712 lines
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712 lines
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<a accesskey="H" href="./index.html"> HOME </a>
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</div><div id="content">
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<h1 class="title">Stewart Platform - Decentralized Active Damping</h1>
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<div id="table-of-contents">
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<h2>Table of Contents</h2>
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<div id="text-table-of-contents">
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<ul>
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<li><a href="#orgfba33d4">1. Inertial Control</a>
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<ul>
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<li><a href="#org0ea4bd4">1.1. Identification of the Dynamics</a></li>
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<li><a href="#org5a29480">1.2. Effect of the Flexible Joint stiffness on the Dynamics</a></li>
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<li><a href="#orga92be75">1.3. Obtained Damping</a></li>
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<li><a href="#orgb29f377">1.4. Conclusion</a></li>
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</ul>
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</li>
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<li><a href="#org5fde56d">2. Integral Force Feedback</a>
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<ul>
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<li><a href="#org8823e64">2.1. Identification of the Dynamics with perfect Joints</a></li>
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<li><a href="#org2aff899">2.2. Effect of the Flexible Joint stiffness on the Dynamics</a></li>
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<li><a href="#org40dffdd">2.3. Obtained Damping</a></li>
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<li><a href="#org2ae5aaf">2.4. Conclusion</a></li>
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</ul>
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</li>
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<li><a href="#org9425768">3. Direct Velocity Feedback</a>
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<ul>
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<li><a href="#org61043ac">3.1. Identification of the Dynamics with perfect Joints</a></li>
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<li><a href="#org8f71141">3.2. Effect of the Flexible Joint stiffness on the Dynamics</a></li>
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<li><a href="#org87c6911">3.3. Obtained Damping</a></li>
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<li><a href="#org516fed1">3.4. Conclusion</a></li>
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</ul>
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</li>
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</ul>
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</div>
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</div>
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<p>
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The following decentralized active damping techniques are briefly studied:
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</p>
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<ul class="org-ul">
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<li>Inertial Control (proportional feedback of the absolute velocity): Section <a href="#org3c68d9e">1</a></li>
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<li>Integral Force Feedback: Section <a href="#org62cd19c">2</a></li>
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<li>Direct feedback of the relative velocity of each strut: Section <a href="#org587277a">3</a></li>
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</ul>
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<div id="outline-container-orgfba33d4" class="outline-2">
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<h2 id="orgfba33d4"><span class="section-number-2">1</span> Inertial Control</h2>
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<div class="outline-text-2" id="text-1">
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<p>
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<a id="org3c68d9e"></a>
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</p>
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</div>
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<div id="outline-container-org0ea4bd4" class="outline-3">
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<h3 id="org0ea4bd4"><span class="section-number-3">1.1</span> Identification of the Dynamics</h3>
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<div class="outline-text-3" id="text-1-1">
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<div class="org-src-container">
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<pre class="src src-matlab">stewart = initializeFramesPositions(<span class="org-string">'H'</span>, 90e<span class="org-type">-</span>3, <span class="org-string">'MO_B'</span>, 45e<span class="org-type">-</span>3);
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stewart = generateGeneralConfiguration(stewart);
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stewart = computeJointsPose(stewart);
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stewart = initializeStrutDynamics(stewart);
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stewart = initializeJointDynamics(stewart, <span class="org-string">'disable'</span>, <span class="org-constant">true</span>);
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stewart = initializeCylindricalPlatforms(stewart);
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stewart = initializeCylindricalStruts(stewart);
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stewart = computeJacobian(stewart);
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stewart = initializeStewartPose(stewart);
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</pre>
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</div>
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<div class="org-src-container">
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<pre class="src src-matlab"><span class="org-matlab-cellbreak"><span class="org-comment">%% Options for Linearized</span></span>
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options = linearizeOptions;
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options.SampleTime = 0;
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<span class="org-matlab-cellbreak"><span class="org-comment">%% Name of the Simulink File</span></span>
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mdl = <span class="org-string">'stewart_active_damping'</span>;
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<span class="org-matlab-cellbreak"><span class="org-comment">%% Input/Output definition</span></span>
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clear io; io_i = 1;
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io(io_i) = linio([mdl, <span class="org-string">'/F'</span>], 1, <span class="org-string">'openinput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Actuator Force Inputs [N]</span>
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io(io_i) = linio([mdl, <span class="org-string">'/Vm'</span>], 1, <span class="org-string">'openoutput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Absolute velocity of each leg [m/s]</span>
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<span class="org-matlab-cellbreak"><span class="org-comment">%% Run the linearization</span></span>
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G = linearize(mdl, io, options);
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G.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
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G.OutputName = {<span class="org-string">'Vm1'</span>, <span class="org-string">'Vm2'</span>, <span class="org-string">'Vm3'</span>, <span class="org-string">'Vm4'</span>, <span class="org-string">'Vm5'</span>, <span class="org-string">'Vm6'</span>};
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</pre>
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</div>
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<p>
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The transfer function from actuator forces to force sensors is shown in Figure <a href="#orgfc5367b">1</a>.
