From c8ffeb14a78563084fd37a846c33a6cc6de29e0f Mon Sep 17 00:00:00 2001 From: Theodore Date: Wed, 11 Sep 2024 20:39:07 +0200 Subject: [PATCH] v3.5 (#86) --- .github/workflows/dev.yml | 2 +- .gitignore | 9 +- docs/Basic/Compile.md | 272 +++++++------- docs/Basic/Obtain.md | 40 +-- docs/Basic/Performance.md | 28 +- docs/Basic/Structure.md | 6 +- docs/Collection/Configure/step.md | 8 +- docs/Collection/Define/bc.md | 38 +- docs/Collection/Define/expression.md | 12 +- docs/Collection/Define/load.md | 16 +- docs/Collection/Define/node.md | 20 +- docs/Collection/Process/materialtest.md | 8 +- docs/Collection/Process/materialtestbyload.md | 4 +- docs/Collection/Process/sectiontest.md | 12 +- docs/Collection/Process/set.md | 22 +- docs/Developer/C/material.md | 42 +-- docs/Developer/CPP/element.md | 66 ++-- docs/Developer/CPP/material.md | 8 +- .../Structural/Dynamics/bouncing-of-a-ball.md | 2 +- .../dynamic-analysis-of-a-portal-frame.md | 4 +- .../Dynamics/process-ground-motion.ipynb | 334 ++++++++++++++++++ .../Dynamics/process-ground-motion.json | 1 + .../Dynamics/process-ground-motion.md | 256 ++++++++++++++ .../process-ground-motion_11_0.png | Bin 0 -> 38965 bytes .../process-ground-motion_13_0.png | Bin 0 -> 36494 bytes .../process-ground-motion_15_0.png | Bin 0 -> 35871 bytes .../process-ground-motion_3_0.png | Bin 0 -> 25816 bytes .../process-ground-motion_5_0.png | Bin 0 -> 30827 bytes .../process-ground-motion_7_0.png | Bin 0 -> 29233 bytes .../process-ground-motion_9_0.png | Bin 0 -> 24683 bytes ...ory-analysis-of-an-elastic-coupled-wall.md | 2 +- docs/Library/Constraint/FixedLength.gif | Bin 0 -> 219264 bytes docs/Library/Constraint/FixedLength.md | 69 +++- docs/Library/Constraint/MaxForce.gif | Bin 0 -> 210606 bytes docs/Library/Constraint/MaxForce.md | 71 ++++ docs/Library/Constraint/MaximumGap2D.md | 2 +- docs/Library/Constraint/MaximumGap3D.md | 2 +- docs/Library/Constraint/MinimumGap2D.md | 2 +- docs/Library/Constraint/MinimumGap3D.md | 2 +- docs/Library/Integrator/BatheTwoStep.md | 4 + .../Material3D/Elastic/MooneyRivlin.md | 4 + .../Material/Material3D/Elastic/Yeoh.md | 2 +- docs/Library/Section/SectionNM/NM2D2.md | 14 +- docs/Library/Section/SectionNM/NM2D3.md | 10 +- docs/Library/Section/SectionNM/NM3D2.md | 20 +- docs/Library/Section/SectionNM/NM3D3.md | 18 +- docs/Library/Section/SectionNM/SectionNM.md | 2 +- docs/README.md | 19 +- docs/SUMMARY.md | 2 + mkdocs.yml | 2 + requirements.txt | 18 +- setup.py | 46 ++- 52 files changed, 1155 insertions(+), 366 deletions(-) create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion.ipynb create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion.json create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion.md create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_11_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_13_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_15_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_3_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_5_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_7_0.png create mode 100644 docs/Example/Structural/Dynamics/process-ground-motion_files/process-ground-motion_9_0.png create mode 100644 docs/Library/Constraint/FixedLength.gif create mode 100644 docs/Library/Constraint/MaxForce.gif create mode 100644 docs/Library/Constraint/MaxForce.md diff --git a/.github/workflows/dev.yml b/.github/workflows/dev.yml index f4c2b50310..381f0a1524 100644 --- a/.github/workflows/dev.yml +++ b/.github/workflows/dev.yml @@ -29,5 +29,5 @@ jobs: git config --global user.name "Theodore Chang" git config --global user.email "tlcfem@gmail.com" git pull - mike deploy 3.4 + mike deploy 3.5 git push origin gh-pages diff --git a/.gitignore b/.gitignore index ca330e3a7b..b68121c66c 100644 --- a/.gitignore +++ b/.gitignore @@ -1,15 +1,16 @@ -*egg-info +__pycache__ .idea .obsidian +.venv .vscode -__pycache__ +*egg-info build dist docs/Doxygen site suanPan-dev +suanPan-linux* suanPan-manual.py suanPan-manual.spec venv -working -suanPan-linux* \ No newline at end of file +working \ No newline at end of file diff --git a/docs/Basic/Compile.md b/docs/Basic/Compile.md index 539b7c71ed..dd58947799 100644 --- a/docs/Basic/Compile.md +++ b/docs/Basic/Compile.md @@ -1,60 +1,78 @@ # Compile -## Docker Images +## With Docker -For Linux users, if there is no access to `sudo` but can build containers with Docker, it is possible to compile the -project with -Docker. Check the provided [Dockerfiles](https://github.com/TLCFEM/suanPan/tree/dev/Script) for more information. +### Docker Images -Once the container is built, the `.tar.gz` will be placed under `/`. Simply copy them out and install/unpack the -archive. The `.deb` or `.rpm` packages are installed in the images, so they can be used directly. +For Linux users, if there is no access to `sudo` but can build containers with Docker, it is possible to compile the +project with Docker. +Check the provided [Dockerfiles](https://github.com/TLCFEM/suanPan/tree/dev/Script) for more information. + +Once the image is built, use `sp`, `suanpan` or `suanPan` to invoke the program in the container. + +### Dev Container + +Two images are provided for development purposes. + +```bash +# vtk+mkl+cuda +docker pull tlcfem/suanpan-env-cuda +# vtk+mkl +docker pull tlcfem/suanpan-env +``` + +They can be used as development containers. +VS Code and CLion can be configured to use these containers for development. +There is no need to install any dependencies on the host machine. + +## Without Docker The following is a general guide that covers three main operating systems. -## Prerequisites +### Prerequisites -1. To configure the source code, [CMake](https://cmake.org/download/) shall be available. Please download and install it - before configuring the source code package. -2. The linear algebra driver used is [OpenBLAS](https://github.com/xianyi/OpenBLAS). You may want to compile it with the - optimal configuration based on the specific machine. Otherwise, precompiled binaries (dynamic platform) are available - in this [repository](https://github.com/TLCFEM/prebuilds). -3. It is strongly recommended installing Intel MKL for potentially better performance. -4. Please be aware that MKL is throttled on AMD platforms. Performance comparisons can be seen for - example [here](https://github.com/flame/blis/blob/master/docs/Performance.md). If you have AMD CPUs please collect - more knowledge to determine which linear algebra library is more suitable. +1. To configure the source code, [CMake](https://cmake.org/download/) shall be available. Please download and install it + before configuring the source code package. +2. The linear algebra driver used is [OpenBLAS](https://github.com/xianyi/OpenBLAS). You may want to compile it with the + optimal configuration based on the specific machine. Otherwise, precompiled binaries (dynamic platform) are available + in this [repository](https://github.com/TLCFEM/prebuilds). +3. It is strongly recommended installing Intel MKL for potentially better performance. +4. Please be aware that MKL is throttled on AMD platforms. Performance comparisons can be seen for + example [here](https://github.com/flame/blis/blob/master/docs/Performance.md). If you have AMD CPUs please collect + more knowledge to determine which linear algebra library is more suitable. -## Toolsets +### Toolsets A number of new features from new standards are utilized. To compile the binary, a compiler that supports **C++20** is required. GCC 11, Clang 13, MSVC 14.3, Intel compilers and later version of those compilers are tested with the source code. -On Windows, Visual Studio 2022 with Intel oneAPI toolkit is recommended. Alternatively, [WinLibs](http://winlibs.com/) -can be used if GCC compilers are preferred. +On Windows, Visual Studio with Intel oneAPI toolkit is recommended. +Alternatively, [WinLibs](http://winlibs.com/) can be used if GCC compilers are preferred. -On other platforms (Linux and macOS), simply use GCC (at least version 10) which comes with a valid Fortran -compiler. Clang can also be used for C/CPP code, but since Clang and GCC have different supports for C++20, successful +On other platforms (Linux and macOS), simply use GCC which comes with a valid Fortran compiler. +Clang can also be used for C/CPP code, but since Clang and GCC have different supports for C++20, successful compilation is not guaranteed with Clang. -## Obtain Source Code +### Obtain Source Code Download the source code archive from GitHub [Releases](https://github.com/TLCFEM/suanPan/releases) or the latest [code](https://github.com/TLCFEM/suanPan/archive/master.zip). -## Configure and Compile +### Configure and Compile The manual compilation is not difficult in general. The CI/CD configuration files can be referred to if you wish. Please check [this](https://github.com/TLCFEM/suanPan/tree/dev/.github/workflows) page. Here some general guidelines are given. -### Visual Studio +#### Windows (Visual Studio) A solution file is provided under `MSVC/suanPan` folder. There are two configurations: -1. `Debug`: Assume no available Fortran compiler, all Fortran related libraries are provided as precompiled DLLs. Use - OpenBLAS for linear algebra. Multithreading disabled. Visualisation disabled. HDF5 support disabled. -2. `Release`: Fortran libraries are configured with Intel compilers. Use MKL for linear algebra. Multithreading enabled. - Visualisation enabled with VTK version 9.2. HDF5 support enabled. CUDA enabled. +1. `Debug`: Assume no available Fortran compiler, all Fortran related libraries are provided as precompiled DLLs. Use + OpenBLAS for linear algebra. Multithreading disabled. Visualisation disabled. HDF5 support disabled. +2. `Release`: Fortran libraries are configured with Intel compilers. Use MKL for linear algebra. Multithreading enabled. + Visualisation enabled with VTK version 9.2. HDF5 support enabled. CUDA enabled. This [repository](https://github.com/TLCFEM/prebuilds) contains some precompiled libraries used. @@ -63,109 +81,107 @@ open the solution and switch to Debug configuration, ignore all potential warnin To compile `Release` version, please -1. Make sure oneAPI both base and HPC toolkits, as well as VS integration, are installed. Be aware of this issue - if you are using VS 2022: [Microsoft Visual Studio 2022 Version 17.2 and Newer Fails to Integrate with the Intel - Fortran Compiler](https://www.intel.com/content/www/us/en/developer/articles/troubleshooting/vs2022-version-17-2-and-intel-fortran-integration.html). - The MKL is enabled via integrated option `Parallel`. +1. Make sure oneAPI both base and HPC toolkits, as well as VS integration, are installed. + The MKL is enabled via integrated option `Parallel`. -2. Make sure CUDA is installed. The environment variable `$(CUDA_PATH)` is used to locate headers. +2. Make sure CUDA is installed. The environment variable `$(CUDA_PATH)` is used to locate headers. -3. Make sure VTK is available. Then define a system environment variable `$(VTK_DIR)`, which points - to the root folder of VTK library. On my machine, it is +3. Make sure VTK is available. Then define a system environment variable `$(VTK_DIR)`, which points + to the root folder of VTK library. On my machine, it is - ```powershell - VTK_DIR=C:\Program Files\VTK\ - ``` + ```powershell + VTK_DIR=C:\Program Files\VTK\ + ``` - For versions other than 9.2, names of the linked libraries shall be manually changed as they contain version numbers. - Thus, it is not a good idea to switch to a different version. Precompiled VTK library is also available in - this [repository](https://github.com/TLCFEM/prebuilds). + For versions other than 9.2, names of the linked libraries shall be manually changed as they contain version numbers. + Thus, it is not a good idea to switch to a different version. Precompiled VTK library is also available in + this [repository](https://github.com/TLCFEM/prebuilds). -4. Make sure MAGMA is available. Then define a system environment variable `$(MAGMA_DIR)`, which points - to the root folder of MAGMA library. On my machine, it is +4. Make sure MAGMA is available. Then define a system environment variable `$(MAGMA_DIR)`, which points + to the root folder of MAGMA library. On my machine, it is - ```powershell - MAGMA_DIR=C:\Program Files\MAGMA\ - ``` - - You probably need to compile MAGMA yourself. You can manually remove all magma related settings in the solution file - if you don't want to use it. + ```powershell + MAGMA_DIR=C:\Program Files\MAGMA\ + ``` + + You probably need to