiB, 96.29% compilation time) 11.354222 seconds (6.01 M allocations: 384.374 MiB, 1.36% gc time, 98.17% compilation time) 249.526269 seconds (135.71 M allocations: 8.078 GiB, 2.39% gc time, 99.83% compilation time) SimulationsTests: Error During Test at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/SimulationsTests/runtests.jl:5 Got exception outside of a @test LoadError: ArgumentError: cannot reinterpret an `Float64` array to `NTuple{81, Float64}` whose first dimension has size `9`. The resulting array would have a non-integral first dimension. Stacktrace: [1] (::Base.var"#thrownonint#reinterpret##0")(S::Core.TypeEgal{Float64}, T::Core.TypeEgal{NTuple{81, Float64}}, dim::Int64) @ Base reinterpretarray.jl:76 [2] reinterpret(::Core.TypeEgal{NTuple{81, Float64}}, a::Matrix{Float64}) @ Base reinterpretarray.jl:96 [inlined] [3] _totuple(T::Core.TypeEgal{NTuple{81, Float64}}, itr::Matrix{Float64}) @ Base reinterpretarray.jl:983 [4] NTuple{81, Float64}(itr::Matrix{Float64}) @ Base tuple.jl:467 [5] TensorValue(data::Matrix{Float64}) @ Gridap.TensorValues ~/.julia/packages/Gridap/eNa8j/src/TensorValues/TensorValueTypes.jl:66 [6] ∂Ce_∂C(::ViscousIncompressible, γα::Float64, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, invUvn::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, λα::Float64, F::TensorValue{3, 3, Float64, 9}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:366 [7] ViscousTangentOperator(obj::ViscousIncompressible, Se_::HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, ∂Se∂Ce_::HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, F::TensorValue{3, 3, Float64, 9}, Ce_trial::TensorValue{3, 3, Float64, 9}, Ce::TensorValue{3, 3, Float64, 9}, invUv::TensorValue{3, 3, Float64, 9}, invUvn::TensorValue{3, 3, Float64, 9}, λα::Float64) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:417 [8] Tangent(obj::ViscousIncompressible, Se_::Function, ∂Se∂Ce_::Function, F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:547 [9] (::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}})(F::TensorValue{3, 3, Float64, 9}, Fn::TensorValue{3, 3, Float64, 9}, A::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:22 [inlined] [10] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}})(∂ΨiFF::HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, Ai::VectorValue{10, Float64}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [inlined] [11] (::Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}})(args::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base operators.jl:1381 [inlined] [12] (::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}})(acc::TensorValue{9, 9, Float64, 81}, x::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, VectorValue{10, Float64}}) @ Base reduce.jl:98 [inlined] [13] _foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, init::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}) @ Base reduce.jl:56 [14] foldl_impl(op::Base.MappingRF{Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}, Base.BottomRF{typeof(+)}}, nt::TensorValue{9, 9, Float64, 81}, itr::Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}) @ Base reduce.jl:46 [inlined] [15] mapfoldl_impl(f::typeof(identity), op::typeof(+), nt::TensorValue{9, 9, Float64, 81}, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}) @ Base reduce.jl:42 [16] mapfoldl(f::Function, op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; init::TensorValue{9, 9, Float64, 81}) @ Base reduce.jl:173 [17] mapreduce(f::typeof(identity), op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:306 [inlined] [18] reduce(op::Function, itr::Base.Generator{Base.Iterators.Zip{Tuple{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}}}, Base.Splat{HyperFEM.PhysicalModels.var"#∂Ψ∂FF##4#∂Ψ∂FF##5"{TensorValue{3, 3, Float64, 9}, TensorValue{3, 3, Float64, 9}}}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:498 [inlined] [19] mapreduce(f::Function, op::Function, itr::Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}, itrs::Tuple{VectorValue{10, Float64}, VectorValue{10, Float64}, VectorValue{10, Float64}}; kw::@Kwargs{init::TensorValue{9, 9, Float64, 81}}) @ Base reduce.jl:307 [20] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}})(::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::Vararg{VectorValue{10, Float64}}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:89 [21] (::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}})(::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::Vararg{VectorValue{10, Float64}}) @ HyperFEM.PhysicalModels ~/.julia/packages/HyperFEM/y0wAc/src/PhysicalModels/ViscousModels.jl:134 [22] evaluate!(::Nothing, ::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}, ::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:93 [inlined] [23] evaluate(::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}, ::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:87 [inlined] [24] return_value(::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}, ::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:64 [inlined] [25] return_type(::HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}, ::TensorValue{3, 3, Float64, 9}, ::TensorValue{3, 3, Float64, 9}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}, ::VectorValue{10, Float64}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:62 [inlined] [26] return_value(::Broadcasting{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:191 [27] return_value(::Gridap.Fields.BroadcastingFieldOpMap{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}) @ Gridap.Fields ~/.julia/packages/Gridap/eNa8j/src/Fields/FieldArrays.jl:570 [inlined] [28] return_type(::Gridap.Fields.BroadcastingFieldOpMap{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{TensorValue{3, 3, Float64, 9}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}, ::Vector{VectorValue{10, Float64}}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:62 [inlined] [29] lazy_map(::Gridap.Fields.BroadcastingFieldOpMap{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, ::LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{HyperFEM.PhysicalModels.var"#14#15"}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{typeof(adjoint)}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{typeof(dot)}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{FillArrays.Fill{Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{FillArrays.Fill{Gridap.Fields.LinearCombinationMap{Colon}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Broadcasting{PosNegReindex{Vector{Float64}, Vector{Float64}}}, 1, Tuple{Base.OneTo{Int64}}}, Vector{Float64}, 1, Tuple{Table{Int32, Vector{Int32}, Vector{Int32}}}}, FillArrays.Fill{Matrix{TensorValue{3, 3, Float64, 9}}, 1, Tuple{Base.OneTo{Int64}}}}}}}}}}}, ::LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{HyperFEM.PhysicalModels.var"#14#15"}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{typeof(adjoint)}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Gridap.Fields.BroadcastingFieldOpMap{typeof(dot)}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{FillArrays.Fill{Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{FillArrays.Fill{Gridap.Fields.LinearCombinationMap{Colon}, 1, Tuple{Base.OneTo{Int64}}}, Vector{TensorValue{3, 3, Float64, 9}}, 1, Tuple{LazyArray{FillArrays.Fill{Broadcasting{PosNegReindex{Vector{Float64}, Vector{Float64}}}, 1, Tuple{Base.OneTo{Int64}}}, Vector{Float64}, 1, Tuple{Table{Int32, Vector{Int32}, Vector{Int32}}}}, FillArrays.Fill{Matrix{TensorValue{3, 3, Float64, 9}}, 1, Tuple{Base.OneTo{Int64}}}}}}}}}}}, ::Vector{Vector{VectorValue{10, Float64}}}, ::Vector{Vector{VectorValue{10, Float64}}}, ::Vector{Vector{VectorValue{10, Float64}}}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/LazyArrays.jl:57 [30] evaluate!