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</p>
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<div id="orgfc5367b" class="figure">
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<p><img src="figs/inertial_plant_coupling.png" alt="inertial_plant_coupling.png" />
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</p>
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<p><span class="figure-number">Figure 1: </span>Transfer function from the Actuator force \(F_{i}\) to the absolute velocity of the same leg \(v_{m,i}\) and to the absolute velocity of the other legs \(v_{m,j}\) with \(i \neq j\) in grey (<a href="./figs/inertial_plant_coupling.png">png</a>, <a href="./figs/inertial_plant_coupling.pdf">pdf</a>)</p>
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</div>
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</div>
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</div>
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<div id="outline-container-org5a29480" class="outline-3">
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<h3 id="org5a29480"><span class="section-number-3">1.2</span> Effect of the Flexible Joint stiffness on the Dynamics</h3>
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<div class="outline-text-3" id="text-1-2">
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<p>
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We add some stiffness and damping in the flexible joints and we re-identify the dynamics.
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</p>
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<div class="org-src-container">
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<pre class="src src-matlab">stewart = initializeJointDynamics(stewart);
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Gf = linearize(mdl, io, options);
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Gf.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
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Gf.OutputName = {<span class="org-string">'Vm1'</span>, <span class="org-string">'Vm2'</span>, <span class="org-string">'Vm3'</span>, <span class="org-string">'Vm4'</span>, <span class="org-string">'Vm5'</span>, <span class="org-string">'Vm6'</span>};
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
The new dynamics from force actuator to force sensor is shown in Figure <a href="#org2ee5d65">2</a>.
|
|
</p>
|
|
|
|
<div id="org2ee5d65" class="figure">
|
|
<p><img src="figs/inertial_plant_flexible_joint_decentralized.png" alt="inertial_plant_flexible_joint_decentralized.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 2: </span>Transfer function from the Actuator force \(F_{i}\) to the absolute velocity sensor \(v_{m,i}\) (<a href="./figs/inertial_plant_flexible_joint_decentralized.png">png</a>, <a href="./figs/inertial_plant_flexible_joint_decentralized.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-orga92be75" class="outline-3">
|
|
<h3 id="orga92be75"><span class="section-number-3">1.3</span> Obtained Damping</h3>
|
|
<div class="outline-text-3" id="text-1-3">
|
|
<p>
|
|
The control is a performed in a decentralized manner.
|
|
The \(6 \times 6\) control is a diagonal matrix with pure proportional action on the diagonal:
|
|
\[ K(s) = g
|
|
\begin{bmatrix}
|
|
1 & & 0 \\
|
|
& \ddots & \\
|
|
0 & & 1
|
|
\end{bmatrix} \]
|
|
</p>
|
|
|
|
<p>
|
|
The root locus is shown in figure <a href="#org78a599c">3</a> and the obtained pole damping function of the control gain is shown in figure <a href="#org0b6bb28">4</a>.