compile MAGMA yourself. You can manually remove all magma related settings in the solution file + if you don't want to use it. Alternatively, `CMake` can be used to generate solution files if some external packages are not available. -### Ubuntu +#### Ubuntu The following instructions are based on Ubuntu 20.04. [CMake](https://cmake.org/) is used to manage builds. It is recommended to use **CMake** GUI if appropriate. -1. Install necessary tools. +1. Install necessary tools. - ```bash - sudo apt-get install gcc-10 g++-10 gfortran-10 git cmake libomp5 -y - ``` + ```bash + sudo apt-get install gcc-10 g++-10 gfortran-10 git cmake libomp5 -y + ``` -2. Clone the project. +2. Clone the project. - ```bash - git clone -b master https://github.com/TLCFEM/suanPan.git - ``` + ```bash + git clone -b master https://github.com/TLCFEM/suanPan.git + ``` -3. Create build folder and configure via CMake. The default configuration disables parallelism `-DBUILD_MULTITHREAD=OFF` - and enables HDF5 via bundled library `-DUSE_HDF5=ON`. Please - check [`Option.cmake`](https://github.com/TLCFEM/suanPan/blob/dev/Option.cmake) file or use GUI for available - options. +3. Create build folder and configure via CMake. The default configuration disables parallelism `-DBUILD_MULTITHREAD=OFF` + and enables HDF5 via bundled library `-DUSE_HDF5=ON`. Please + check [`Option.cmake`](https://github.com/TLCFEM/suanPan/blob/dev/Option.cmake) file or use GUI for available + options. - ```bash - cd suanPan && mkdir build && cd build - cmake ../ - ``` + ```bash + cd suanPan && mkdir build && cd build + cmake ../ + ``` -4. Invoke `make`. +4. Invoke `make`. - ```bash - make -j4 - ``` + ```bash + make -j4 + ``` Check the following recording. [![asciicast](https://asciinema.org/a/418406.svg)](https://asciinema.org/a/418406) -#### Install VTK +##### Install VTK Ubuntu official repository does not (Fedora does!) contain the latest VTK library. It's better to compile it manually. -1. Install OpenGL first, as well as compilers if necessary. +1. Install OpenGL first, as well as compilers if necessary. - ```bash - sudo apt install gcc-10 g++-10 gfortran-10 libglu1-mesa-dev freeglut3-dev mesa-common-dev libglvnd-dev - ``` + ```bash + sudo apt install gcc-10 g++-10 gfortran-10 libglvnd-dev + ``` -2. Obtain VTK source code and unpack. +2. Obtain VTK source code and unpack. - ```bash - wget https://www.vtk.org/files/release/9.1/VTK-9.1.0.tar.gz - tar -xf VTK-9.1.0.tar.gz - ``` + ```bash + wget https://www.vtk.org/files/release/9.1/VTK-9.1.0.tar.gz + tar -xf VTK-9.1.0.tar.gz + ``` -3. Create folder for building VTK. +3. Create folder for building VTK. - ```bash - mkdir VTK-build && cd VTK-build - ``` + ```bash + mkdir VTK-build && cd VTK-build + ``` -4. Configure and compile VTK library. If necessary, installation destination can be modified. Here static libraries are - built. +4. Configure and compile VTK library. If necessary, installation destination can be modified. Here static libraries are + built. - ```bash - cmake -DCMAKE_BUILD_TYPE=Release -DBUILD_SHARED_LIBS=OFF -DCMAKE_INSTALL_PREFIX=../VTK-out ../VTK-9.1.0 - make install -j4 - ``` + ```bash + cmake -DCMAKE_BUILD_TYPE=Release -DBUILD_SHARED_LIBS=OFF -DCMAKE_INSTALL_PREFIX=../VTK-out ../VTK-9.1.0 + make install -j4 + ``` -5. Now obtain `suanPan` source code and unpack it. To configure it with VTK support, users may use the following - flag `-DUSE_VTK=ON`. If `FindVTK` is presented and `VTK` is installed to default location, there is no need - to provide the variable `VTK_DIR`, otherwise point it to the `lib/cmake/vtk-9.1` folder. +5. Now obtain `suanPan` source code and unpack it. To configure it with VTK support, users may use the following + flag `-DUSE_VTK=ON`. If `FindVTK` is presented and `VTK` is installed to default location, there is no need + to provide the variable `VTK_DIR`, otherwise point it to the `lib/cmake/vtk-9.1` folder. -#### Install MKL +##### Install MKL The provided CMake configuration covers both `oneMKL` and `Intel MKL 2020`. Please note MKL is included in oneAPI toolkit starting from 2021, which has a different folder structure compared to Intel Parallel Studio. @@ -174,40 +190,40 @@ The following guide is a manual installation is based on Ubuntu terminal using t See [this page](https://www.intel.com/content/www/us/en/develop/documentation/installation-guide-for-intel-oneapi-toolkits-linux/top/installation/install-using-package-managers/apt.html) for details. -1. Add repository. To summarise, - - ```bash - wget https://apt.repos.intel.com/intel-gpg-keys/GPG-PUB-KEY-INTEL-SW-PRODUCTS.PUB - sudo apt-key add GPG-PUB-KEY-INTEL-SW-PRODUCTS.PUB - echo "deb https://apt.repos.intel.com/oneapi all main" | sudo tee /etc/apt/sources.list.d/oneAPI.list - ``` - -2. Install the package. - - ```bash - sudo apt update && sudo apt install intel-oneapi-mkl-devel -y - ``` - -3. Now compile `suanPan` by enabling MKL via option `-DUSE_MKL=ON`. The corresponding `MKLROOT` shall be assigned, for - example `-DMKLROOT=/opt/intel/oneapi/mkl/latest/`, depending on the installation location. The configuration used - for snap is the following one. - - ```bash - -DCMAKE_INSTALL_PREFIX= - -DCMAKE_BUILD_TYPE=Release - -DBUILD_MULTITHREAD=ON - -DUSE_HDF5=ON - -DUSE_VTK=ON - -DVTK_DIR=$CRAFT_PART_BUILD/lib/cmake/vtk-9.2/ - -DUSE_MKL=ON - -DMKLROOT=/opt/intel/oneapi/mkl/latest - -DUSE_INTEL_OPENMP=OFF - -DLINK_DYNAMIC_MKL=OFF - ``` +1. Add repository. To summarise, + + ```bash + wget https://apt.repos.intel.com/intel-gpg-keys/GPG-PUB-KEY-INTEL-SW-PRODUCTS.PUB + sudo apt-key add GPG-PUB-KEY-INTEL-SW-PRODUCTS.PUB + echo "deb https://apt.repos.intel.com/oneapi all main" | sudo tee /etc/apt/sources.list.d/oneAPI.list + ``` + +2. Install the package. + + ```bash + sudo apt update && sudo apt install intel-oneapi-mkl-devel -y + ``` + +3. Now compile `suanPan` by enabling MKL via option `-DUSE_MKL=ON`. The corresponding `MKLROOT` shall be assigned, for + example `-DMKLROOT=/opt/intel/oneapi/mkl/latest/`, depending on the installation location. The configuration used + for snap is the following one. + + ```bash + -DCMAKE_INSTALL_PREFIX= + -DCMAKE_BUILD_TYPE=Release + -DBUILD_MULTITHREAD=ON + -DUSE_HDF5=ON + -DUSE_VTK=ON + -DVTK_DIR=$CRAFT_PART_BUILD/lib/cmake/vtk-9.2/ + -DUSE_MKL=ON + -DMKLROOT=/opt/intel/oneapi/mkl/latest + -DUSE_INTEL_OPENMP=OFF + -DLINK_DYNAMIC_MKL=OFF + ``` -### Fedora +#### Fedora -#### VTK +##### VTK Fedora offers the latest VTK library, simply install it. @@ -215,7 +231,7 @@ Fedora offers the latest VTK library, simply install it. sudo dnf install vtk-devel ``` -#### MKL +##### MKL Intel also provides a repository to install MKL via `dnf`. See [this page](https://www.intel.com/content/www/us/en/develop/documentation/installation-guide-for-intel-oneapi-toolkits-linux/top/installation/install-using-package-managers/yum-dnf-zypper.html) @@ -250,7 +266,7 @@ sudo dnf install intel-oneapi-mkl-devel The source can be compiled with VTK and MKL enabled. -### macOS +#### macOS The following guide is based on macOS Big Sur (11). diff --git a/docs/Basic/Obtain.md b/docs/Basic/Obtain.md index 4393bbfd6a..9a47868fee 100644 --- a/docs/Basic/Obtain.md +++ b/docs/Basic/Obtain.md @@ -2,7 +2,7 @@ ## Docker Image -A docker image is available at [Docker Hub](https://hub.docker.com/repository/docker/tlcfem/suanpan). To use it, +A docker image is available at [Docker Hub](https://hub.docker.com/r/tlcfem/suanpan). To use it, docker needs to be installed first. See [this page](https://docs.docker.com/get-docker/) for details. Once docker is installed, it is possible to pull the image via: @@ -27,7 +27,7 @@ sp One can also attach volume to the container to access the files in the host machine. This may be the main use case. -And then run the file inside the container. +Then one can run the file inside the container as follows. ```bash docker run -it --rm -v /path/to/host/folder:/path/to/container/folder tlcfem/suanpan @@ -56,7 +56,7 @@ For older versions or other flavours of Linux, successful execution is not guara Please consider compiling the binaries manually. In order to enable `CUDA` backed solvers, the program shall be compiled locally with preinstalled external libraries. -See this page [Compile](Compile.md). +See [this](Compile.md) page. Currently, the following package managers can be used to install the program. @@ -98,10 +98,9 @@ Then it is possible to use `suanpan` to invoke the application. ## Execute Program -By default, the `AVX` support is turned on to utilize CPU capability. For CPUs that do not support `AVX`, the +By default, the `AVX2` support is turned on to utilize CPU capability. For CPUs that do not support `AVX2`, the application **cannot** be successfully executed. Users can either compile the program by themselves or request a -specific version by filing an issue. Processors that do not support `AVX` may be too slow to perform HPC based -simulations. +specific version by filing an issue. The name of the executable is `suanPan`, however, snap/chocolatey/scoop will create shim executable named as `suanpan`. Depending on how the application is installed, one may use `suanpan` or `suanPan` to invoke the application. @@ -115,8 +114,9 @@ do so, users can, for example, in Windows, use the following command. set OMP_NUM_THREADS=6 ``` -On Linux, the dynamic loading path need to be set so that dynamic libraries such as `libtbb.so` can be successfully -found. If the application is installed via snap/apt/dnf, it is automatically done. +On Linux, the dynamic loading path needs to be set so that dynamic libraries such as `libtbb.so` can be successfully +found. +If the application is installed via `snap`/`apt`/`dnf`, it is automatically done. ```bash # current path contains suanPan @@ -266,8 +266,8 @@ It provides syntax highlighting and code completion. ## Sublime Text Workspace -I personally use [Sublime Text](https://www.sublimetext.com/) as my model editor. Other tools -like [Atom](https://atom.io/) and [VS Code](https://code.visualstudio.com/) can also be used. +I personally use [Sublime Text](https://www.sublimetext.com/) as my model editor. +Other tools like [VS Code](https://code.visualstudio.com/) can also be used. ### Syntax Highlighting @@ -370,19 +370,19 @@ The application itself does **not** write any files to folders other than the cu There are some exceptions though. -1. If the [`terminal`](../Collection/Process/terminal.md) command is used, one can change files in the file system. -2. If one decides to download new versions via the bundled updater, the archive is downloaded to the current working - directory. The updater is not always bundled. +1. If the [`terminal`](../Collection/Process/terminal.md) command is used, one can change files in the file system. +2. If one decides to download new versions via the bundled updater, the archive is downloaded to the current working + directory. The updater is not always bundled. The script `suanPan.sh` writes the following files to the system. -1. `$HOME/.local/share/applications/suanPan.desktop` -2. `$HOME/.local/bin/suanpan` -3. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-build` -4. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-completions` -5. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-syntax` +1. `$HOME/.local/share/applications/suanPan.desktop` +2. `$HOME/.local/bin/suanpan` +3. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-build` +4. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-completions` +5. `$HOME/.config/sublime-text/Packages/User/suanPan.sublime-syntax` The script `AddAssociation.bat` changes the following settings. -1. Associate `*.sp` and `*.supan` files with the program. -2. Copy configuration files to default folder if Sublime Text is installed. +1. Associate `*.sp` and `*.supan` files with the program. +2. Copy configuration files to default folder if Sublime Text is installed. diff --git a/docs/Basic/Performance.md b/docs/Basic/Performance.md index 91d91ff98b..18fcf8db3b 100644 --- a/docs/Basic/Performance.md +++ b/docs/Basic/Performance.md @@ -27,20 +27,20 @@ Users are encouraged to `perf` the performance of various analysis types. Here are some tips that may improve the performance. -1. If the analysis is known to be linear elastic, use `set linear_system true` to skip convergence test and iteration. - Note the analysis should be both material and geometric linear. -2. If the global system is known to be symmetric, use `set symm_mat true` to use a symmetric storage. - Analyses involving 1D materials are mostly (**_not always_**) symmetric. - Analyses involving 2D and 3D materials are mostly (**_not always_**) **_not_** symmetric. -3. Consider a proper stepping strategy. A fixed stepping size may be unnecessarily expensive. - A proper adaptive stepping strategy can significantly improve the performance. -4. Prefer a dense solver over a sparse solver if the system is small. - A dense solver is generally faster than a sparse solver for small systems. -5. Prefer a mixed-precision algorithm `set precision mixed` over a full-precision algorithm if the system is large. - A mixed-precision algorithm is generally faster than a full-precision algorithm for large systems. - See following for details. -6. The performance of various sparser solver can vary significantly. - It is recommended to try different solvers to find the best one. +1. If the analysis is known to be linear elastic, use `set linear_system true` to skip convergence test and iteration. + Note the analysis should be both material and geometric linear. +2. If the global system is known to be symmetric, use `set symm_mat true` to use a symmetric storage. + Analyses involving 1D materials are mostly (**_not always_**) symmetric. + Analyses involving 2D and 3D materials are mostly (**_not always_**) **_not_** symmetric. +3. Consider a proper stepping strategy. A fixed stepping size may be unnecessarily expensive. + A proper adaptive stepping strategy can significantly improve the performance. +4. Prefer a dense solver over a sparse solver if the system is small. + A dense solver is generally faster than a sparse solver for small systems. +5. Prefer a mixed-precision algorithm `set precision mixed` over a full-precision algorithm if the system is large. + A mixed-precision algorithm is generally faster than a full-precision algorithm for large systems. + See following for details. +6. The performance of various sparser solver can vary significantly. + It is recommended to try different solvers to find the best one. ## Mixed-Precision Algorithm diff --git a/docs/Basic/Structure.md b/docs/Basic/Structure.md index bc79f3a886..815c08bc3f 100644 --- a/docs/Basic/Structure.md +++ b/docs/Basic/Structure.md @@ -2,9 +2,9 @@ The default parser accepts a **three-part** structure. They are: -1. Model Properties Setup -2. Analysis Properties Setup -3. Post-processing +1. Model Properties Setup +2. Analysis Properties Setup +3. Post-processing The previous cantilever beam example is used here to explain the structure. The model is shown as follows. diff --git a/docs/Collection/Configure/step.md b/docs/Collection/Configure/step.md index 0eee014672..c114b9437d 100644 --- a/docs/Collection/Configure/step.md +++ b/docs/Collection/Configure/step.md @@ -5,7 +5,7 @@ Please refer to the specific type of steps for details. For any steps available, a default **asymmetric** **banded** dense storage is used. This storage scheme fits most problems. The LAPACK driver used is `_gbsv()`. The main reason behind such a choice stems from two aspects. -1. For 2D and 3D problems, most material models have asymmetric stiffness moduli. The global stiffness matrix is then - asymmetric. -2. If the problem shows softening behaviour, the stiffness matrix is not always positive definite, the symmetric solver - fails to solve such a matrix. +1. For 2D and 3D problems, most material models have asymmetric stiffness moduli. The global stiffness matrix is then + asymmetric. +2. If the problem shows softening behaviour, the stiffness matrix is not always positive definite, the symmetric solver + fails to solve such a matrix. diff --git a/docs/Collection/Define/bc.md b/docs/Collection/Define/bc.md index 685c0bbbdc..de1b42d4b5 100644 --- a/docs/Collection/Define/bc.md +++ b/docs/Collection/Define/bc.md @@ -28,22 +28,22 @@ grouppenaltybc (1) (2) (3...) ## Remark -1. Both `fix` and `fix2` serve the same purpose but with different approaches. The `fix` command modifies the - corresponding main diagonal term by multiplying a large number, for example $$10^8$$. The `fix2` command erase the - column and row of target DoF and set the main diagonal to unity. In both case, the corresponding right hand side - entry is erased. -2. The `fix` and `penaltybc` commands is computationally efficient but leads to an ill-conditioned matrix. This may not - be a problem for direct solvers but will greatly affect the performance of iterative solvers. The penalty number can - be controlled by [`set`](../Process/set.md) command via `constraint_multiplier` option. -3. The `fix2` and `multiplierbc` commands requires more operations but the final matrix is well conditioned. -4. The performance difference is almost negligible. Either one can be used with direct solvers. The error won't - accumulate as there is a special mechanism to prevent it. -5. The DoF identifier `(2)` takes the following string input: `1`, `2`, `3`, `4`, `5`, `6`, `pinned`, `encastre` - , `xsymm`, `ysymm`, `zsymm` and the corresponding initials `p`, `e`, `x`, `y`, `z`. The names do not actually reflect - their meaning, instead, following DoFs would be restrained when string input is given. - 1. `pinned`: 1 2 3 - 2. `encastre`: 1 2 3 4 5 6 - 3. `xsymm`: 1 5 6 - 4. `ysymm`: 2 4 6 - 5. `zsymm`: 3 4 5 -6. The nontrivial Dirichlet boundary condition is treated as displacement load. +1. Both `fix` and `fix2` serve the same purpose but with different approaches. The `fix` command modifies the + corresponding main diagonal term by multiplying a large number, for example $$10^8$$. The `fix2` command erase the + column and row of target DoF and set the main diagonal to unity. In both case, the corresponding right hand side + entry is erased. +2. The `fix` and `penaltybc` commands is computationally efficient but leads to an ill-conditioned matrix. This may not + be a problem for direct solvers but will greatly affect the performance of iterative solvers. The penalty number can + be controlled by [`set`](../Process/set.md) command via `constraint_multiplier` option. +3. The `fix2` and `multiplierbc` commands requires more operations but the final matrix is well conditioned. +4. The performance difference is almost negligible. Either one can be used with direct solvers. The error won't + accumulate as there is a special mechanism to prevent it. +5. The DoF identifier `(2)` takes the following string input: `1`, `2`, `3`, `4`, `5`, `6`, `pinned`, `encastre`, + `xsymm`, `ysymm`, `zsymm` and the corresponding initials `p`, `e`, `x`, `y`, `z`. The names do not actually reflect + their meaning, instead, following DoFs would be restrained when string input is given. + 1. `pinned`: 1 2 3 + 2. `encastre`: 1 2 3 4 5 6 + 3. `xsymm`: 1 5 6 + 4. `ysymm`: 2 4 6 + 5. `zsymm`: 3 4 5 +6. The nontrivial Dirichlet boundary condition is treated as displacement load. diff --git a/docs/Collection/Define/expression.md b/docs/Collection/Define/expression.md index 8b74673821..bdd9e9e56b 100644 --- a/docs/Collection/Define/expression.md +++ b/docs/Collection/Define/expression.md @@ -51,12 +51,12 @@ Thus, it ***cannot*** be used in models that require automatic computation of de ## Remarks -1. The variables in the expression need to be explicitly given as the arguments. - It can be either unquoted or quoted by `"`. -2. Multiple variables must be separated by vertical bar `|`. -3. The expression can be given as a string or as a file name. The program tries to load the file first. If the file - does not exist, the program tries to parse the string as an expression. -4. No whitespace (',', ' ', etc.) is allowed in any arguments. +1. The variables in the expression need to be explicitly given as the arguments. + It can be either unquoted or quoted by `"`. +2. Multiple variables must be separated by vertical bar `|`. +3. The expression can be given as a string or as a file name. The program tries to load the file first. If the file + does not exist, the program tries to parse the string as an expression. +4. No whitespace (',', ' ', etc.) is allowed in any arguments. `exprtk` provides very powerful functionalities. It is possible to apply logics and control flows in the expression. diff --git a/docs/Collection/Define/load.md b/docs/Collection/Define/load.md index 4725730eda..5a796911d2 100644 --- a/docs/Collection/Define/load.md +++ b/docs/Collection/Define/load.md @@ -138,14 +138,14 @@ load refload (1) (2) (3) (4) (5...) ## Remarks -1. The leading `load` keyword can often be omitted for simplicity. -2. The `acceleration` is by default applied to all active nodes in the model if `[5...]` is not assigned. -3. The true load magnitude is the product of nominal magnitude and amplitude. This is similar to ABAQUS. -4. The multipoint displacement control algorithm [`MPDC`](../../Library/Solver/MPDC.md) is automatically enabled if - a `displacement` or `groupdisplacement` is used. -5. Optionally, the displacement can be applied by using [`MPC`](../../Library/Constraint/MPC.md) constraint. -6. The multipoint displacement control algorithm [`MPDC`](../../Library/Solver/MPDC.md) is automatically enabled if - a `supportdisplacement`, `supportvelocity` and/or `supportacceleration` are used. +1. The leading `load` keyword can often be omitted for simplicity. +2. The `acceleration` is by default applied to all active nodes in the model if `[5...]` is not assigned. +3. The true load magnitude is the product of nominal magnitude and amplitude. This is similar to ABAQUS. +4. The multipoint displacement control algorithm [`MPDC`](../../Library/Solver/MPDC.md) is automatically enabled if + a `displacement` or `groupdisplacement` is used. +5. Optionally, the displacement can be applied by using [`MPC`](../../Library/Constraint/MPC.md) constraint. +6. The multipoint displacement control algorithm [`MPDC`](../../Library/Solver/MPDC.md) is automatically enabled if + a `supportdisplacement`, `supportvelocity` and/or `supportacceleration` are used. **It must be noted that nodal displacement loads are only valid for one single step.** This means, if a displacement load is defined within a step, it will be activated for that step only. diff --git a/docs/Collection/Define/node.md b/docs/Collection/Define/node.md index f3a9b90da3..21e7e62364 100644 --- a/docs/Collection/Define/node.md +++ b/docs/Collection/Define/node.md @@ -74,13 +74,13 @@ The following quantities can be recorded using the commands similar to `plainrec ### Remarks -1. For static analysis, normally only displacement `U` and resistance `RF` are activated. Thus, recording other - quantities returns trivial results. -2. If the required quantity is not active, the output will be empty. -3. The damping and inertial forces are collected from all the elements in the model. It **must** be noted that the - recorded values do **not** include any contributions that do not stem from elements. For example, the damping - force given by global damping models cannot be split to individual elements; thus it is not reflected in the - nodal damping force. This design is necessary as one may wish to separate contributions from various sources apart. -4. To record **global** damping and inertial forces that account for the total force, use `GDF`, `GDF1`, `GDF2`, - `GDF3`, `GDF4`, `GDF5`, `GDF6`, `GIF`, `GIF1`, `GIF2`, `GIF3`, `GIF4`, `GIF5`, `GIF6`, which stand for global - damping force and global inertial force. +1. For static analysis, normally only displacement `U` and resistance `RF` are activated. Thus, recording other + quantities returns trivial results. +2. If the required quantity is not active, the output will be empty. +3. The damping and inertial forces are collected from all the elements in the model. It **must** be noted that the + recorded values do **not** include any contributions that do not stem from elements. For example, the damping + force given by global damping models cannot be split to individual elements; thus it is not reflected in the + nodal damping force. This design is necessary as one may wish to separate contributions from various sources apart. +4. To record **global** damping and inertial forces that account for the total force, use `GDF`, `GDF1`, `GDF2`, + `GDF3`, `GDF4`, `GDF5`, `GDF6`, `GIF`, `GIF1`, `GIF2`, `GIF3`, `GIF4`, `GIF5`, `GIF6`, which stand for global + damping force and global inertial force. diff --git a/docs/Collection/Process/materialtest.md b/docs/Collection/Process/materialtest.md index bb2f600317..8c76a3ad8b 100644 --- a/docs/Collection/Process/materialtest.md +++ b/docs/Collection/Process/materialtest.md @@ -27,10 +27,10 @@ materialTest3D (1) (2...7) (8) [9...] ## Remarks -1. The increment size could be either