BEAMbot
Bistable Electromagnetically Actuated Modular robots
How much controllable locomotion can emerge when electronics selects where and when bistable cells snap?
Each cell is a vacuum-formed PETG shell with laser-cut flexures, permanent magnets, a coil and a mechanical stop. Its geometry sets the force response. Bistability stores the state and elastic energy without holding current, and a short pulse triggers the snap. Across modules, the choice of which cells snap and when turns discrete states into whole-body motion. The tethered three-module robot moves forward and turns this way.
- Stroke
- 19.0± 0.6 mm
- 10-mm shell, 0.3-mm PETG
- Set / reset force
- 0.54/0.27N
- mean ± SD, 3 specimens × 3 cycles
- Jump clearance
- 22mm
- electrically triggered; 35-mm hub rise
- Gaits
- 3
- forward, left and right turns, all from actuation timing
My roleI developed the thermoforming and post-form laser-cutting process for the curved bistable cells. I also worked on magnet–coil switching, built single- and multi-module prototypes and their drive electronics, and ran the mechanical and switching characterization.
Open questions
- How can shape program mechanics? Calibrated FEA and repeated mechanical tests will link dome shape, flexure pattern and crease condition to the stable states and actuation requirements.
- How do arrangement and timing compose motion? Placement, orientation, activation order and phase will be varied to find repeatable translation and turning.
- How can actuation get lighter? Off-center magnets and multilayer flexible-PCB coils will be weighed against switching force, pulse energy, heating and mass, working toward untethered modules.
- How can modules change capability? Interchangeable mechanical cells and electronic “lids” could allow local control with shared power.
With Paul Ducarme and Lucia Stein-Montalvo · PI: Nivedita Arora · First author Manuscript in preparation