Example: Microrobot leg 3D. Introduction This model shows the movement of a silicon micro-robot leg...
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Transcript of Example: Microrobot leg 3D. Introduction This model shows the movement of a silicon micro-robot leg...
Example: Microrobot leg 3D
Introduction
• This model shows the movement of a silicon micro-robot leg due to thermal expansion as a function of time.
• The heat transfer and structural mechanics equations are solved sequentially in a time-dependent analysis.
– The heat transfer problem is a transient analysis while the structural problem is modeled in a quasi-static analysis.
• In order to reduce the degrees of freedom a geometry simplification was required for the 3D model removing two layers:
– The thin highly-conductive layer and poorly conductive layer are modeled with the thin conductive shell application mode from the heat transfer module and stiff spring temperature boundary conditions respectively.
– The shell element application from the structural mechanical module is used for modeling the mechanical part.
Geometry
Heating resistors
Cured polyamide (high thermal expansion coefficient)
Silicon leg
• The general heat transfer equation:
• The principle of virtual work for the structural mechanics
Domain Equations
QTk )(
dSdVdVS
t
V
t
V
t )()()( upupεσ sv
Boundary Conditions - heat
Highly conductive layer& stiff spring condition
Highly conductive layer onlyConvective flux
Convective fluxAll other boundaries have thermal insulation conditions
Boundary Conditions – structural mechanics
No displacement
Structural shell element including thermal expansion
All other boundaries are free to move
Results
• The microrobot leg bends due to the heating of the leg
Results
• The maximum displacement at the tip of the leg is 0.6 mm for a heat source of 2e13W/m3 during 9 ms.
Results
• The highly conductive layer and the stiff spring condition accurately model the thin layers.
Results - Animation
Conclusion
• A thermal stress analysis is straight forward to perform in the Structural Mechanics module
• Model shows the possibility to replace thin layers by a specific boundary condition, and save memory:
– Highly conductive layer boundary condition (already implemented)– Stiff spring condition to model a poorly conductive layer– Direct coupling of shell and solid element in structural mechanics
• Large transient multiphysics problem solve sequentially using quasi-static analysis and the manual definition of the linearization point.