positive or negative. -2. The loading direction reverses after given numbers of steps. -3. The strain-stress history would be saved to `RESULT.txt`. If `HDF5` is used, the result would be additionally saved - to `RESULT.h5`. Besides, a `gnuplot` file named `RESULT.plt` will be generated. +1. The increment size could be either positive or negative. +2. The loading direction reverses after given numbers of steps. +3. The strain-stress history would be saved to `RESULT.txt`. If `HDF5` is used, the result would be additionally saved + to `RESULT.h5`. Besides, a `gnuplot` file named `RESULT.plt` will be generated. ## Usage diff --git a/docs/Collection/Process/materialtestbyload.md b/docs/Collection/Process/materialtestbyload.md index 67e27234fe..62afa09a24 100644 --- a/docs/Collection/Process/materialtestbyload.md +++ b/docs/Collection/Process/materialtestbyload.md @@ -27,5 +27,5 @@ materialTestByLoad3D (1) (2...7) (8) [9...] ## Remarks -1. The Newton-Raphson method is implemented to solve the corresponding strain increments. - Thus, softening models should not be tested in this way. +1. The Newton-Raphson method is implemented to solve the corresponding strain increments. + Thus, softening models should not be tested in this way. diff --git a/docs/Collection/Process/sectiontest.md b/docs/Collection/Process/sectiontest.md index fdf1239a0e..a27b0153e7 100644 --- a/docs/Collection/Process/sectiontest.md +++ b/docs/Collection/Process/sectiontest.md @@ -26,12 +26,12 @@ sectionTest3D (1) (2...4) (5) [6...] ## Remarks -1. The increment size could be either positive or negative. -2. The loading direction reverses after given numbers of steps. -3. The strain-stress history would be saved to `RESULT.txt`. If `HDF5` is used, the result would be additionally saved - to `RESULT.h5`. -4. The deformation vector consists of axial deformation, rotation about strong axis, rotation about weak axis. 1D, 2D - and 3D sections have the first, first two and all three components respectively. +1. The increment size could be either positive or negative. +2. The loading direction reverses after given numbers of steps. +3. The strain-stress history would be saved to `RESULT.txt`. If `HDF5` is used, the result would be additionally saved + to `RESULT.h5`. +4. The deformation vector consists of axial deformation, rotation about strong axis, rotation about weak axis. 1D, 2D + and 3D sections have the first, first two and all three components respectively. ## Example diff --git a/docs/Collection/Process/set.md b/docs/Collection/Process/set.md index 0d5dbd336c..cfd52e5024 100644 --- a/docs/Collection/Process/set.md +++ b/docs/Collection/Process/set.md @@ -146,17 +146,17 @@ All available settings are summarised in the following table. Some empirical guidance can be concluded as follows. -1. For most cases, the asymmetric banded storage with full precision solver is the most general option. -2. The best performance is obtained by using symmetric banded storage, if the (effective) stiffness matrix is guaranteed - to be positive definite, users shall use it as a priority. -3. The mixed precision algorithm often gives the most significant performance boost for full storage with `CUDA` solver. - It outperforms the full precision algorithm when the size of system exceeds several thousands. -4. The `SPIKE` solver is slightly slower than the conventional `LAPACK` implementations. -5. The `SuperLU` solver is slower than the `MUMPS` solver. The multithreaded `SuperLU` performs LU factorization in - parallel but forward/back substitution in sequence. -6. The `PARDISO` direct solver and `FGMRES` iterative solver are provided by `MKL`. -7. The `MUMPS` solver supports both symmetric and asymmetric algorithms. One can use `set symm_mat true` - or `set symm_mat false`. +1. For most cases, the asymmetric banded storage with full precision solver is the most general option. +2. The best performance is obtained by using symmetric banded storage, if the (effective) stiffness matrix is guaranteed + to be positive definite, users shall use it as a priority. +3. The mixed precision algorithm often gives the most significant performance boost for full storage with `CUDA` solver. + It outperforms the full precision algorithm when the size of system exceeds several thousands. +4. The `SPIKE` solver is slightly slower than the conventional `LAPACK` implementations. +5. The `SuperLU` solver is slower than the `MUMPS` solver. The multithreaded `SuperLU` performs LU factorization in + parallel but forward/back substitution in sequence. +6. The `PARDISO` direct solver and `FGMRES` iterative solver are provided by `MKL`. +7. The `MUMPS` solver supports both symmetric and asymmetric algorithms. One can use `set symm_mat true` + or `set symm_mat false`. ### Iterative System Solver diff --git a/docs/Developer/C/material.md b/docs/Developer/C/material.md index c5868e5bef..109fd9548f 100644 --- a/docs/Developer/C/material.md +++ b/docs/Developer/C/material.md @@ -36,27 +36,27 @@ state may or may not be the converged state, thus may or may not be kept in an i Some remarks to explain those operations. -1. In operation `*info=0`, memory shall be allocated to store two states and other relevant variables. Since it is not - known to the main executable how large the memory is required, this has to be done by the library using whatever - methods to allocate. -2. In operation `*info=2`, trial state is updated based on trial strain and current state (as an incremental form is - implemented). This operation will be called in a static analysis, or by elements that only computes strains. Before - calling this operation, the trial strain will be written to the corresponding location of allocated memory some place - defined in `*data`. -3. In operation `*info=3`, trial state is updated based on trial strain, trial strain rate and current state (as an - incremental form is implemented). This operation will be called by elements that computes both strains and strain - rates and pass them to material models. Often, the resulting stiffness and damping matrices shall be computed. Before - calling this operation, the trial strain and the trial strain rate will be written to the corresponding location of - allocated memory some place defined in `*data`. -4. In operation `*info=4`, we simply overwrite current state with trial state as the trial state now converges after - several iterations. -5. In operation `*info=5`, when this operation is called, convergence is not met, so we overwrite trial state with - current state and update the system with a smaller increment of (pseudo) time. -6. In operation `*info=6`, all state variables and history variables shall be reverted to initial (potential zero) - state. -7. In operation `*info=7`, all model parameters shall be checked to see if a proper material model can be defined. This - cannot be done in the main executable although the command is processed in the main executable, in which all - parameters will be read as double inputs and stored in a raw double array in `*data`. +1. In operation `*info=0`, memory shall be allocated to store two states and other relevant variables. Since it is not + known to the main executable how large the memory is required, this has to be done by the library using whatever + methods to allocate. +2. In operation `*info=2`, trial state is updated based on trial strain and current state (as an incremental form is + implemented). This operation will be called in a static analysis, or by elements that only computes strains. Before + calling this operation, the trial strain will be written to the corresponding location of allocated memory some place + defined in `*data`. +3. In operation `*info=3`, trial state is updated based on trial strain, trial strain rate and current state (as an + incremental form is implemented). This operation will be called by elements that computes both strains and strain + rates and pass them to material models. Often, the resulting stiffness and damping matrices shall be computed. Before + calling this operation, the trial strain and the trial strain rate will be written to the corresponding location of + allocated memory some place defined in `*data`. +4. In operation `*info=4`, we simply overwrite current state with trial state as the trial state now converges after + several iterations. +5. In operation `*info=5`, when this operation is called, convergence is not met, so we overwrite trial state with + current state and update the system with a smaller increment of (pseudo) time. +6. In operation `*info=6`, all state variables and history variables shall be reverted to initial (potential zero) + state. +7. In operation `*info=7`, all model parameters shall be checked to see if a proper material model can be defined. This + cannot be done in the main executable although the command is processed in the main executable, in which all + parameters will be read as double inputs and stored in a raw double array in `*data`. In a typical analysis flow, `*info=0` will be called first to initialise memory, then `*info=7` will be called to valid parameters. If it fails, `*info=1` will be called. Otherwise, either `*info=2` or `*info=3` will be called to update diff --git a/docs/Developer/CPP/element.md b/docs/Developer/CPP/element.md index f04407b02c..37c0f7cc2d 100644 --- a/docs/Developer/CPP/element.md +++ b/docs/Developer/CPP/element.md @@ -148,12 +148,12 @@ void initialize_base(const shared_ptr&) override final; A number of tasks are performed in the default initialization. -1. Check if all involved nodes are active, if not, the element will be disabled. -2. Check the current number of DoFs of each involved node, if it is smaller than that required by the current element, - then reset it. -3. Check if there is a valid and active material/section model based on the corresponding tag provided in the - constructor, if not, the element will be disabled. -4. On the second run, check again if all nodes are active, if not, the element will be disabled. +1. Check if all involved nodes are active, if not, the element will be disabled. +2. Check the current number of DoFs of each involved node, if it is smaller than that required by the current element, + then reset it. +3. Check if there is a valid and active material/section model based on the corresponding tag provided in the + constructor, if not, the element will be disabled. +4. On the second run, check again if all nodes are active, if not, the element will be disabled. ## General Procedure @@ -187,11 +187,11 @@ The latter three manage states. Normally it is necessary to call the correspondi material/section models if the implemented element itself does not store history variables. As the name suggests, we need to update the trial state in the first method. A general procedure would be: -1. obtain nodal displacement/velocity vector by calling for example `get_trial_displacement()`, -2. compute strain at each integration point, -3. update material models using new trial strains, -4. get material response and form element resistance and stiffness matrix. If necessary, mass/damping matrix shall be - updated according to the new trial state. +1. obtain nodal displacement/velocity vector by calling for example `get_trial_displacement()`, +2. compute strain at each integration point, +3. update material models using new trial strains, +4. get material response and form element resistance and stiffness matrix. If necessary, mass/damping matrix shall be + updated according to the new trial state. ### If You Decide To Manage States In Your Way @@ -223,25 +223,25 @@ virtual const mat& get_initial_secant() const; As a general guideline, here are some conventions to follow: -1. It is not recommended using the second approach, that is, managing internal variables at derived class level, unless - all methods are carefully implemented. -2. All state updates, including all history variables, shall only happen in the `update_status()` method, as all get - methods are declared as `const`. -3. It is sometimes useful to update trial strain related variables only in `update_status()` and compute responses in - the corresponding getters. In that case, a `const_cast` is required. By doing so, developers must clearly know what - the operation means. A typical example would be, for example, the modified Newton algorithm or - the [`BFGS`](../../Library/Solver/BFGS.md) method, in which `update_status()` will only be called once and getters of - resistances and matrices would be called several times for each iteration in each