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2020-01-22 16:31:44 +01:00
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< a accesskey = "h" href = "./index.html" > UP < / 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" >
< h2 > Table of Contents< / h2 >
< div id = "text-table-of-contents" >
< ul >
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< li > < a href = "#orgfba33d4" > 1. Inertial Control< / a >
< ul >
< li > < a href = "#org0ea4bd4" > 1.1. Identification of the Dynamics< / a > < / li >
< li > < a href = "#org5a29480" > 1.2. Effect of the Flexible Joint stiffness on the Dynamics< / a > < / li >
< li > < a href = "#orga92be75" > 1.3. Obtained Damping< / a > < / li >
< li > < a href = "#orgb29f377" > 1.4. Conclusion< / a > < / li >
< / ul >
< / li >
< li > < a href = "#org5fde56d" > 2. Integral Force Feedback< / a >
< ul >
< li > < a href = "#org8823e64" > 2.1. Identification of the Dynamics with perfect Joints< / a > < / li >
< li > < a href = "#org2aff899" > 2.2. Effect of the Flexible Joint stiffness on the Dynamics< / a > < / li >
< li > < a href = "#org40dffdd" > 2.3. Obtained Damping< / a > < / li >
< li > < a href = "#org2ae5aaf" > 2.4. Conclusion< / a > < / li >
< / ul >
< / li >
< 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 >
< li > < a href = "#org8f71141" > 3.2. Effect of the Flexible Joint stiffness on the Dynamics< / a > < / li >
< li > < a href = "#org87c6911" > 3.3. Obtained Damping< / a > < / li >
< li > < a href = "#org516fed1" > 3.4. Conclusion< / a > < / li >
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< / ul >
< / li >
< / ul >
< / div >
< / div >
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< p >
The following decentralized active damping techniques are briefly studied:
< / p >
< ul class = "org-ul" >
< li > Inertial Control (proportional feedback of the absolute velocity): Section < a href = "#org3c68d9e" > 1< / a > < / li >
< li > Integral Force Feedback: Section < a href = "#org62cd19c" > 2< / a > < / li >
< li > Direct feedback of the relative velocity of each strut: Section < a href = "#org587277a" > 3< / a > < / li >
< / ul >
< div id = "outline-container-orgfba33d4" class = "outline-2" >
< 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 >
< a id = "org3c68d9e" > < / a >
< / p >
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< / div >
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< div id = "outline-container-org0ea4bd4" class = "outline-3" >
< 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" >
< 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);
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 >
< 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" > '/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 >
< 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" > '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 >
< / div >
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< p >
The transfer function from actuator forces to force sensors is shown in Figure < a href = "#orgfc5367b" > 1< / a > .
< / p >
< div id = "orgfc5367b" class = "figure" >
< p > < img src = "figs/inertial_plant_coupling.png" alt = "inertial_plant_coupling.png" / >
< / p >
< 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 >
< / div >
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< / div >
< / div >
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< div id = "outline-container-org5a29480" class = "outline-3" >
< 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 >
We add some stiffness and damping in the flexible joints and we re-identify the dynamics.
< / p >
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< div class = "org-src-container" >
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< 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" > '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 >
< / div >
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< 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 >
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< / div >
< / div >
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< div id = "outline-container-orga92be75" class = "outline-3" >
< h3 id = "orga92be75" > < span class = "section-number-3" > 1.3< / span > Obtained Damping< / h3 >
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< div class = "outline-text-3" id = "text-1-3" >
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< 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 >
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< 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;
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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 >
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 >
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< 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 > };
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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 > };
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< / pre >
< / div >
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< 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 >
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< / div >
< / div >
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< 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 >
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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 >
options = linearizeOptions;
options.SampleTime = 0;
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< 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 > ;
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< 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 > };
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< / pre >
< / div >
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< 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 >
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< div class = "org-src-container" >
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< 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 > };
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< / pre >
< / div >
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< 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 >
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< / div >
< / div >
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< 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" >
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< p >
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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:
\[ K(s) = g
\begin{bmatrix}
s & & \\
& \ddots & \\
& & s
\end{bmatrix} \]
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< / p >
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< 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 >
< / div >
< / div >
< / div >
< div id = "outline-container-org516fed1" class = "outline-3" >
< h3 id = "org516fed1" > < span class = "section-number-3" > 3.4< / span > Conclusion< / h3 >
< div class = "outline-text-3" id = "text-3-4" >
< 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 >
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< / div >
< / div >
< / div >
< / div >
< div id = "postamble" class = "status" >
< p class = "author" > Author: Dehaeze Thomas< / p >
2020-02-06 15:39:35 +01:00
< p class = "date" > Created: 2020-02-06 jeu. 15:39< / p >
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< / div >
< / body >
< / html >