|
|
</p>
|
|
|
|
<div id="org78a599c" class="figure">
|
|
<p><img src="figs/root_locus_inertial_rot_stiffness.png" alt="root_locus_inertial_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 3: </span>Root Locus plot with Decentralized Inertial Control when considering the stiffness of flexible joints (<a href="./figs/root_locus_inertial_rot_stiffness.png">png</a>, <a href="./figs/root_locus_inertial_rot_stiffness.pdf">pdf</a>)</p>
|
|
</div>
|
|
|
|
|
|
<div id="org0b6bb28" class="figure">
|
|
<p><img src="figs/pole_damping_gain_inertial_rot_stiffness.png" alt="pole_damping_gain_inertial_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 4: </span>Damping of the poles with respect to the gain of the Decentralized Inertial Control when considering the stiffness of flexible joints (<a href="./figs/pole_damping_gain_inertial_rot_stiffness.png">png</a>, <a href="./figs/pole_damping_gain_inertial_rot_stiffness.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-orgb29f377" class="outline-3">
|
|
<h3 id="orgb29f377"><span class="section-number-3">1.4</span> Conclusion</h3>
|
|
<div class="outline-text-3" id="text-1-4">
|
|
<div class="important">
|
|
<p>
|
|
Joint stiffness does increase the resonance frequencies of the system but does not change the attainable damping when using relative motion sensors.
|
|
</p>
|
|
|
|
</div>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org5fde56d" class="outline-2">
|
|
<h2 id="org5fde56d"><span class="section-number-2">2</span> Integral Force Feedback</h2>
|
|
<div class="outline-text-2" id="text-2">
|
|
<p>
|
|
<a id="org62cd19c"></a>
|
|
</p>
|
|
</div>
|
|
|
|
<div id="outline-container-org8823e64" class="outline-3">
|
|
<h3 id="org8823e64"><span class="section-number-3">2.1</span> Identification of the Dynamics with perfect Joints</h3>
|
|
<div class="outline-text-3" id="text-2-1">
|
|
<p>
|
|
We first initialize the Stewart platform without joint stiffness.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab">stewart = initializeFramesPositions(<span class="org-string">'H'</span>, 90e<span class="org-type">-</span>3, <span class="org-string">'MO_B'</span>, 45e<span class="org-type">-</span>3);
|
|
stewart = generateGeneralConfiguration(stewart);
|
|
stewart = computeJointsPose(stewart);
|
|
stewart = initializeStrutDynamics(stewart);
|
|
stewart = initializeJointDynamics(stewart, <span class="org-string">'disable'</span>, <span class="org-constant">true</span>);
|
|
stewart = initializeCylindricalPlatforms(stewart);
|
|
stewart = initializeCylindricalStruts(stewart);
|
|
stewart = computeJacobian(stewart);
|
|
stewart = initializeStewartPose(stewart);
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
And we identify the dynamics from force actuators to force sensors.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab"><span class="org-matlab-cellbreak"><span class="org-comment">%% Options for Linearized</span></span>
|
|
options = linearizeOptions;
|
|
options.SampleTime = 0;
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Name of the Simulink File</span></span>
|
|
mdl = <span class="org-string">'stewart_active_damping'</span>;
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Input/Output definition</span></span>
|
|
clear io; io_i = 1;
|
|
io(io_i) = linio([mdl, <span class="org-string">'/F'</span>], 1, <span class="org-string">'openinput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Actuator Force Inputs [N]</span>
|
|
io(io_i) = linio([mdl, <span class="org-string">'/Fm'</span>], 1, <span class="org-string">'openoutput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Force Sensor Outputs [N]</span>
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Run the linearization</span></span>
|
|
G = linearize(mdl, io, options);
|
|
G.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
|
|
G.OutputName = {<span class="org-string">'Fm1'</span>, <span class="org-string">'Fm2'</span>, <span class="org-string">'Fm3'</span>, <span class="org-string">'Fm4'</span>, <span class="org-string">'Fm5'</span>, <span class="org-string">'Fm6'</span>};
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
The transfer function from actuator forces to force sensors is shown in Figure <a href="#orgae4e327">5</a>.