(cache::Nothing, f::Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellFields.jl:399 ┌ [31] evaluate(f::Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) │ @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:87 [inlined] ├ [32] (::Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}})(x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) │ @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellFields.jl:247 [inlined] ├ [33] (::Gridap.CellData.var"#evaluate!##0#evaluate!##1"{Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}})(i::Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}) │ @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellFields.jl:398 [inlined] ├ [34] map(f::Gridap.CellData.var"#evaluate!##0#evaluate!##1"{Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, t::Tuple{Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##6"{HyperFEM.PhysicalModels.var"#∂Ψ∂FF#∂Ψ∂FF##3"{Tuple{HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}, HyperFEM.PhysicalModels.var"#∂Ψ∂F∂F#∂Ψ∂F∂F##0"{ViscousIncompressible, HyperFEM.PhysicalModels.var"#∂S∂C#SecondPiola##7"{HyperFEM.PhysicalModels.var"#∂2Ψ∂2dC#SecondPiola##6"{Float64}, HyperFEM.PhysicalModels.var"#∂2Ψ∂CdC#SecondPiola##5"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}, HyperFEM.PhysicalModels.var"#S#SecondPiola##4"{HyperFEM.PhysicalModels.var"#∂Ψ∂dC#SecondPiola##3"{Float64}, HyperFEM.PhysicalModels.var"#∂Ψ∂C#SecondPiola##2"{Float64}, HyperFEM.PhysicalModels.var"#H#SecondPiola##0"}}}}, HyperFEM.PhysicalModels.var"#∂Ψuu#164"{HyperFEM.PhysicalModels.var"#∂Ψ2_∂J2#163"{HyperFEM.PhysicalModels.var"#∂log2∂J2#160"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#∂Ψ_∂J#161"{HyperFEM.PhysicalModels.var"#∂log∂J#159"{Float64}, HyperFEM.PhysicalModels.var"#J#156", Float64, Float64}, HyperFEM.PhysicalModels.var"#H#157", Float64}}}, Gridap.CellData.OperationCellField{ReferenceDomain, typeof(adjoint)}}) │ @ Base tuple.jl:360 ├ [35] evaluate!(cache::Nothing, f::Gridap.CellData.OperationCellField{ReferenceDomain, typeof(inner)}, x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) │ @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellFields.jl:398 ╰───── repeated 2 times [41] evaluate(f::Gridap.CellData.OperationCellField{ReferenceDomain, typeof(inner)}, x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) @ Gridap.Arrays ~/.julia/packages/Gridap/eNa8j/src/Arrays/Maps.jl:87 [inlined] [42] (::Gridap.CellData.OperationCellField{ReferenceDomain, typeof(inner)})(x::Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}) @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellFields.jl:247 [43] integrate(f::Gridap.CellData.OperationCellField{ReferenceDomain, typeof(inner)}, quad::CellQuadrature{ReferenceDomain, PhysicalDomain}) @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/CellQuadratures.jl:151 [44] integrate(f::Gridap.CellData.OperationCellField{ReferenceDomain, typeof(inner)}, b::Gridap.CellData.GenericMeasure) @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/DomainContributions.jl:168 [45] *(a::Gridap.CellData.Integrand, b::Gridap.CellData.GenericMeasure) @ Gridap.CellData ~/.julia/packages/Gridap/eNa8j/src/CellData/DomainContributions.jl:152 [46] jacobian(::GeneralizedMaxwell{NeoHookean3D}, ::Kinematics{Mechano, Solid}, ::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}, ::Gridap.FESpaces.SingleFieldFEBasis{Gridap.FESpaces.TrialBasis, ReferenceDomain}, ::Gridap.FESpaces.SingleFieldFEBasis{Gridap.FESpaces.TestBasis, ReferenceDomain}, ::Gridap.CellData.GenericMeasure, ::Float64, ::Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#14#15"}, ::CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, ::CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, ::Vararg{CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}}) @ HyperFEM.WeakForms ~/.julia/packages/HyperFEM/y0wAc/src/WeakForms/WeakForms.jl:52 [47] (::var"#118#119"{Float64, Int64, Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#14#15"}, Tuple{CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}}, Gridap.CellData.GenericMeasure, Kinematics{Mechano, Solid}, GeneralizedMaxwell{NeoHookean3D}})(u::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}, du::Gridap.FESpaces.SingleFieldFEBasis{Gridap.FESpaces.TrialBasis, ReferenceDomain}, v::Gridap.FESpaces.SingleFieldFEBasis{Gridap.FESpaces.TestBasis, ReferenceDomain}) @ Main ~/.julia/packages/HyperFEM/y0wAc/test/data/ViscoElasticSimulation.jl:73 [48] allocate_jacobian(op::Gridap.FESpaces.FEOperatorFromWeakForm, uh::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}) @ Gridap.FESpaces ~/.julia/packages/Gridap/eNa8j/src/FESpaces/FEOperatorsFromWeakForm.jl:70 [49] jacobian(op::Gridap.FESpaces.FEOperatorFromWeakForm, u::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}) @ Gridap.FESpaces ~/.julia/packages/Gridap/eNa8j/src/FESpaces/FEOperators.jl:76 [50] jacobian(op::Gridap.FESpaces.AlgebraicOpFromFEOp, x::Vector{Float64}) @ Gridap.FESpaces ~/.julia/packages/Gridap/eNa8j/src/FESpaces/FEOperators.jl:182 [51] instantiate_caches(x::Vector{Float64}, nls::NewtonSolver, op::Gridap.FESpaces.AlgebraicOpFromFEOp) @ HyperFEM.ComputationalModels ~/.julia/packages/HyperFEM/y0wAc/src/ComputationalModels/FESpaces.jl:130 [52] StaticNonlinearModel(res::var"#res#114"{Int64, Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#14#15"}, Tuple{CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}}, Gridap.CellData.GenericMeasure, Kinematics{Mechano, Solid}, GeneralizedMaxwell{NeoHookean3D}}, jac::var"#jac#117"{Int64, Gridap.CellData.OperationCellField{ReferenceDomain, HyperFEM.PhysicalModels.var"#14#15"}, Tuple{CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}, CellState{VectorValue{10, Float64}, Gridap.CellData.CellPoint{ReferenceDomain, FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}, LazyArray{Gridap.Geometry.CartesianMap{3, Float64, 9}, Vector{VectorValue{3, Float64}}, 1, Tuple{FillArrays.Fill{Vector{VectorValue{3, Float64}}, 1, Tuple{Base.OneTo{Int64}}}}}, Gridap.Geometry.BodyFittedTriangulation{3, 3, CartesianDiscreteModel{3, Float64, typeof(identity)}, CartesianGrid{3, Float64, typeof(identity)}, IdentityVector{Int64}}}}}, Gridap.CellData.GenericMeasure, Kinematics{Mechano, Solid}, GeneralizedMaxwell{NeoHookean3D}}, U::TrialFESpace{UnconstrainedFESpace{Vector{Float64}, Gridap.FESpaces.NodeToDofGlue{VectorValue{3, Int32}}}}, V::UnconstrainedFESpace{Vector{Float64}, Gridap.FESpaces.NodeToDofGlue{VectorValue{3, Int32}}}, dirbc::DirichletBC{Vector{Vector{Float64}}}; assem_U::GenericSparseMatrixAssembler, nls::NewtonSolver, xh::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}, xh⁻::SingleFieldFEFunction{Gridap.CellData.GenericCellField{ReferenceDomain}}) @ HyperFEM.ComputationalModels ~/.julia/packages/HyperFEM/y0wAc/src/ComputationalModels/Drivers.jl:107 [53] visco_elastic_simulation(; t_end::Int64, writevtk::Bool, verbose::Bool) @ Main ~/.julia/packages/HyperFEM/y0wAc/test/data/ViscoElasticSimulation.jl:77 [54] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/SimulationsTests/ViscoElasticSimulationTest.jl:6 [55] include(mapexpr::Function, mod::Module, _path::String) @ Base Base.jl:335 [56] top-level scope @ ~/.julia/packages/HyperFEM/y0wAc/test/SimulationsTests/runtests.jl:7 [57] macro expansion @ /opt/julia/share/julia/stdlib/v1.14/Test/src/Test.jl:2247 [inlined] [58] macro expansion @ ~/.julia/packages/HyperFEM/y0wAc/test/SimulationsTests/runtests.jl:7 [inlined] in expression starting at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/SimulationsTests/ViscoElasticSimulationTest.jl:6 Test Summary: | Pass Fail Error Total Time HyperFEMTests | 375 8 6 389 28m21.2s ConstitutiveModels | 300 8 5 313 23m05.7s composition of HGO_1Fiber | 3 3 14.4s HGO_4Fibers | 3 3 14.2s composition of HGO_4Fibers+MooneyRivlin3D | 3 3 53.5s Iso+Aniso | 3 3 48.2s Iso+MultiAniso | 3 3 1.5s NonlinearMooneyRivlin_CV | 3 3 1m08.0s NonlinearNeoHookean_CV | 3 3 8.4s IsochoricNeoHookean3D | 5 5 10.7s LinearElasticity2D | 3 3 2.7s LinearElasticity3D | 3 3 17.2s