sub-step. Splitting updater and - getters apart will for sure save some computation efforts but is also error-prone. -4. Normally the damping matrix and the mass matrix shall only be defined as functions of current state at most --- if - they are not constants. Essentially, they cannot be functions of trial strain/displacement if a quadratic convergence - rate shall be preserved. -5. If the stiffness matrix is constant throughout the analysis, it is recommended to use - function `ConstantStiffness(ElementData*)` to declare such a feature in order to save some memory. -6. If the damping matrix is constant throughout the analysis, it is recommended to use - function `ConstantDamping(ElementData*)` to declare such a feature in order to save some memory. -7. If the mass matrix is constant throughout the analysis, it is recommended to use - function `ConstantMass(ElementData*)` to declare such a feature in order to save some memory. +1. It is not recommended using the second approach, that is, managing internal variables at derived class level, unless + all methods are carefully implemented. +2. All state updates, including all history variables, shall only happen in the `update_status()` method, as all get + methods are declared as `const`. +3. It is sometimes useful to update trial strain related variables only in `update_status()` and compute responses in + the corresponding getters. In that case, a `const_cast` is required. By doing so, developers must clearly know what + the operation means. A typical example would be, for example, the modified Newton algorithm or + the [`BFGS`](../../Library/Solver/BFGS.md) method, in which `update_status()` will only be called once and getters of + resistances and matrices would be called several times for each iteration in each sub-step. Splitting updater and + getters apart will for sure save some computation efforts but is also error-prone. +4. Normally the damping matrix and the mass matrix shall only be defined as functions of current state at most --- if + they are not constants. Essentially, they cannot be functions of trial strain/displacement if a quadratic convergence + rate shall be preserved. +5. If the stiffness matrix is constant throughout the analysis, it is recommended to use + function `ConstantStiffness(ElementData*)` to declare such a feature in order to save some memory. +6. If the damping matrix is constant throughout the analysis, it is recommended to use + function `ConstantDamping(ElementData*)` to declare such a feature in order to save some memory. +7. If the mass matrix is constant throughout the analysis, it is recommended to use + function `ConstantMass(ElementData*)` to declare such a feature in order to save some memory. ## Record Response @@ -263,6 +263,6 @@ remaining is automatically handled by the base class. For different dimensions, here are some very simple elements implemented for reference. -1. 1D --- `Spring01` a spring element based on infinitesimal displacement. -2. 2D --- `ElementExample` a three-node triangle plain membrane element. -3. 3D --- `C3D4` a four-node tetragon using one-node integration. \ No newline at end of file +1. 1D --- `Spring01` a spring element based on infinitesimal displacement. +2. 2D --- `ElementExample` a three-node triangle plain membrane element. +3. 3D --- `C3D4` a four-node tetragon using one-node integration. \ No newline at end of file diff --git a/docs/Developer/CPP/material.md b/docs/Developer/CPP/material.md index ba6c6b3a2e..e2dbdbe1d0 100644 --- a/docs/Developer/CPP/material.md +++ b/docs/Developer/CPP/material.md @@ -2,10 +2,10 @@ ## Things to Know -1. There is no need to write wrappers. Various wrappers are available to wrap 3D material models for 1D and 2D - applications. -2. Unless the 2D material model is formulated directly in the 2D space, for example the plane stress space (such as the - Barlat-Lian model), developers are not encouraged to write any 2D versions of 3D models. +1. There is no need to write wrappers. Various wrappers are available to wrap 3D material models for 1D and 2D + applications. +2. Unless the 2D material model is formulated directly in the 2D space, for example the plane stress space (such as the + Barlat-Lian model), developers are not encouraged to write any 2D versions of 3D models. ## Main Tasks of a Material Model diff --git a/docs/Example/Structural/Dynamics/bouncing-of-a-ball.md b/docs/Example/Structural/Dynamics/bouncing-of-a-ball.md index 28bd667b75..77c235184d 100644 --- a/docs/Example/Structural/Dynamics/bouncing-of-a-ball.md +++ b/docs/Example/Structural/Dynamics/bouncing-of-a-ball.md @@ -1,4 +1,4 @@ -# [★★★☆☆] Bouncing of A Ball +# [★★★☆☆] Bouncing of a Ball In this example we show the application of the [`RigidWall`](../../../Library/Constraint/RigidWall.md) and [`RestitutionWall`](../../../Library/Constraint/RestitutionWall.md) constraints. It is also possible to define a diff --git a/docs/Example/Structural/Dynamics/dynamic-analysis-of-a-portal-frame.md b/docs/Example/Structural/Dynamics/dynamic-analysis-of-a-portal-frame.md index 5bd166d222..2bcd48dfa5 100644 --- a/docs/Example/Structural/Dynamics/dynamic-analysis-of-a-portal-frame.md +++ b/docs/Example/Structural/Dynamics/dynamic-analysis-of-a-portal-frame.md @@ -1,6 +1,6 @@ -# [★★☆☆☆] Dynamic Analysis of A Portal Frame +# [★★☆☆☆] Dynamic Analysis of a Portal Frame -A portal frame is analyzed using viscous damper as energy dissipater. +A portal frame is analyzed using viscous damper as energy dissipator. The model script can be downloaded. [dynamic-analysis-of-a-portal-frame.zip](dynamic-analysis-of-a-portal-frame.zip) diff --git a/docs/Example/Structural/Dynamics/process-ground-motion.ipynb b/docs/Example/Structural/Dynamics/process-ground-motion.ipynb new file mode 100644 index 0000000000..1eba26d9b6 --- /dev/null +++ b/docs/Example/Structural/Dynamics/process-ground-motion.ipynb @@ -0,0 +1,334 @@ +{ + "cells": [ + { + "cell_type": "markdown", + "id": "2bac110441a87485", + "metadata": {}, + "source": [ + "# [★★☆☆☆] Process Ground Motion for Dynamic Analysis\n", + "\n", + "In this example, we mainly introduce and discuss different methods to introduce ground motion into response history analyses.\n", + "For different methods, different considerations shall be taken into account.\n", + "\n", + "The ground motion record can be one of acceleration, velocity, or displacement.\n", + "Depending on how it is collected, it could either be a processed or raw record.\n", + "Typically, seismometer collects acceleration, and velocity and displacement are derived from acceleration.\n", + "We assume that analysts are given accelerograms. \n", + "\n", + "## EOM\n", + "\n", + "The equation of motion is often written as follows, assuming linear elasticity.\n", + "\n", + "$$\n", + "\\mathbf{M}\\ddot{\\mathbf{u}}+\\mathbf{C}\\dot{\\mathbf{u}}+\\mathbf{K}\\mathbf{u}=\\mathbf{f}.\n", + "$$\n", + "\n", + "To incorporate ground motion in the form of acceleration, one can choose the following methods.\n", + "\n", + "1. Apply the acceleration on the upper structure, in the form of inertial force, with the assist of the global mass matrix.\n", + " This method involves the global mass matrix $$\\mathbf{M}$$, and assumes $$\\mathbf{M}$$ is constant, or at least remains constant within the time step.\n", + "2. Apply the ground motion on the supports.\n", + " This method mimics the real-world situation.\n", + " The ground motion is applied on the supports, and the structure is allowed to move freely.\n", + " Thus, final results contain rigid body motion.\n", + " Furthermore, since conventionally displacement is used as the primary unknown, the given acceleration shall be converted to displacement.\n", + "\n", + "## Ground Motion as Inertial Force\n", + "\n", + "The inertial force can be formulated as follows.\n", + "\n", + "$$\n", + "\\mathbf{f}_g=\\mathbf{M}\\ddot{\\mathbf{u}}_g.\n", + "$$\n", + "\n", + "However, when applied in the form of force, there is a risk of unintended spurious force.\n", + "One can refer to the paper [10.1080/13632469.2024.2372814](https://doi.org/10.1080/13632469.2024.2372814) for more details.\n", + "The conclusion is that, one shall always process the ground motion based on the time step size used in response history analysis, regardless of the source of the ground motion, processed or raw.\n", + "\n", + "## Ground Motion as Support Displacement\n", + "\n", + "The ground motion can also be applied on the supports.\n", + "In this case, the ground motion is converted to displacement.\n", + "But how?\n", + "Naturally, acceleration shall be integrated twice to obtain displacement.\n", + "However, the integration process is not straightforward.\n", + "Furthermore, not any integration method is suitable for this purpose.\n", + "\n", + "## Example" + ] + }, + { + "cell_type": "code", + "id": "b83c3a5400383b5b", + "metadata": {}, + "source": [ + "import json\n", + "\n", + "import numpy as np\n", + "\n", + "with open('process-ground-motion.json', 'r') as f:\n", + " record = json.load(f)\n", + "\n", + "waveform = np.array(record['raw_data'], dtype=float)\n", + "waveform /= max(abs(waveform))\n", + "dt = record['time_interval']\n", + "duration = dt * len(waveform)" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "47e2d06e33a1ece1", + "metadata": {}, + "source": [ + "Let's peek at the ground motion record." + ] + }, + { + "cell_type": "code", + "id": "ee96e41253792b14", + "metadata": {}, + "source": [ + "import matplotlib.pyplot as plt\n", + "\n", + "\n", + "def plot_waveform(_dt, _waveform):\n", + " plt.plot(np.arange(0, _dt * len(_waveform), _dt), _waveform)\n", + " plt.xlabel('Time [s]')\n", + " plt.ylabel('Acceleration')\n", + " plt.grid(True)\n", + "\n", + "\n", + "plot_waveform(dt, waveform)" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "f21bbcac7d2819", + "metadata": {}, + "source": [ + "Let's also check the frequency content of the ground motion.\n", + "It can be done by Fourier transform." + ] + }, + { + "cell_type": "code", + "id": "4d18e3fe7266dedc", + "metadata": {}, + "source": [ + "from scipy.fft import rfft, rfftfreq\n", + "\n", + "\n", + "def plot_freq(_dt, _waveform):\n", + " n = len(_waveform)\n", + " frequencies = rfftfreq(n, _dt)\n", + " fft_values = 2 * np.abs(rfft(_waveform)) / n\n", + "\n", + " plt.plot(frequencies, fft_values)\n", + " plt.xlabel('Frequency [Hz]')\n", + " plt.ylabel('Amplitude')\n", + " plt.yscale('log')\n", + " plt.grid(True)\n", + "\n", + "\n", + "plot_freq(dt, waveform)" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "fc88a67deac98aec", + "metadata": {}, + "source": [ + "It appears that the provided ground motion has been filtered using a band-pass filter.\n", + "The frequency content above 50 Hz is significantly reduced.\n", + "\n", + "This ground motion is sampled at 200 Hz, with an interval of 0.005 s.\n", + "If it is used in a response history analysis with a time step of 0.005 s, the ground motion shall be processed.\n", + "The de facto method is to perform linear interpolation." + ] + }, + { + "cell_type": "code", + "id": "475dd4f999d3f48d", + "metadata": {}, + "source": [ + "from scipy.interpolate import interp1d\n", + "\n", + "interp_func = interp1d(np.arange(0, duration, dt), waveform)\n", + "\n", + "\n", + "def upsample(n):\n", + " _dt = dt / n\n", + " return _dt, interp_func(np.arange(0, duration - dt, _dt))\n", + "\n", + "\n", + "interp_dt, interp_waveform = upsample(10)\n", + "plot_freq(interp_dt, interp_waveform)" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "f3aeb8c74eca6a1b", + "metadata": {}, + "source": [ + "From the graph, one shall see that the interpolated acceleration contain significantly large components beyond the original 100 Hz.\n", + "It is thus concluded that ***significant spurious response may be present***.