Update conclusion about flexible joints
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@@ -504,7 +504,7 @@ It is shown that the bending stiffness of the flexible joints have very little i
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The bending stiffness of the flexible joint does not significantly change the dynamics.
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#+end_important
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* Translation Stiffness
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* Axial Stiffness
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<<sec:trans_stiffness>>
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** Introduction :ignore:
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@@ -993,8 +993,22 @@ The dynamics from $\bm{\tau}^\prime$ to $\bm{\epsilon}_{\mathcal{X}_n}$ (for the
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<<sec:conclusion>>
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#+begin_important
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For the identified optimal actuator stiffness $k = 10^5\,[N/m]$, the flexible joint should have the following stiffness properties:
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- Bending Stiffness: $K_b < 50\,[Nm/rad]$
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- Torsion Stiffness: $K_t < 50\,[Nm/rad]$
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- Axial Stiffness: $K_a > 10^7\,[N/m]$
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In this study we considered the bending, torsional and axial stiffnesses of the flexible joints used for the nano-hexapod.
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The bending and torsional stiffnesses somehow adds a parasitic stiffness in parallel with the legs.
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It is not found to be much problematic for the considered control architecture (it is however, if Integral Force Feedback is to be used).
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As a consequence of the added stiffness, it could increase a little bit the required actuator force.
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The axial stiffness of the flexible joints can be very problematic for control.
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Small values of the axial stiffness are shown to limit the achievable damping with Direct Velocity Feedback.
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The axial stiffness should therefore be maximized and taken into account in the model of the nano-hexapod.
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For the identified optimal actuator stiffness $k = 10^5\,[N/m]$, the flexible joint should have the following stiffness properties:
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- Axial Stiffness: $K_a > 10^7\,[N/m]$
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- Bending Stiffness: $K_b < 50\,[Nm/rad]$
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- Torsion Stiffness: $K_t < 50\,[Nm/rad]$
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As there is generally a trade-off between bending stiffness and axial stiffness, it should be highlighted that the *axial* stiffness is the most important property of the flexible joints.
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#+end_important
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