|
|
</p>
|
|
|
|
<div id="orgae4e327" class="figure">
|
|
<p><img src="figs/iff_plant_coupling.png" alt="iff_plant_coupling.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 5: </span>Transfer function from the Actuator force \(F_{i}\) to the Force sensor of the same leg \(F_{m,i}\) and to the force sensor of the other legs \(F_{m,j}\) with \(i \neq j\) in grey (<a href="./figs/iff_plant_coupling.png">png</a>, <a href="./figs/iff_plant_coupling.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org2aff899" class="outline-3">
|
|
<h3 id="org2aff899"><span class="section-number-3">2.2</span> Effect of the Flexible Joint stiffness on the Dynamics</h3>
|
|
<div class="outline-text-3" id="text-2-2">
|
|
<p>
|
|
We add some stiffness and damping in the flexible joints and we re-identify the dynamics.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab">stewart = initializeJointDynamics(stewart);
|
|
Gf = linearize(mdl, io, options);
|
|
Gf.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
|
|
Gf.OutputName = {<span class="org-string">'Fm1'</span>, <span class="org-string">'Fm2'</span>, <span class="org-string">'Fm3'</span>, <span class="org-string">'Fm4'</span>, <span class="org-string">'Fm5'</span>, <span class="org-string">'Fm6'</span>};
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
The new dynamics from force actuator to force sensor is shown in Figure <a href="#orgd21a8a8">6</a>.
|
|
</p>
|
|
|
|
<div id="orgd21a8a8" class="figure">
|
|
<p><img src="figs/iff_plant_flexible_joint_decentralized.png" alt="iff_plant_flexible_joint_decentralized.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 6: </span>Transfer function from the Actuator force \(F_{i}\) to the force sensor \(F_{m,i}\) (<a href="./figs/iff_plant_flexible_joint_decentralized.png">png</a>, <a href="./figs/iff_plant_flexible_joint_decentralized.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org40dffdd" class="outline-3">
|
|
<h3 id="org40dffdd"><span class="section-number-3">2.3</span> Obtained Damping</h3>
|
|
<div class="outline-text-3" id="text-2-3">
|
|
<p>
|
|
The control is a performed in a decentralized manner.
|
|
The \(6 \times 6\) control is a diagonal matrix with pure integration action on the diagonal:
|
|
\[ K(s) = g
|
|
\begin{bmatrix}
|
|
\frac{1}{s} & & 0 \\
|
|
& \ddots & \\
|
|
0 & & \frac{1}{s}
|
|
\end{bmatrix} \]
|
|
</p>
|
|
|
|
<p>
|
|
The root locus is shown in figure <a href="#org2cdbf69">7</a> and the obtained pole damping function of the control gain is shown in figure <a href="#orge344229">8</a>.
|
|
</p>
|
|
|
|
<div id="org2cdbf69" class="figure">
|
|
<p><img src="figs/root_locus_iff_rot_stiffness.png" alt="root_locus_iff_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 7: </span>Root Locus plot with Decentralized Integral Force Feedback when considering the stiffness of flexible joints (<a href="./figs/root_locus_iff_rot_stiffness.png">png</a>, <a href="./figs/root_locus_iff_rot_stiffness.pdf">pdf</a>)</p>
|
|
</div>
|
|
|
|
|
|
<div id="orge344229" class="figure">
|
|
<p><img src="figs/pole_damping_gain_iff_rot_stiffness.png" alt="pole_damping_gain_iff_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 8: </span>Damping of the poles with respect to the gain of the Decentralized Integral Force Feedback when considering the stiffness of flexible joints (<a href="./figs/pole_damping_gain_iff_rot_stiffness.png">png</a>, <a href="./figs/pole_damping_gain_iff_rot_stiffness.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org2ae5aaf" class="outline-3">
|
|
<h3 id="org2ae5aaf"><span class="section-number-3">2.4</span> Conclusion</h3>
|
|
<div class="outline-text-3" id="text-2-4">
|
|
<div class="important">
|
|
<p>
|
|
The joint stiffness has a huge impact on the attainable active damping performance when using force sensors.
