Rework hexapod specifications + static deflection

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Thomas Dehaeze 2020-05-08 16:31:43 +02:00
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@ -2027,22 +2027,52 @@ The simulation is considered to be fairly realistic as the model used has been s
* General Conclusion and Further notes
<<sec:conclusion_and_further_notes>>
** Introduction :ignore:
** Nano-Hexapod Specifications
Table summarizing the nano-hexapod wanted characteristics:
<<sec:nano_hexapod_specifications>>
*** Introduction :ignore:
In this section are gathered all the specifications related to the nano-hexapod.
*** Dimensions
:PROPERTIES:
:UNNUMBERED: t
:END:
The wanted dimension of the nano-hexapod are shown in Figure [[fig:nano_hexapod_size]]:
- Diameter of the bottom platform: 300mm
- Diameter of the top platform: 200mm
- Maximum Height: 90mm
#+name: fig:nano_hexapod_size
#+caption: First implementation of the nano-hexapod / metrology reflector and sample interface
[[file:figs/nano_hexapod_size.png]]
*** Flexible Joints
:PROPERTIES:
:UNNUMBERED: t
:END:
Flexible joints are located at each end of the six struts.
These flexible joints should have the following properties:
- High Axial Stiffness: $K_a > 10^7\,[N/m]$
- Small Bending Stiffness: $K_b < 50\,[Nm/rad]$
- Small Torsion Stiffness: $K_t < 50\,[Nm/rad]$
The required angular stroke has not been estimated in this study.
It is however simple to do so as the angular motion of each joint can easily be measured in the multi-body model used to perform the simulations.
Typical angular stroke for such flexible joints is expected.
*** Actuators
:PROPERTIES:
:UNNUMBERED: t
:END:
The actuation part is probably the most important part of the Stewart platform.
- Dimensions (Figure [[fig:nano_hexapod_size]]):
- Maximum Height: 90mm
- Diameter of the bottom platform: 300mm
- Diameter of the top platform: 200mm
- Stiffness:
- Resonances should stay between 5Hz and 50Hz for payload masses up to 50kg
- This corresponds to strut stiffnesses of $k \approx 10^5 - 10^6\,[N/m]$
- Flexible joints:
- Axial Stiffness: $K_a > 10^7\,[N/m]$
- Bending Stiffness: $K_b < 50\,[Nm/rad]$
- Torsion Stiffness: $K_t < 50\,[Nm/rad]$
- Required angular stroke: can be estimated with simulations
- Force:
- Weight: $60\,kg \rightarrow 600\,N \rightarrow 60\,N$ on each actuator
- Dynamic: few Newtons
@ -2054,12 +2084,60 @@ Table summarizing the nano-hexapod wanted characteristics:
This is probably more difficult to obtain.
However, by limiting the acceleration of these stages, we may limit the dynamic tracking errors to acceptable levels
- If the chosen technology allows $\pm 50 \mu m$ that would be safer
- Sensors to be included:
-
#+name: fig:nano_hexapod_size
#+caption: First implementation of the nano-hexapod / metrology reflector and sample interface
[[file:figs/nano_hexapod_size.png]]
*** Sensors
:PROPERTIES:
:UNNUMBERED: t
:END:
A relative displacement sensor must be included in each of the nano-hexapod's legs as explained in Section [[sec:robust_control_architecture]].
The sensors must as the following properties:
- High bandwidth $> 1\,[kHz]$
- Fine resolution $< 10\,[nm]$
- Range of $> 100\,[\mu m]$
Note that the sensor signal will have to pass through the Slip-Ring.
This adds few constrains:
- The sensor signal must be immune to some "electrical noise" that could be induced by the slip-ring
- Limited number of slip-ring channels should be required for the six sensors
Several sensor technology could be used for the nano-hexapod.
Characteristics of those sensors are shown in Table [[tab:characteristics_relative_sensor]].
#+name: tab:characteristics_relative_sensor
#+caption: Characteristics of relative measurement sensors cite:collette11_review
| Technology | Frequency | Resolution | Range | T Range |
|----------------+------------+----------------+--------------+-------------|
| LVDT | DC-200 Hz | 10 nm rms | 1-10 mm | -50,100 °C |
| Eddy current | 5 kHz | 0.1-100 nm rms | 0.5-55 mm | -50,100 °C |
| Capacitive | DC-100 kHz | 0.05-50 nm rms | 50 nm - 1 cm | -40,100 °C |
| Interferometer | 300 kHz | 0.1 nm rms | 10 cm | -250,100 °C |
| Encoder | DC-1 MHz | 1 nm rms | 7-27 mm | 0,40 °C |
*** Architecture
:PROPERTIES:
:UNNUMBERED: t
:END:
** Problem of Static Deflection?
Let's now consider the problem of static deflection when changing the payload.
The maximum payload's mass is $50\,[kg]$, this corresponds to an added vertical force of $\approx 500\,[N]$.
If this is to be compensated by the nano-hexapod, $\approx 100\,[N]$ should be applied by each of the nano-hexapod's actuators.
In such case, the nano-hexapod keeps its nominal configuration.
In practice, this could be done using the relative motion sensor included in each leg, and a feedback control keeping the legs displacements at the wanted value.
This might not be a problem is piezoelectric stacks are used, but it is a big issue is voice coils are used.
An alternative would be to accept that the nano-hexapod experiences some static deflection.
With a vertical nano-hexapod stiffness $\approx 10^6\,[N/m]$, the maximum static deflection would be:
\[ k_z \approx 10^6\,[N/m] \longrightarrow \Delta z = \frac{\Delta m g}{k_z} \approx 0.5\,[mm] \]
This will change a little bit the architecture of the nano-hexapod but this should be too small to change significantly the dynamics.
** Sensor Noise introduced by the Metrology
Say that is will introduce noise inside the bandwidth (100Hz)

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@ -63,3 +63,10 @@
doi = {10.1016/j.jsv.2006.07.050},
url = {https://doi.org/10.1016/j.jsv.2006.07.050},
}
@techreport{collette11_review,
author = {Collette, C and Artoos, K and Guinchard, M and Janssens, S and Carmona Fernandez, P and Hauviller, C},
institution = {cern},
title = {Review of sensors for low frequency seismic vibration measurement},
year = {2011},
}