\n", + "\n", + "The ground motion can also be converted to displacement by using cumulative integration." + ] + }, + { + "cell_type": "code", + "id": "17f94ee4505e4a29", + "metadata": {}, + "source": [ + "from scipy.integrate import cumulative_trapezoid\n", + "\n", + "disp = cumulative_trapezoid(cumulative_trapezoid(waveform, dx=dt), dx=dt)\n", + "\n", + "plot_waveform(dt, disp)" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "b57fe55bbaba866d", + "metadata": {}, + "source": [ + "What acceleration would such a displacement produce if the Newmark method is used?" + ] + }, + { + "cell_type": "code", + "id": "1d22160efc1c4057", + "metadata": {}, + "source": [ + "def newmark(displacement, interval, gamma=.5, beta=.25):\n", + " acceleration: np.ndarray = np.zeros_like(displacement)\n", + " velocity: np.ndarray = np.zeros_like(displacement)\n", + " for i in range(1, len(displacement)):\n", + " acceleration[i] = (displacement[i] - displacement[i - 1] - interval * velocity[i - 1] - (\n", + " 0.5 - beta) * interval ** 2 * acceleration[i - 1]) / beta / interval ** 2\n", + " velocity[i] = velocity[i - 1] + (1.0 - gamma) * interval * acceleration[i - 1] + gamma * interval * \\\n", + " acceleration[i]\n", + " return acceleration\n", + "\n", + "\n", + "acc = newmark(disp, dt)\n", + "\n", + "plot_freq(dt, waveform)\n", + "plot_freq(dt, acc)\n", + "plt.legend(['Original', 'Trap -> Newmark'])\n", + "pass" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "84885ff8", + "metadata": {}, + "source": [ + "In the above, we use Newmark method to compute the acceleration that corresponds to the integrated displacement.\n", + "By comparing two accelerations records (original ground motion and converted from the integrated displacement), we could see some slight differences.\n", + "Such differences appear to be negligible.\n", + "\n", + "However, if the acceleration is linearly interpolated, what would such a process bring?" + ] + }, + { + "cell_type": "code", + "id": "df1e929947c8320e", + "metadata": {}, + "source": [ + "from scipy.integrate import cumulative_simpson\n", + "\n", + "\n", + "def double_convert(_dt, _waveform):\n", + " return newmark(cumulative_simpson(cumulative_simpson(_waveform, dx=_dt), dx=_dt), _dt)\n", + "\n", + "\n", + "plot_freq(interp_dt, interp_waveform)\n", + "plot_freq(interp_dt, double_convert(interp_dt, interp_waveform))\n", + "plt.legend(['Original', 'Trap -> Newmark'])\n", + "pass" + ], + "outputs": [], + "execution_count": null + }, + { + "cell_type": "markdown", + "id": "e07d9b3d", + "metadata": {}, + "source": [ + "It seems the high frequency noise is significantly larger if the acceleration is integrated using an arbitrary integration method.\n", + "Let's choose a different upsampling rate." + ] + }, + { + "metadata": {}, + "cell_type": "code", + "source": [ + "interp_dt, interp_waveform = upsample(2)\n", + "plot_freq(interp_dt, interp_waveform)\n", + "plot_freq(interp_dt, double_convert(interp_dt, interp_waveform))\n", + "plt.legend(['Original', 'Trap -> Newmark'])\n", + "pass" + ], + "id": "f3e9640253d19d9e", + "outputs": [], + "execution_count": null + }, + { + "metadata": {}, + "cell_type": "markdown", + "source": [ + "From the figure, one can assert that, if the structure responds to 200 Hz signals, the response could be significant as by choosing to integrate the acceleration using a method that is different from the one used in response history analysis (here, the Newmark method).\n", + "\n", + "## Remarks\n", + "\n", + "In the above example, we have demonstrated two things.\n", + "\n", + "1. As discussed in [10.1080/13632469.2024.2372814](https://doi.org/10.1080/13632469.2024.2372814), when ground motion is applied in the form of inertial force, linear interpolation of acceleration introduces high frequency noise, the amplitude of which could be relatively large. This would introduce spurious responses.\n", + "2. When ground motion is applied in the form of support displacement, an inconsistent integration method that is used to integrate acceleration to displacement could introduce high frequency noise as well, if the integration method is different from the one used in response history analysis. This type of spurious response is not significant if the acceleration is not linear interpolated.\n", + "\n", + "In conclusion, analysts shall be aware of two things.\n", + "\n", + "1. Linear interpolation is bad. It shall be avoided, or at least cannot be used alone.\n", + "2. When converting acceleration to displacement, or vice versa, the integration method shall be consistent with the one used in response history analysis.\n", + "\n", + "No matter what, the applied load, in the form of either inertial force or support displacement, shall be processed based on the time step size used in response history analysis." + ], + "id": "2eb2d719943420ae" + } + ], + "metadata": { + "kernelspec": { + "display_name": "Python 3", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.11.9" + } + }, + "nbformat": 4, + "nbformat_minor": 5 +} diff --git a/docs/Example/Structural/Dynamics/process-ground-motion.json b/docs/Example/Structural/Dynamics/process-ground-motion.json new file mode 100644 index 0000000000..1ec2d3e148 --- /dev/null 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 \ No newline at end of file diff --git a/docs/Example/Structural/Dynamics/process-ground-motion.md b/docs/Example/Structural/Dynamics/process-ground-motion.md new file mode 100644 index 0000000000..3615554240 --- /dev/null +++ b/docs/Example/Structural/Dynamics/process-ground-motion.md @@ -0,0 +1,256 @@ +# [★★☆☆☆] Process Ground Motion for Dynamic Analysis + +In this example, we mainly introduce and discuss different methods to introduce ground motion into response history analyses. +For different methods, different considerations shall be taken into account. + +The ground motion record can be one of acceleration, velocity, or displacement. +Depending on how it is collected, it could either be a processed or raw record. +Typically, seismometer collects acceleration, and velocity and displacement are derived from acceleration. +We assume that analysts are given accelerograms. + +## EOM + +The equation of motion is often written as follows, assuming linear elasticity. + +$$ +\mathbf{M}\ddot{\mathbf{u}}+\mathbf{C}\dot{\mathbf{u}}+\mathbf{K}\mathbf{u}=\mathbf{f}. +$$ + +To incorporate ground motion in the form of acceleration, one can choose the following methods. + +1. Apply the acceleration on the upper structure, in the form of inertial force, with the assist of the global mass matrix. + This method involves the global mass matrix $$\mathbf{M}$$, and assumes $$\mathbf{M}$$ is constant, or at least remains constant within the time step. +2. Apply the ground motion on the supports. + This method mimics the real-world situation. + The ground motion is applied on the supports, and the structure is allowed to move freely. + Thus, final results contain rigid body motion. + Furthermore, since conventionally displacement is used as the primary unknown, the given acceleration shall be converted to displacement. + +## Ground Motion as Inertial Force + +The inertial force can be formulated as follows. + +$$ +\mathbf{f}_g=\mathbf{M}\ddot{\mathbf{u}}_g. +$$ + +However, when applied in the form of force, there is a risk of unintended spurious force. +One can refer to the paper [10.1080/13632469.2024.2372814](https://doi.org/10.1080/13632469.2024.2372814) for more details. +The conclusion is that, one shall always process the ground motion based on the time step size used in response history analysis, regardless of the source of the ground motion, processed or raw. + +## Ground Motion as Support Displacement + +The ground motion can also be applied on the supports. +In this case, the ground motion is converted to displacement. +But how? +Naturally, acceleration shall be integrated twice to obtain displacement. +However, the integration process is not straightforward. +Furthermore, not any integration method is suitable for this purpose. + +## Example + + +```python +import json + +import numpy as np + +with open('process-ground-motion.json', 'r') as f: + record = json.load(f) + +waveform = np.array(record['raw_data'], dtype=float) +waveform /= max(abs(waveform)) +dt = record['time_interval'] +duration = dt * len(waveform) +``` + +Let's peek at the ground motion record. + + +```python +import matplotlib.pyplot as plt + + +def plot_waveform(_dt, _waveform): + plt.plot(np.arange(0, _dt * len(_waveform), _dt), _waveform) + plt.xlabel('Time [s]') + plt.ylabel('Acceleration') + plt.grid(True) + + +plot_waveform(dt, waveform) +``` + + + +![png](process-ground-motion_files/process-ground-motion_3_0.png) + + + +Let's also check the frequency content of the ground motion. +It can be done by Fourier transform. + + +```python +from scipy.fft import rfft, rfftfreq + + +def plot_freq(_dt, _waveform): + n = len(_waveform) + frequencies = rfftfreq(n, _dt) + fft_values = 2 * np.abs(rfft(_waveform)) / n + + plt.plot(frequencies, fft_values) + plt.xlabel('Frequency [Hz]') + plt.ylabel('Amplitude') + plt.yscale('log') + plt.grid(True) + + +plot_freq(dt, waveform) +``` + + + +![png](process-ground-motion_files/process-ground-motion_5_0.png) + + + +It appears that the provided ground motion has been filtered using a band-pass filter. +The frequency content above 50 Hz is significantly reduced. + +This ground motion is sampled at 200 Hz, with an interval of 0.005 s. +If it is used in a response history analysis with a time step of 0.005 s, the ground motion shall be processed. +The de facto method is to perform linear interpolation. + + +```python +from scipy.interpolate import interp1d + +interp_func = interp1d(np.arange(0, duration, dt), waveform) + + +def upsample(n): + _dt = dt / n + return _dt, interp_func(np.arange(0, duration - dt, _dt)) + + +interp_dt, interp_waveform = upsample(10) +plot_freq(interp_dt, interp_waveform) +``` + + + +![png](process-ground-motion_files/process-ground-motion_7_0.png) + + + +From the graph, one shall see that the interpolated acceleration contain significantly large components beyond the original 100 Hz. +It is thus concluded that ***significant spurious response may be present***. + +The ground motion can also be converted to displacement by using cumulative integration. + + +```python +from scipy.integrate import cumulative_trapezoid + +disp = cumulative_trapezoid(cumulative_trapezoid(waveform, dx=dt), dx=dt) + +plot_waveform(dt, disp) +``` + + + +![png](process-ground-motion_files/process-ground-motion_9_0.png) + + + +What acceleration would such a displacement produce if the Newmark method is used? + + +```python +def newmark(displacement, interval, gamma=.5, beta=.25): + acceleration: np.ndarray = np.zeros_like(displacement) + velocity: np.ndarray = np.zeros_like(displacement) + for i in range(1, len(displacement)): + acceleration[i] = (displacement[i] - displacement[i - 1] - interval * velocity[i - 1] - ( + 0.5 - beta) * interval ** 2 * acceleration[i - 1]) / beta / interval ** 2 + velocity[i] = velocity[i - 1] + (1.0 - gamma) * interval * acceleration[i - 1] + gamma * interval * \ + acceleration[i] + return acceleration + + +acc = newmark(disp, dt) + +plot_freq(dt, waveform) +plot_freq(dt, acc) +plt.legend(['Original', 'Trap -> Newmark']) +pass +``` + + + +![png](process-ground-motion_files/process-ground-motion_11_0.png) + + + +In the above, we use Newmark method to compute the acceleration that corresponds to the integrated displacement. +By comparing two accelerations records (original ground motion and converted from the integrated displacement), we could see some slight differences. +Such differences appear to be negligible. + +However, if the acceleration is linearly interpolated, what would such a process bring? + + +```python +from scipy.integrate import cumulative_simpson + + +def double_convert(_dt, _waveform): + return newmark(cumulative_simpson(cumulative_simpson(_waveform, dx=_dt), dx=_dt), _dt) + + +plot_freq(interp_dt, interp_waveform) +plot_freq(interp_dt, double_convert(interp_dt, interp_waveform)) +plt.legend(['Original', 'Trap -> Newmark']) +pass +``` + + + +![png](process-ground-motion_files/process-ground-motion_13_0.png) + + + +It seems the high frequency noise is significantly larger if the acceleration is integrated using an arbitrary integration method. +Let's choose a different upsampling rate. + + +```python +interp_dt, interp_waveform = upsample(2) +plot_freq(interp_dt, interp_waveform) +plot_freq(interp_dt, double_convert(interp_dt, interp_waveform)) +plt.legend(['Original', 'Trap -> Newmark']) +pass +``` + + + +![png](process-ground-motion_files/process-ground-motion_15_0.png) + + + +From the figure, one can assert that, if the structure responds to 200 Hz signals, the response could be significant as by choosing to integrate the acceleration using a method that is different from the one used in response history analysis (here, the Newmark method). + +## Remarks + +In the above example, we have demonstrated two things. + +1. As discussed in [10.1080/13632469.2024.2372814](https://doi.org/10.1080/13632469.2024.2372814), when ground motion is applied in the form of inertial force, linear interpolation of acceleration introduces high frequency noise, the amplitude of which could be relatively large. This would introduce spurious responses. +2. When ground motion is applied in the form of support displacement, an inconsistent integration method that is used to integrate acceleration to displacement could introduce high frequency noise as well, if the integration method is different from the one used in response history analysis. This type of spurious response is not significant if the acceleration is not linear interpolated. + +In conclusion, analysts shall be aware of two things. + +1. Linear interpolation is bad. It shall be avoided, or at least cannot be used alone. +2. 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a/docs/Example/Structural/Dynamics/response-history-analysis-of-an-elastic-coupled-wall.md +++ b/docs/Example/Structural/Dynamics/response-history-analysis-of-an-elastic-coupled-wall.md @@ -1,4 +1,4 @@ -# [★★★☆☆] Response History Analysis of An Elastic Coupled Wall +# [★★★☆☆] Response History Analysis of an Elastic Coupled Wall In this page, we perform eigen analysis and response history analysis of an elastic coupled wall model. diff --git a/docs/Library/Constraint/FixedLength.gif b/docs/Library/Constraint/FixedLength.gif new file mode 100644 index 0000000000000000000000000000000000000000..c1dfd2f242516289ca9c11e2aa6f6262744f6d60 GIT binary patch literal 219264 zcmd43WmuJK+b%i?0TmPxDFu-Z!2l@{0qIsL5fJILXap%~kcL4Iy1P4tL6?+-NOw0X z`+f%CbiUtwzvEqd?e*>T!$0%TUvoU?b>=N9F2cqAQW+fy+l9f{gq&G zc@BSST*<(0$9mtJ^oGnmp-4`Vl&iE)h$tl3g#x9u%Y~k$-e6IXH>qRfP?J#i;*~Oc zYLxNZtVB*P?x|6Mrd>VDeN9cfmgg3qY40e|v1yZB7k_TvK*g$J;@NHBg4DEYx-S(k zppZtzs>~%C%l;_vo=^k@qXHF+${oI76|;KwM?v?c5(E{})yz`ge(E8jkfdOge`;JS 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b/docs/Library/Constraint/FixedLength.md index cc589ca4d3..7a59e4bd22 100644 --- a/docs/Library/Constraint/FixedLength.md +++ b/docs/Library/Constraint/FixedLength.md @@ -6,6 +6,19 @@ border stiffness matrix. The constraint is satisfied exactly. The `FixedLength2D` and `FixedLength3D` constraints behave similar to the `Tie` element, the nonlinear constraint is implemented via Lagrange multiplier method. +The position $$\mathbf{x}$$ of a given node can be expressed as the summation of coordinate $$\mathbf{d}$$ and +displacement $$\mathbf{u}$$. + +$$ +\mathbf{x}=\mathbf{d}+\mathbf{u}. +$$ + +The constraint enforces that + +$$ +\Big|\mathbf{x}_i-\mathbf{x}_j\Big|=\Big|\mathbf{d}_i-\mathbf{d}_j\Big|. +$$ + It shall not be used with global damping models in dynamic analysis since it alters the frequency distribution, leading to an unintended damping response. Only damping models that do not depend on system properties can be used. @@ -20,4 +33,58 @@ constraint fixedlength3d (1) (2) (3) # (1) int, unique constraint tag # (2) int, node tag # (3) int, node tag -``` \ No newline at end of file +``` + +## Example + +![two cantilever beams](FixedLength.gif) + +A vertical load is applied to the free end of the top beam. +The free ends of the two beams are connected by a `FixedLength2D` constraint. + +```text +node 1 0 0 +node 2 1 0 +node 11 .2 0 +node 12 .4 0 +node 13 .6 0 +node 14 .8 0 + +node 3 1 -.2 +node 4 2 -.2 +node 21 1.2 -.2 +node 22 1.4 -.2 +node 23 1.6 -.2 +node 24 1.8 -.2 + +material Elastic1D 1 10 + +element EB21 1 1 11 12 1 1 1 +element EB21 2 11 12 12 1 1 1 +element EB21 3 12 13 12 1 1 1 +element EB21 4 13 14 12 1 1 1 +element EB21 5 14 2 12 1 1 1 + +element EB21 6 3 21 12 1 1 1 +element EB21 7 21 22 12 1 1 1 +element EB21 8 22 23 12 1 1 1 +element EB21 9 23 24 12 1 1 1 +element EB21 10 24 4 12 1 1 1 + +fix2 1 P 1 4 + +constraint FixedLength2D 2 2 3 + +cload 1 0 10 2 2 + +step static 1 1 +set ini_step_size 1E-2 +set fixed_step_size true +set symm_mat false + +converger RelIncreDisp 1 1E-10 10 1 + +analyze + +exit +``` diff --git a/docs/Library/Constraint/MaxForce.gif b/docs/Library/Constraint/MaxForce.gif new file mode 100644 index 0000000000000000000000000000000000000000..196a37d2023bed90c9d0d5947de94339bc59a594 GIT binary patch literal 210606 zcmd43WmJ`WzcxDQ6cLaH>28%0k#3L%0hN*l5s?(7ySqCklkVSM| zde*bnv-dt{zh|7U4jF?F+}H2QzofJTFQ1+!d^hM66GY8wLC5tLk3^J|R{Q!I^aBI} zse#%-pw3RL%gfF+Y!Ihl#C z8s$f_!0+IpVo@)sl&STu?V(t_wr!oZZ8-^zivEY;hhhn|oa*<5ASQG$V21|%6P;x zMAS;8b$s+)+IS^1nEX zpA0#Jaw;}0)<^FAz%R-FoR(9~+^3h3TZf2J!Q^9^xK{o{5q-O`{-Pq#hlI)3z7679 zW#o)%{IUslp&d?<{SQPVB~+~WB=n8nXK7nS;FHT*d**p04hSmc6@WmFA+;VcwOWSn z+{5#u!R@hGm5v^fifS)B6WYV$GxE#pA%$fbC2b|;W#HVLgv3Nk$Kar}HZ!Yt@oC`l z(tL16qLY7?g-e3Im8Y$POGs!039X8P*pu?C*qqpan!>aQulE%Reyxxg6BTKQzrDi? 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`L=FtF^*a@cn`8;Sy5+$$!6nkAc40+X7( z?C>c&DvmQ%KM9G>rGSZk`xfg~@zcd*&xljj=&0a|Wz9|$_-v{DBZt*ur6=c0?a^9} z>y1njwk2(ic)Ic`9MoXFFZwOPH+bc$_YWew~o&*=m8JtGB&U&uey@ z8H1~ZI>3bF?8(plK#{z%o2x^=D##_<(n;|36=%VWE9+&}_uz{iT`#spsoL|o9d{-N zG{#d#e>CAfFk7U)&`J?S3Fmae=+c%J{^NI7X2FAcaprn5OH>&SaYq|W#uRFNfoD4J z#f6=M@ft2l7`p(8;F`g-V+xbiq#+b*l0?XhUZ7h-T%LTn%VG*{dR;U=#|tSBNFn~x zP#uC74^oM|RGVlx%snVJQCZ&p31onvJosrZM$f|C%+EnbpxmTGv;uF&bN%B(L7~gr zW8d=R{7;ZOABG^Bke|4WIH7O4E|HMM%csErO@Zn~HIn^XOeTyV-M)zy+o4T?j36NS zTRJV(+C5Psop7PDbaKi)B*ia^-;;bZ80q)g-*`9rmeLv_Ja!iBW0&$F_n9XeL2i@hK#J_t6uF%( znp(R#i7kVSj|H^)VR=(4wklPFHfg*qPConLCx1EoAV8+!v7g!#eYGv z{_~Lc_-=nE?of$X;kVGQ7rQ&WB981@WDuz+dK=86cP6t0YX2P)L?y;BiU~vr zh>Rf?u6wY^69*1?2qbGDtk%Sy~gj0{k8PiByA1mK8_&&O#JgAvx) zS+H#-@^lLH-+#`??>VbX&J(x7TLcO%P^s(dS8*!Zq-wRo@n#p9hQMs`PS1X%#>gyJ zh(mOpyw%(|1q`dVqQ|bsD#5K{<@t_-Il>M}oPdO$SOgAvpALlo&KBhXu|gxEnx(gL zSZRB|(CMmDJE{Vd(~e65DAzcM+<_hPxSaQDOCG%7vJ_4#K@H8m_hKlg7I65lcHB=y z#<8vlVC2`k=5H=1!Ep}pf(s3)USy=2X&{^y_U)}+7U(_ep`G53LMK_3cwY49`?O}} s^Jg%{qVwUZX*x7~4{?Riu#vb9B(%3;$hN&s(^U0xOV literal 0 HcmV?d00001 diff --git a/docs/Library/Constraint/MaxForce.md b/docs/Library/Constraint/MaxForce.md new file mode 100644 index 0000000000..dde2afac95 --- /dev/null +++ b/docs/Library/Constraint/MaxForce.md @@ -0,0 +1,71 @@ +# MaxForce + +The `MaxForce` constraint applies a [`FixedLength`](FixedLength.md) constraint to a pair of nodes. +The constraint is only active when the force is below a specified threshold. + +## Syntax + +``` +maxforce2d (1) (2) (3) (4) +maxforce3d (1) (2) (3) (4) +constraint maxforce2d (1) (2) (3) (4) +constraint maxforce3d (1) (2) (3) (4) +# (1) int, unique constraint tag +# (2) int, node tag +# (3) int, node tag +# (4) double, magnitude of constraint force +``` + +## Example + +![two cantilever beams](MaxForce.gif) + +A vertical displacement is applied to the free end of the top beam. +The free ends of the two beams are connected by a `MaxForce2D` constraint. + +```text +node 1 0 0 +node 2 1 0 +node 11 .2 0 +node 12 .4 0 +node 13 .6 0 +node 14 .8 0 + +node 3 1 -.2 +node 4 2 -.2 +node 21 1.2 -.2 +node 22 1.4 -.2 +node 23 1.6 -.2 +node 24 1.8 -.2 + +material Elastic1D 1 10 1E-4 + +element EB21 1 1 11 12 1 1 1 +element EB21 2 11 12 12 1 1 1 +element EB21 3 12 13 12 1 1 1 +element EB21 4 13 14 12 1 1 1 +element EB21 5 14 2 12 1 1 1 + +element EB21 6 3 21 12 1 1 1 +element EB21 7 21 22 12 1 1 1 +element EB21 8 22 23 12 1 1 1 +element EB21 9 23 24 12 1 1 1 +element EB21 10 24 4 12 1 1 1 + +fix2 1 P 1 4 + +constraint MaxForce2D 2 2 3 4.0 + +displacement 1 0 .3 2 2 + +step dynamic 1 1 +set ini_step_size 1E-2 +set fixed_step_size true +set symm_mat false + +converger RelIncreDisp 1 1E-10 10 1 + +analyze + +exit +``` diff --git a/docs/Library/Constraint/MaximumGap2D.md b/docs/Library/Constraint/MaximumGap2D.md index f474c3b50d..dc94d85be5 100644 --- a/docs/Library/Constraint/MaximumGap2D.md +++ b/docs/Library/Constraint/MaximumGap2D.md @@ -15,7 +15,7 @@ constraint MaximumGap2D (1) (2) (3) (4) This is a conditional constraint that limits the distance between two nodes, viz., $$ -\left|\mathbf{x}_i+\mathbf{u}_i\-\mathbf{x}_j-\mathbf{u}_j\right|\leq{}D_{max}. +\left|\mathbf{d}_i+\mathbf{u}_i-\mathbf{d}_j-\mathbf{u}_j\right|\leq{}D_{max}. $$ The participating DoFs are `1` and `2`. diff --git a/docs/Library/Constraint/MaximumGap3D.md b/docs/Library/Constraint/MaximumGap3D.md index 4ca1ef73fd..908bd81d46 100644 --- a/docs/Library/Constraint/MaximumGap3D.md +++ b/docs/Library/Constraint/MaximumGap3D.md @@ -15,7 +15,7 @@ constraint MaximumGap3D (1) (2) (3) (4) This is a conditional constraint that limits the distance between two nodes, viz., $$ -\left|\mathbf{x}_i+\mathbf{u}_i\-\mathbf{x}_j-\mathbf{u}_j\right|\leq{}D_{max}. +\left|\mathbf{d}_i+\mathbf{u}_i-\mathbf{d}_j-\mathbf{u}_j\right|\leq{}D_{max}. $$ The participating DoFs are `1`, `2` and `3`. diff --git a/docs/Library/Constraint/MinimumGap2D.md b/docs/Library/Constraint/MinimumGap2D.md index 754cf222a4..db54657e44 100644 --- a/docs/Library/Constraint/MinimumGap2D.md +++ b/docs/Library/Constraint/MinimumGap2D.md @@ -15,7 +15,7 @@ constraint MinimumGap2D (1) (2) (3) (4) This is a conditional constraint that limits the distance between two nodes, viz., $$ -\left|\mathbf{x}_i+\mathbf{u}_i\-\mathbf{x}_j-\mathbf{u}_j\right|\geq{}D_{min}. +\left|\mathbf{d}_i+\mathbf{u}_i-\mathbf{d}_j-\mathbf{u}_j\right|\geq{}D_{min}. $$ The participating DoFs are `1` and `2`. diff --git a/docs/Library/Constraint/MinimumGap3D.md b/docs/Library/Constraint/MinimumGap3D.md index aa7616051d..2dfac41fd6 100644 --- a/docs/Library/Constraint/MinimumGap3D.md +++ b/docs/Library/Constraint/MinimumGap3D.md @@ -15,7 +15,7 @@ constraint MinimumGap3D (1) (2) (3) (4) This is a conditional constraint that limits the distance between two nodes, viz., $$ -\left|\mathbf{x}_i+\mathbf{u}_i\-\mathbf{x}_j-\mathbf{u}_j\right|\geq{}D_{min}. +\left|\mathbf{d}_i+\mathbf{u}_i-\mathbf{d}_j-\mathbf{u}_j\right|\geq{}D_{min}. $$ The participating DoFs are `1`, `2`, and `3`. diff --git a/docs/Library/Integrator/BatheTwoStep.md b/docs/Library/Integrator/BatheTwoStep.md index c77e44a74b..2b5e238470 100644 --- a/docs/Library/Integrator/BatheTwoStep.md +++ b/docs/Library/Integrator/BatheTwoStep.md @@ -11,6 +11,10 @@ References: The implementation follows the original algorithm. The only difference is the step size defined in `suanPan` is the mean step size of two sub-step sizes, that is $$\Delta{}t/2$$ in the references. +For further discussions on this type of algorithm, one can check the following references. + +1. [10.1007/s11071-023-09065-7](https://doi.org/10.1007/s11071-023-09065-7) + ## Syntax ``` diff --git a/docs/Library/Material/Material3D/Elastic/MooneyRivlin.md b/docs/Library/Material/Material3D/Elastic/MooneyRivlin.md index c210f314df..76e92d941f 100644 --- a/docs/Library/Material/Material3D/Elastic/MooneyRivlin.md +++ b/docs/Library/Material/Material3D/Elastic/MooneyRivlin.md @@ -10,6 +10,10 @@ $$ where $$A_{10}$$ and $$A_{01}$$ are two material constants and $$K$$ is the bulk modulus. +## References + +1. [10.1007/978-1-4419-1746-1](https://doi.org/10.1007/978-1-4419-1746-1) Chapter 3.5.2.1 + ## Syntax ``` diff --git a/docs/Library/Material/Material3D/Elastic/Yeoh.md b/docs/Library/Material/Material3D/Elastic/Yeoh.md index cb09a89e54..79ba5b5b71 100644 --- a/docs/Library/Material/Material3D/Elastic/Yeoh.md +++ b/docs/Library/Material/Material3D/Elastic/Yeoh.md @@ -40,7 +40,7 @@ The following command shall be used. material Yeoh 1 20 4000 ``` -If density is nonzero, say for example $$\rho=1E-4$$, then the following command shall be used. +If density is nonzero, say for example $$\rho=10^{-4}$$, then the following command shall be used. ``` material Yeoh 1 20 4000 1E-4 diff --git a/docs/Library/Section/SectionNM/NM2D2.md b/docs/Library/Section/SectionNM/NM2D2.md index 46edc621bc..f7094d6e4b 100644 --- a/docs/Library/Section/SectionNM/NM2D2.md +++ b/docs/Library/Section/SectionNM/NM2D2.md @@ -30,8 +30,8 @@ $$ f=1.15p^2+m_s^2+3.67p^2m_s^2-c $$ -where $$p$$ and $$m_s$$ are normalised axial force and moment (about strong axis). The surface is suitable for -I-sections. +where $$p$$ and $$m_s$$ are normalised axial force and moment (about the strong axis). +This surface is suitable for I-sections. ### Option Two @@ -54,8 +54,9 @@ section NM2D2 (1) (2...9) [(10) (11) (12) ...] # (12) double, c_i ``` -In the above command, parameters `(10)`, `(11)` and `(12)` form a triplet and can be appended as many groups as analyst -wishes. The surface is assumed to possess the following form, +In the above command, parameters `(10)`, `(11)` and `(12)` form a triplet and can be appended as many groups as the +analyst wishes. +The surface is assumed to possess the following form, $$ f=\sum_{i=1}^na_ip^{b_i}m_s^{c_i}-d. @@ -68,8 +69,9 @@ syntax as follows. section NM2D2 (1) (2...9) 1.15 2. 0. 1. 0. 2. 3.67 2. 