|
|
Thus, if Integral Force Feedback is to be used in a Stewart platform with flexible joints, the rotational stiffness of the joints should be minimized.
|
|
</p>
|
|
|
|
</div>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org9425768" class="outline-2">
|
|
<h2 id="org9425768"><span class="section-number-2">3</span> Direct Velocity Feedback</h2>
|
|
<div class="outline-text-2" id="text-3">
|
|
<p>
|
|
<a id="org587277a"></a>
|
|
</p>
|
|
</div>
|
|
|
|
<div id="outline-container-org61043ac" class="outline-3">
|
|
<h3 id="org61043ac"><span class="section-number-3">3.1</span> Identification of the Dynamics with perfect Joints</h3>
|
|
<div class="outline-text-3" id="text-3-1">
|
|
<p>
|
|
We first initialize the Stewart platform without joint stiffness.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab">stewart = initializeFramesPositions(<span class="org-string">'H'</span>, 90e<span class="org-type">-</span>3, <span class="org-string">'MO_B'</span>, 45e<span class="org-type">-</span>3);
|
|
stewart = generateGeneralConfiguration(stewart);
|
|
stewart = computeJointsPose(stewart);
|
|
stewart = initializeStrutDynamics(stewart);
|
|
stewart = initializeJointDynamics(stewart, <span class="org-string">'disable'</span>, <span class="org-constant">true</span>);
|
|
stewart = initializeCylindricalPlatforms(stewart);
|
|
stewart = initializeCylindricalStruts(stewart);
|
|
stewart = computeJacobian(stewart);
|
|
stewart = initializeStewartPose(stewart);
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
And we identify the dynamics from force actuators to force sensors.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab"><span class="org-matlab-cellbreak"><span class="org-comment">%% Options for Linearized</span></span>
|
|
options = linearizeOptions;
|
|
options.SampleTime = 0;
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Name of the Simulink File</span></span>
|
|
mdl = <span class="org-string">'stewart_active_damping'</span>;
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Input/Output definition</span></span>
|
|
clear io; io_i = 1;
|
|
io(io_i) = linio([mdl, <span class="org-string">'/F'</span>], 1, <span class="org-string">'openinput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Actuator Force Inputs [N]</span>
|
|
io(io_i) = linio([mdl, <span class="org-string">'/Dm'</span>], 1, <span class="org-string">'openoutput'</span>); io_i = io_i <span class="org-type">+</span> 1; <span class="org-comment">% Relative Displacement Outputs [N]</span>
|
|
|
|
<span class="org-matlab-cellbreak"><span class="org-comment">%% Run the linearization</span></span>
|
|
G = linearize(mdl, io, options);
|
|
G.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
|
|
G.OutputName = {<span class="org-string">'Dm1'</span>, <span class="org-string">'Dm2'</span>, <span class="org-string">'Dm3'</span>, <span class="org-string">'Dm4'</span>, <span class="org-string">'Dm5'</span>, <span class="org-string">'Dm6'</span>};
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
The transfer function from actuator forces to relative motion sensors is shown in Figure <a href="#orgd8d51db">9</a>.
|
|
</p>
|
|
|
|
<div id="orgd8d51db" class="figure">
|
|
<p><img src="figs/dvf_plant_coupling.png" alt="dvf_plant_coupling.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 9: </span>Transfer function from the Actuator force \(F_{i}\) to the Relative Motion Sensor \(D_{m,j}\) with \(i \neq j\) (<a href="./figs/dvf_plant_coupling.png">png</a>, <a href="./figs/dvf_plant_coupling.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
|
|
<div id="outline-container-org8f71141" class="outline-3">
|
|
<h3 id="org8f71141"><span class="section-number-3">3.2</span> Effect of the Flexible Joint stiffness on the Dynamics</h3>
|
|
<div class="outline-text-3" id="text-3-2">
|
|
<p>
|
|
We add some stiffness and damping in the flexible joints and we re-identify the dynamics.
|
|
</p>
|
|
<div class="org-src-container">
|
|
<pre class="src src-matlab">stewart = initializeJointDynamics(stewart);
|
|
Gf = linearize(mdl, io, options);
|
|
Gf.InputName = {<span class="org-string">'F1'</span>, <span class="org-string">'F2'</span>, <span class="org-string">'F3'</span>, <span class="org-string">'F4'</span>, <span class="org-string">'F5'</span>, <span class="org-string">'F6'</span>};
|
|
Gf.OutputName = {<span class="org-string">'Dm1'</span>, <span class="org-string">'Dm2'</span>, <span class="org-string">'Dm3'</span>, <span class="org-string">'Dm4'</span>, <span class="org-string">'Dm5'</span>, <span class="org-string">'Dm6'</span>};
|
|
</pre>
|
|
</div>
|
|
|
|
<p>
|
|
The new dynamics from force actuator to relative motion sensor is shown in Figure <a href="#orgb18f950">10</a>.
|
|
</p>
|
|
|
|
<div id="orgb18f950" class="figure">
|
|
<p><img src="figs/dvf_plant_flexible_joint_decentralized.png" alt="dvf_plant_flexible_joint_decentralized.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 10: </span>Transfer function from the Actuator force \(F_{i}\) to the relative displacement sensor \(D_{m,i}\) (<a href="./figs/dvf_plant_flexible_joint_decentralized.png">png</a>, <a href="./figs/dvf_plant_flexible_joint_decentralized.pdf">pdf</a>)</p>
|
|
</div>
|
|
</div>
|
|
</div>
|
|
|
|
<div id="outline-container-org87c6911" class="outline-3">
|
|
<h3 id="org87c6911"><span class="section-number-3">3.3</span> Obtained Damping</h3>
|
|
<div class="outline-text-3" id="text-3-3">
|
|
<p>
|
|
The control is a performed in a decentralized manner.
|
|
The \(6 \times 6\) control is a diagonal matrix with pure derivative action on the diagonal:
|
|
\[ K(s) = g
|
|
\begin{bmatrix}
|
|
s & & \\
|
|
& \ddots & \\
|
|
& & s
|
|
\end{bmatrix} \]
|
|
</p>
|
|
|
|
<p>
|
|
The root locus is shown in figure <a href="#org5cb31c8">11</a> and the obtained pole damping function of the control gain is shown in figure <a href="#org4618492">12</a>.
|
|
</p>
|
|
|
|
<div id="org5cb31c8" class="figure">
|
|
<p><img src="figs/root_locus_dvf_rot_stiffness.png" alt="root_locus_dvf_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 11: </span>Root Locus plot with Direct Velocity Feedback when considering the Stiffness of flexible joints (<a href="./figs/root_locus_dvf_rot_stiffness.png">png</a>, <a href="./figs/root_locus_dvf_rot_stiffness.pdf">pdf</a>)</p>
|
|
</div>
|
|
|
|
|
|
<div id="org4618492" class="figure">
|
|
<p><img src="figs/pole_damping_gain_dvf_rot_stiffness.png" alt="pole_damping_gain_dvf_rot_stiffness.png" />
|
|
</p>
|
|
<p><span class="figure-number">Figure 12: </span>Damping of the poles with respect to the gain of the Direct Velocity Feedback when considering the Stiffness of flexible joints (<a href="./figs/pole_damping_gain_dvf_rot_stiffness.png">png</a>, <a href="./figs/pole_damping_gain_dvf_rot_stiffness.pdf">pdf</a>)</p>
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<div id="outline-container-org516fed1" class="outline-3">
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<h3 id="org516fed1"><span class="section-number-3">3.4</span> Conclusion</h3>
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<div class="outline-text-3" id="text-3-4">
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<div class="important">
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<p>
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Joint stiffness does increase the resonance frequencies of the system but does not change the attainable damping when using relative motion sensors.
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</p>
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<div id="postamble" class="status">
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<p class="author">Author: Dehaeze Thomas</p>
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<p class="date">Created: 2020-02-06 jeu. 15:39</p>
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