In this document, we wish to estimate the centrifugal forces due to the spindle's rotation when the sample's center of mass is off-centered with respect to the rotation axis.
This is the case then the sample is moved by the micro-hexapod.
The centrifugal forces are defined as represented Figure [[fig:centrifugal]] where:
- $M$ is the total mass of the rotating elements in $[kg]$
- $\omega$ is the rotation speed in $[rad/s]$
- $r$ is the distance to the rotation axis in $[m]$
The mass of the sample can vary from $1\,kg$ to $50\,kg$ to which is added to mass of the metrology reflector and the nano-hexapod's top platform (here set to $15\,kg$).
#+begin_src matlab
M_light = 16; % mass of excentred parts mooving [kg]
M_heavy = 65; % [kg]
#+end_src
For the light mass, the rotation speed is 60rpm whereas for the heavy mass, it is equal to 1rpm.
#+begin_src matlab
w_light = 2*pi; % rotational speed [rad/s]
w_heavy = 2*pi/60; % rotational speed [rad/s]
#+end_src
Finally, we consider a mass eccentricity of $10\,mm$.
#+CAPTION: Centrifugal forces function of the rotation speed
#+RESULTS:
[[file:figs/centrifugal_forces_rpm.png]]
* Maximum rotation speed as a function of the mass
We plot the maximum rotation speed as a function of the mass for different maximum force that we can use to counteract the centrifugal forces (Figure [[fig:max_force_rpm]]).
From a specified maximum allowed centrifugal force (here set to $10\,[N]$), the maximum rotation speed as a function of the sample's mass is shown in Figure [[fig:max_force_rpm]].