Home > arte3.2.0 > demos > inversedynamics_1DOFplanar.m

inversedynamics_1DOFplanar

PURPOSE ^

SCRIPT TEST FOR THE 2DOF arm

SYNOPSIS ^

This is a script file.

DESCRIPTION ^

 SCRIPT TEST FOR THE 2DOF arm

CROSS-REFERENCE INFORMATION ^

This function calls: This function is called by:

SOURCE CODE ^

0001 % SCRIPT TEST FOR THE 2DOF arm
0002 
0003 % Copyright (C) 2012, by Arturo Gil Aparicio
0004 %
0005 % This file is part of ARTE (A Robotics Toolbox for Education).
0006 %
0007 % ARTE is free software: you can redistribute it and/or modify
0008 % it under the terms of the GNU Lesser General Public License as published by
0009 % the Free Software Foundation, either version 3 of the License, or
0010 % (at your option) any later version.
0011 %
0012 % ARTE is distributed in the hope that it will be useful,
0013 % but WITHOUT ANY WARRANTY; without even the implied warranty of
0014 % MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
0015 % GNU Lesser General Public License for more details.
0016 %
0017 % You should have received a copy of the GNU Leser General Public License
0018 % along with ARTE.  If not, see <http://www.gnu.org/licenses/>.
0019 
0020 close all
0021 
0022 q1 = [0 ];    
0023 q2 = [pi/2];
0024 
0025 
0026 
0027 %general call to inverse dynamic function
0028 %TAU = inversedynamic(param, Q, QD, QDD, GRAV, FEXT)
0029 
0030 %load example arm
0031 planar=load_robot('example', '1dofplanar');
0032 
0033 
0034 %Tau is cero at any joint at the presented position.
0035 fprintf('\nTorques at each joint given position = [0 0], and velocity=[0 0] and standard gravity acting on Z0')
0036 tau = inversedynamic(planar, q1, [0], [1], [0 0 9.81]', [0 0 0 0 0 0]')
0037 
0038 drawrobot3d(planar,q1)
0039 disp('press any key to continue')
0040 pause
0041 
0042 
0043 %now, change the direction of gravity, which is equivalent to change the
0044 %mounting position of the arm. All torques appear as a consequence of a
0045 %gravitational load acting on the COM of each link
0046 fprintf('\nTorques at each joint given position = [0 0], and velocity=[0 0] and standard gravity acting on Y0')
0047 tau = inversedynamic(planar, q1, [0 0], [0 0], [ 0 -9.81 0]', [0 0 0 0 0 0]')
0048 disp('press any key to continue')
0049 pause
0050 
0051 
0052 %Now, apply forces expressed at the X2 Y2 Z2 reference system.
0053 %Please note that forces acting on X2, Z2 and moments acting on My2 and Mx2
0054 %do not contribute to the torques at each joint. Please add forces in Y2
0055 %direction and moments acting on Z2 direction
0056 fprintf('\nTorques at each joint given position = [0 0], and velocity=[0 0] and standard gravity acting on Z0, forces expressed on X2Y2Z2 [1 0 1 1 1 0]')
0057 tau = inversedynamic(planar, q1, [0 0], [ 0 0], [0 0 9.81]', [1 0 1 1 1 0]')
0058 disp('press any key to continue')
0059 pause
0060 
0061 
0062 
0063 %Now, compute torques necessary to bring the arm to a general kinetic state
0064 fprintf('\nTorques at each joint given position = [0 0], and velocity=[0 0] and standard gravity acting on Z0, forces expressed on X2Y2Z2 [0 1 0 0 0 1]')
0065 tau = inversedynamic(planar, q2, [1 1], [1 1], [0 0 9.81]', [0 1 0 0 0 1]')
0066 
0067 drawrobot3d(planar,q2)
0068 disp('press any key to continue')
0069 pause
0070 
0071

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