2. ``` -The only validation implemented is the number of triplets. The command takes $$3n$$ parameters and interprets them -accordingly. Please make sure the definition is correct. +The only validation implemented is the number of triplets. +The command takes $$3n$$ parameters and interprets them accordingly. +Please make sure the definition is correct. ## Remarks diff --git a/docs/Library/Section/SectionNM/NM2D3.md b/docs/Library/Section/SectionNM/NM2D3.md index 28bac80013..d3765b00c8 100644 --- a/docs/Library/Section/SectionNM/NM2D3.md +++ b/docs/Library/Section/SectionNM/NM2D3.md @@ -27,8 +27,9 @@ section NM2D3 (1) (2...12) [(13) (14) (15) ...] # (15) double, c_i ``` -In the above command, parameters `(13)`, `(14)` and `(15)` form a triplet and can be appended as many groups as analyst -wishes. The surface is assumed to possess the following form, +In the above command, parameters `(13)`, `(14)` and `(15)` form a triplet and can be appended as many groups as the +analyst wishes. +The surface is assumed to possess the following form, $$ f=\sum_{i=1}^na_ip^{b_i}m_s^{c_i}-d. @@ -40,5 +41,6 @@ For example, the surface $$f=1.15p^2+m_s^2+3.67p^2m_s^2-c$$ can be expressed as section NM2D3 (1) (2...12) 1.15 2. 0. 1. 0. 2. 3.67 2. 2. ``` -The only validation implemented is the number of triplets. The command takes $$3n$$ parameters and interprets them -accordingly. Please make sure the definition is correct. \ No newline at end of file +The only validation implemented is the number of triplets. +The command takes $$3n$$ parameters and interprets them accordingly. +Please make sure the definition is correct. diff --git a/docs/Library/Section/SectionNM/NM3D2.md b/docs/Library/Section/SectionNM/NM3D2.md index cd4946f9fb..6baace6470 100644 --- a/docs/Library/Section/SectionNM/NM3D2.md +++ b/docs/Library/Section/SectionNM/NM3D2.md @@ -31,8 +31,8 @@ $$ f=1.15p^2+m_s^2+m_w^4+3.67p^2m_s^2+3p^6m_w^2+4.65m_s^4m_w^2-c $$ -where $$p$$, $$m_s$$ and $$m_w$$ are normalised axial force and moments about strong and weak axes. -The surface is suitable for I-sections. +where $$p$$, $$m_s$$ and $$m_w$$ are normalised axial force and moments about the strong and weak axes. +This surface is suitable for I-sections. ### Option Two @@ -59,7 +59,8 @@ section NM3D2 (1) (2...11) [(12) (13) (14) (15)...] ``` In the above command, parameters `(12)`, `(13)`, `(14)` and `(15)` form a set of parameters and can be appended as many -groups as analyst wishes. The surface is assumed to possess the following form, +groups as the analyst wishes. +The surface is assumed to possess the following form, $$ f=\sum_{i=1}^na_ip^{b_i}m_s^{c_i}m_w^{d_i}-e. @@ -69,11 +70,18 @@ For example, the previous surface $$f=1.15p^2+m_s^2+m_w^4+3.67p^2m_s^2+3p^6m_w^2 expressed with the second syntax as follows. ``` -section NM3D2 (1) (2...11) 1.15 2. 0. 0. 1. 0. 2. 0. 3.67 2. 2. 0. 3. 6. 0. 2. 4.65 0. 4. 2. +section NM3D2 (1) (2...11) \ +1.15 2. 0. 0. \ +1. 0. 2. 0. \ +1. 0. 0. 4. \ +3.67 2. 2. 0. \ +3. 6. 0. 2. \ +4.65 0. 4. 2. ``` -The only validation implemented is the number of triplets. The command takes $$4n$$ parameters and interprets them -accordingly. Please make sure the definition is correct. +The only validation implemented is the number of triplets. +The command takes $$4n$$ parameters and interprets them accordingly. +Please make sure the definition is correct. ## Remarks diff --git a/docs/Library/Section/SectionNM/NM3D3.md b/docs/Library/Section/SectionNM/NM3D3.md index 85c463ce7c..9aa4d1fc29 100644 --- a/docs/Library/Section/SectionNM/NM3D3.md +++ b/docs/Library/Section/SectionNM/NM3D3.md @@ -30,8 +30,9 @@ section NM3D3 (1) (2...14) [(15) (16) (17) (18)...] # (18) double, d_i ``` -In the above command, parameters `(15)`, `(16)`, `(17)` and `(18)` form a set and can be appended as many groups as analyst -wishes. The surface is assumed to possess the following form, +In the above command, parameters `(15)`, `(16)`, `(17)` and `(18)` form a set and can be appended as many groups as the +analyst wishes. +The surface is assumed to possess the following form, $$ f=\sum_{i=1}^na_ip^{b_i}m_s^{c_i}m_w^{d_i}-e. @@ -40,8 +41,15 @@ $$ For example, the surface $$f=1.15p^2+m_s^2+m_w^4+3.67p^2m_s^2+3p^6m_w^2+4.65m_s^4m_w^2-c$$ can be expressed as follows. ``` -section NM3D3 (1) (2...14) 1.15 2. 0. 0. 1. 0. 2. 0. 3.67 2. 2. 0. 3. 6. 0. 2. 4.65 0. 4. 2. +section NM3D3 (1) (2...14) \ +1.15 2. 0. 0. \ +1. 0. 2. 0. \ +1. 0. 0. 4. \ +3.67 2. 2. 0. \ +3. 6. 0. 2. \ +4.65 0. 4. 2. ``` -The only validation implemented is the number of triplets. The command takes $$4n$$ parameters and interprets them -accordingly. Please make sure the definition is correct. \ No newline at end of file +The only validation implemented is the number of triplets. +The command takes $$4n$$ parameters and interprets them accordingly. +Please make sure the definition is correct. diff --git a/docs/Library/Section/SectionNM/SectionNM.md b/docs/Library/Section/SectionNM/SectionNM.md index ee10cccc69..6e25277d5b 100644 --- a/docs/Library/Section/SectionNM/SectionNM.md +++ b/docs/Library/Section/SectionNM/SectionNM.md @@ -18,7 +18,7 @@ The `SectionNM` takes elemental deformation and resistance (which are local quan and directly compute the force and moment. Loosely speaking, the `SectionNM` is a special model that accounts for two end sections simultaneously. -According to [1], the whole model can be implemented at the element level. +According to [10.1061/JSENDH.STENG-12176](http://dx.doi.org/10.1061/JSENDH.STENG-12176), the whole model can be implemented at the element level. It is chosen to separate the model into the element part (`NMB*` elements) and the section part (`NM2D*` and `NM3D*` sections) for better code organisation. diff --git a/docs/README.md b/docs/README.md index e88fdc2a7e..b98c57ed9d 100644 --- a/docs/README.md +++ b/docs/README.md @@ -30,6 +30,13 @@ implement new ideas within the framework. For reference, I am able to implement within hours. If you have experience in developing new models in any language, you shall be able to do the same. The architecture is continuously evolving to provide a hassle-free platform for researchers to implement new ideas. +Modern programming paradigms for parallel computing have evolved a lot in recent years. +C++ itself has also received a huge number of updates starting from `C++11`. +`suanPan` is basically a practice of modern parallel computing with brand-new language features. +The civil/structural community also needs an update of new tools for efficient numerical analysis. +`suanPan` is designed to offer a concise but highly extensible framework for finite element analysis. +With the assist of `Armadillo`, the syntax of which is expressive, researchers can try out new ideas easily. + ## Where to start? It is not easy to pick up a new finite element analysis tool, but it is not impossible. @@ -62,18 +69,6 @@ examples. You shall be able to have a better understanding of the syntax by chec Here is a complete [table of contents](SUMMARY.md). If you are interested in the architecture of the program, you can check the [slides](ARCH.pdf) I prepared for a talk. -## About - -Many FEM packages are available out there, so why another package? -Commercial packages are great, but may be too expensive for individuals to get access to. -The limited extensibility is another pain in the butt. -Modern programming paradigms for parallel computing have evolved a lot in recent years. -C++ itself has also received a huge number of updates starting from `C++11`. -`suanPan` is basically a practice of modern parallel computing with brand-new language features. -The civil/structural community also needs an update of new tools for efficient numerical analysis. -`suanPan` is designed to offer a concise but highly extensible framework for finite element analysis. -With the assist of `Armadillo`, the syntax of which is expressive, researchers can try out new ideas easily. - ## Contribution You are very welcome to contribute to the application. Please feel free to create feature requests or directly contact diff --git a/docs/SUMMARY.md b/docs/SUMMARY.md index f98399e68d..6738beb378 100644 --- a/docs/SUMMARY.md +++ b/docs/SUMMARY.md @@ -44,6 +44,7 @@ * [triple pendulum](Example/Structural/Dynamics/triple-pendulum.md) * [computing response spectrum](Example/Structural/Dynamics/computing-response-spectrum.md) * [integrate with python](Example/Structural/Dynamics/integrating-preprocessing-with-python.md) + * [process ground motion](Example/Structural/Dynamics/process-ground-motion.md) * Hybrid * [vibration of a displaced beam](Example/Structural/Hybrid/vibration-of-a-displaced-beam.md) * Buckling @@ -128,6 +129,7 @@ * [RigidWall](Library/Constraint/RigidWall.md) * [RestitutionWall](Library/Constraint/RestitutionWall.md) * [FixedLength](Library/Constraint/FixedLength.md) +* [MaxForce](Library/Constraint/MaxForce.md) * [NodeLine](Library/Constraint/NodeLine.md) * [NodeFacet](Library/Constraint/NodeFacet.md) * [Embed2D](Library/Constraint/Embed2D.md) diff --git a/mkdocs.yml b/mkdocs.yml index 6f19992bce..3641708231 100644 --- a/mkdocs.yml +++ b/mkdocs.yml @@ -6,6 +6,7 @@ theme: name: material features: - navigation.tabs + - navigation.footer favicon: suanPan.svg logo: suanPan.svg palette: @@ -65,6 +66,7 @@ plugins: ignore: - docs/Example/Structural/Statics/thin-walled-section.ipynb - docs/Example/Structural/Dynamics/integrating-preprocessing-with-python.ipynb + - docs/Example/Structural/Dynamics/process-ground-motion.ipynb - overwrite_math # - with-pdf: # cover_subtitle: An Open Source, Parallel and Heterogeneous Finite Element Analysis Framework diff --git a/requirements.txt b/requirements.txt index 2cdf5a7d4e..646cae7e34 100644 --- a/requirements.txt +++ b/requirements.txt @@ -1,16 +1,16 @@ django-weasyprint==2.3.0 dload==0.6 h5py==3.11.0 -ipykernel==6.29.4 -jupytext==1.16.2 -matplotlib==3.8.4 +ipykernel==6.29.5 +jupytext==1.16.4 +matplotlib==3.9.2 mdx-truly-sane-lists==1.3 -mike==2.1.1 -mkdocs-awesome-pages-plugin==2.9.2 -mkdocs-jupyter==0.24.7 -mkdocs-material==9.5.21 +mike==2.1.3 +mkdocs-awesome-pages-plugin==2.9.3 +mkdocs-jupyter==0.25.0 +mkdocs-material==9.5.34 mkdocs-with-pdf==0.9.3 -openpyxl==3.1.2 +openpyxl==3.1.5 pandas==2.2.2 recommonmark==0.7.1 -sectionproperties==3.2.1 \ No newline at end of file +sectionproperties==3.3.0 diff --git a/setup.py b/setup.py index b0b7c05d82..d3aa55405d 100644 --- a/setup.py +++ b/setup.py @@ -1,9 +1,10 @@ import os import re import shutil +import sys import tarfile -import urllib.request import zipfile +from urllib.request import urlopen from setuptools import setup @@ -18,28 +19,17 @@ def install(): remove("docs/Doxygen") remove("site") + # 1. download source code archive_name = "suanPan-dev" url = "https://github.com/TLCFEM/suanPan/archive/refs/heads/dev.zip" - with urllib.request.urlopen(url) as response, open( - f"{archive_name}.zip", "wb" - ) as archive: + with urlopen(url) as response, open(f"{archive_name}.zip", "wb") as archive: shutil.copyfileobj(response, archive) with zipfile.ZipFile(f"{archive_name}.zip", "r") as archive: archive.extractall(".") os.remove(f"{archive_name}.zip") - tar_file = "suanPan-linux-openblas-no-avx" - remove(tar_file) - url = f"https://github.com/TLCFEM/suanPan/releases/download/suanPan-v3.3/{tar_file}.tar.gz" - with urllib.request.urlopen(url) as response, open( - f"{tar_file}.tar.gz", "wb" - ) as archive: - shutil.copyfileobj(response, archive) - with tarfile.open(f"{tar_file}.tar.gz", "r:gz") as archive: - archive.extractall(tar_file) - os.remove(f"{tar_file}.tar.gz") - + # 2. generate doxygen documentation os.chdir(archive_name) doxygen_bin = "doxygen" @@ -62,6 +52,32 @@ def install(): remove(archive_name) + # 3. download binary file + if sys.platform.startswith("linux"): + binary_file_name = "suanPan-linux-openblas-no-avx" + binary_file = f"{binary_file_name}.tar.gz" + else: + binary_file_name = "suanPan-win-mkl-vtk" + binary_file = f"{binary_file_name}.zip" + remove(binary_file_name) + + with urlopen("https://github.com/TLCFEM/suanPan") as response: + content = response.read().decode("utf-8") + version_string = re.search(r"suanPan-v\d\.\d(\.\d)?", content).group(0) + + url = f"https://github.com/TLCFEM/suanPan/releases/download/{version_string}/{binary_file}" + with urlopen(url) as response, open(binary_file, "wb") as archive: + shutil.copyfileobj(response, archive) + + if sys.platform.startswith("linux"): + with tarfile.open(binary_file, "r:gz") as archive: + archive.extractall(binary_file_name) + else: + with zipfile.ZipFile(binary_file, "r") as archive: + archive.extractall(binary_file_name) + + os.remove(binary_file) + with open("requirements.txt") as f: required = f.read().splitlines()