NeoHookean3D | 3 3 7.5s Gent2D | 3 3 1.6s PlaneStressIncompressible_I1PD | 2 2 1.0s MooneyRivlin2D | 3 3 2.1s MooneyRivlin3D | 3 3 20.6s NonlinearMooneyRivlin2D | 3 3 2.1s Yeoh3D | 3 3 11.4s NonlinearMooneyRivlin2D_CV | 3 3 1.6s NonlinearMooneyRivlin3D | 3 3 1m07.1s IncompressibleNeoHookean2D | 3 3 1.5s IncompressibleNeoHookean2D_CV | 3 3 1.4s NonlinearIncompressibleMooneyRivlin2D_CV | 3 3 1.4s EightChain | 3 3 7.0s TransverseIsotropy2D | 4 4 0.6s TransverseIsotropy3D | 4 4 0.0s TermoElectroMech | 10 10 1m00.5s TermoMech | 6 6 0.4s ThermoMech_EntropicPolyconvex | 6 6 42.8s ThermoElectroMech_Bonet | 10 10 50.0s VolumetricEnergy | 3 3 4.0s CoerciveVolumetric | 3 3 4.7s ThermoElectroMech_Govindjee | 10 10 47.1s ThermoElectroMech_PINNS | 2 8 10 1m18.4s Magnetic_αr_mutability | 3 3 0.9s IdealMagnetic2D | 3 3 0.2s IdealMagnetic | 6 6 58.8s HardMagnetic_SoftMaterial3D_aniso | 6 6 1m19.1s HardMagnetic_SoftMaterial3D | 6 6 0.4s Magnetic3D | 3 3 0.1s Magnetic2D | 3 3 0.2s IdealMagnetic_SoftMaterial2D | 6 6 1.6s HardMagnetic_SoftMaterial2D | 6 6 2.2s ARAP2D | 3 3 1.2s ARAP2D_regularized | 3 3 1.6s NonlinearARAP2D | 3 3 1.3s HessianRegularization | 4 4 3.0s Hessian∇JRegularization | 4 4 0.4s broadcastable | 1 1 0.6s VolumetricEnergy | 2 2 1.6s EightChain | 2 2 1.3s EightChain+VolumetricEnergy | 2 2 1.0s NeoHookean3D | 2 2 0.7s ViscousIncompressible | 1 1 2 2m29.8s ViscousIncompressible2 | 1 1 2 0.2s GeneralizedMaxwell EightChain 0-branch | 2 2 1.3s GeneralizedMaxwell NeoHookean 0-branch | 2 2 0.9s GeneralizedMaxwell NeoHookean 1-branch | 1 1 2 1.9s Dissipation ViscousIncompressible | 1 1 0.0s Dissipation invertibility | 5 5 1.5s GeneralizedMaxell energy at rest | 4 4 0.2s ViscousPolyconvex | 4 4 6m48.1s IdealDielectric | 6 6 3.9s Electro+4*HGO_1Fiber | 3 3 0.3s ElectroMechano | 6 6 0.2s FlexoElectroMechanics | 6 6 0.5s ViscoElectricModel | 1 1 2 0.2s ViscoElectricModel 2-branch | 1 1 2 1.3s ConstantEnergyLaw | 10 10 0.0s ConstantCvLaw | 10 10 0.1s EntropicElasticityLaw | 10 10 0.1s NonlinearMeltingLaw | 10 10 0.2s NonlinearSofteningLaw | 10 10 0.2s PolynomialLaw | 10 10 0.1s TensorAlgebra | 57 57 11.4s WeakForms | 18 18 4m09.5s SimulationsTests | 1 1 52.9s RNG of the outermost testset: Random.Xoshiro(0xaa8274f9ec17172d, 0xf26c58a01eefb285, 0xaa70989e79adebfe, 0x395e75c1e4c28b79, 0x678fb23fea9d9b01) ERROR: LoadError: Some tests did not pass: 375 passed, 8 failed, 6 errored, 0 broken. in expression starting at /home/pkgeval/.julia/packages/HyperFEM/y0wAc/test/runtests.jl:5 Testing failed after 1730.95s ERROR: LoadError: Package HyperFEM errored during testing Stacktrace: [1] pkgerror(msg::String) @ Pkg.Types /opt/julia/share/julia/stdlib/v1.14/Pkg/src/Types.jl:68 [2] test(ctx::Pkg.Types.Context, pkgs::Vector{PackageSpec}; coverage::Bool, julia_args::Cmd, test_args::Cmd, test_fn::Nothing, force_latest_compatible_version::Bool, allow_earlier_backwards_compatible_versions::Bool, allow_reresolve::Bool) @ Pkg.Operations /opt/julia/share/julia/stdlib/v1.14/Pkg/src/Operations.jl:3283 [3] test(ctx::Pkg.Types.Context, pkgs::Vector{PackageSpec}; coverage::Bool, test_fn::Nothing, julia_args::Cmd, test_args::Cmd, force_latest_compatible_version::Bool, allow_earlier_backwards_compatible_versions::Bool, allow_reresolve::Bool, kwargs::@Kwargs{io::IOContext{IO}}) @ Pkg.API /opt/julia/share/julia/stdlib/v1.14/Pkg/src/API.jl:587 [4] test(pkgs::Vector{PackageSpec}; io::IOContext{IO}, kwargs::@Kwargs{julia_args::Cmd}) @ Pkg.API /opt/julia/share/julia/stdlib/v1.14/Pkg/src/API.jl:172 [5] test(pkgs::Vector{String}; kwargs::@Kwargs{julia_args::Cmd}) @ Pkg.API /opt/julia/share/julia/stdlib/v1.14/Pkg/src/API.jl:160 [6] test(pkg::String; kwargs::@Kwargs{julia_args::Cmd}) @ Pkg.API /opt/julia/share/julia/stdlib/v1.14/Pkg/src/API.jl:159 [inlined] [7] top-level scope @ /PkgEval.jl/scripts/evaluate.jl:223 in expression starting at /PkgEval.jl/scripts/evaluate.jl:214 PkgEval failed after 2636.25s: package tests unexpectedly errored