# closed_loop_ankle **Repository Path**: luozhijing/closed_loop_ankle ## Basic Information - **Project Name**: closed_loop_ankle - **Description**: 双足串并联转换 - **Primary Language**: Unknown - **License**: Not specified - **Default Branch**: main - **Homepage**: None - **GVP Project**: No ## Statistics - **Stars**: 1 - **Forks**: 0 - **Created**: 2025-06-05 - **Last Updated**: 2025-12-10 ## Categories & Tags **Categories**: Uncategorized **Tags**: None ## README # closed_loop_ankle ​   A mainstream 2-DOF humanoid ankle simulation in Webots. This implementation includes forward and inverse kinematics for a closed-loop ankle, enabling torque mapping between the two motors and the ankle joints. Only for ankle like this: ![ankle](https://github.com/HuNingHe/closed_loop_ankle/blob/main/pictures/ankle.gif) # Test - Ubuntu24.04 - WebotsR2023b # Request - Eigen - [ros2_plot](https://github.com/HuNingHe/ros2_plot) - Webots # Build ```bash git clone https://github.com/HuNingHe/closed_loop_ankle.git cd closed_loop_ankle/contrers/my_contrer && mkdir build cd build && cmake ../ make -j4 ``` # Usage ```bash cd ros2_plot_ws && source install/setup.bash ros2 run ros2_plot ros2_plot # run ros2_plot first!!!! ros2 run plotjuggler plotjuggler # Open webots and run ankle.wbt ``` ​​    If you are not using ros2, you can remove all shared memory related code and recompile, you can run still without data visualization. ​    set `test_kinematics` in `my_contrer.cpp`(line 352) to false, then you can test torque mapping between motors and ankle joint. ​    **suggest to use plot.xml of ros2_plot in plotjuggler**. # Mathematics ​​    You can find the formula below in the code: $$ \begin{bmatrix} \theta_{1} \\ \theta_{2} \end{bmatrix} =f_1(\theta_{p},\theta_{r}, d, L_1,h_1,h_2) $$ ​​​    where $f_1$ is `ankle_ik`, and all subscripts with '1' denote the left motor of ankle, while subscripts with '2' denote the right motor. The subscript 'p' represents the ankle pitch, and 'r' represents the ankle roll. Definitions for the remaining terms 'd', 'L1', 'h1', and 'h2' are link lengths can be found in the two figures below $$ \begin{bmatrix} \dot \theta_1 \\ \dot \theta_2 \end{bmatrix} =\begin{bmatrix} \frac{\delta f_{11}}{\delta \theta_p} & \frac{\delta f_{11}}{\delta \theta_r} \\ \frac{\delta f_{12}}{\delta \theta_p} & \frac{\delta f_{12}}{\delta \theta_r} \end{bmatrix} \begin{bmatrix} \dot \theta_p \\ \dot \theta_r \end{bmatrix}=J_2\begin{bmatrix} \dot \theta_p \\ \dot \theta_r \end{bmatrix} $$ ​​​​    where $\frac{\delta f_{11}}{\delta \theta_{p}}$ is `computeTmLtY`, $\frac{\delta f_{11}}{\delta \theta_{r}}$ is `computeTmLtX`, $\frac{\delta f_{12}}{\delta \theta_{p}}$ is `computeTmRtY`, $\frac{\delta f_{12}}{\delta \theta_{r}}$ is `computeTmRtX`,or general case $J_2=J_1^{-1}$ $$ \begin{bmatrix} \theta_{p} \\ \theta_{r} \end{bmatrix} =\begin{bmatrix} 0.5(\theta_{1}+\theta_{2}) \\ f_2(\theta_{1},\theta_{2}, d, L_1,h_1,h_2) \end{bmatrix} $$ ​​​​    where $f_2$ is `calculateTx` $$ \begin{bmatrix} \dot \theta_p \\ \dot \theta_r \end{bmatrix} =\begin{bmatrix} 0.5 & 0.5 \\ \frac{\delta f_2}{\delta \theta_1} & \frac{\delta f_2}{\delta \theta_2} \end{bmatrix} \begin{bmatrix} \dot \theta_1 \\ \dot \theta_2 \end{bmatrix}=J_1\begin{bmatrix} \dot \theta_1 \\ \dot \theta_2 \end{bmatrix} $$ ​​​​    where $\frac{\delta f_{2}}{\delta \theta_{1}}$ is `calculateTxML`, $\frac{\delta f_{2}}{\delta \theta_{2}}$ is `calculateTxMR` ​​​​    according to the principle of virtual work, we have: $$ \begin{bmatrix} \tau_1 \\ \tau_2 \end{bmatrix}=J_1^T \begin{bmatrix} \tau_{p} \\ \tau_{r} \end{bmatrix} $$ $$ \begin{bmatrix} \tau_{p} \\ \tau_{r} \end{bmatrix}=J_2^T\begin{bmatrix} \tau_1 \\ \tau_2 \end{bmatrix} $$ ​​​​​    Both of 2 motors and 2 joints of the ankle follow the right-hand rule: rotation around the Y-axis in the counterclockwise direction is considered positive, with the X-axis pointing forward and the Z-axis pointing vertically. ​​​​​    Some notations: