On Shaky Ground: Characterising Non-Rigid Base Effects in Mobile Manipulation
Organizations: Faculty of Engineering, Queensland University of Technology, 2 George St, Brisbane, QLD 4000, Australia · Australian Cobotics Centre, Queensland University of Technology, 2 George St, Brisbane, QLD 4000, Australia · QUT Centre for Robotics, Queensland University of Technology, 2 George St, Brisbane, QLD 4000, Australia
Abstract
Mobile robot manipulators extend contact-task capability beyond the workspace of fixed robot installations, but their bases must also sustain the forces generated by the task. On lightweight platforms, base motion and support compliance can change the force and motion realised at the workpiece. How these non-rigid base effects manifest during sustained contact remains insufficiently characterised. This paper investigates non-rigid base effects in mobile robot manipulators through a sanding case study combining exploratory simulation with experiments on two lightweight, unactuated wheeled testbeds. Joint measurements of contact force, tool motion, and base vibration show that sustained contact coexisted with substantial task error: under low base-ground resistance, only 54-70% of a 100 N command was realised, with tool-centre-point errors reaching 100 mm. Increasing base-ground resistance during contact improved force realisation and arrested further tool displacement, while base vibration did not vary consistently with force-tracking error in the tested conditions. These observations illustrate how non-rigid base behaviour can affect contact-task execution and highlight the value of examining force, motion, and vibration together when characterising lightweight mobile manipulation.
Figures & tables
| Simulation | Cart | Trolley | |
|---|---|---|---|
| Arm | UR10 model | UR10 | UR5 |
| Base | Rigid wheels | Aluminium | Plywood |
| Support | Rigid floor | Concrete | Foam |
| Resistance | Varied | Low, high | Low, high |
| Sander speed | Varied | Low, high | High |
| Condition | Result | |||||||||||
| ID | Resistance | Posture | Speed | Slope | (m s -2 ) | |||||||
| (N) | (N) | (N) | (N) | (N s -1 ) | (mm) | med. | max | |||||
| Experiment 1 (cart) | ||||||||||||
| T1 | Low | Standard | Low | 100 | 58.8 | 0.59 | 41.5 | 2.6 | 0.42 | n/a | 0.19 | 0.69 |
| T2 | Low | Low | Low | 100 | 68.3 | 0.68 | 32.1 | 3.7 | 0.32 | n/a | 0.08 | 0.12 |
| T3 | High | Standard | Low | 100 | 94.3 | 0.94 | 6.9 | 3.2 | 0.21 | n/a | 0.29 | 0.77 |
| Aspect | Simulation | Hardware observations |
|---|---|---|
| Base motion | Slip when the required wheel–ground tangential forces exceed the available traction | About 100 mm TCP error at low resistance (T5–T7), accompanied by of 0.54–0.70 (T1, T2, T5–T7), on both platforms |
| Posture sensitivity | Extended posture increases excitation and reduces the stability margin | Low posture reduced median base vibration from 0.19 to 0.08 m s -2 and raised from 0.59 to 0.68 (T1, T2) |
| Base–ground interaction | Higher wheel friction suppresses slip | High resistance raised to 0.88–1.01 on both platforms (T3, T5, T6, T8); the switch arrested TCP-error growth within about 1 s (T5, T6) |
| Oscillation / tool excitation | Tool excitation produced tool and base oscillation; tool speed shifted the dominant frequency | High tool speed produced substantially higher base vibration than low tool speed, both out of contact and at high resistance (T5, T6) |
| Support compliance | Not represented in the rigid-wheel model | Foam nearly tripled median base vibration relative to the hard floor (Figure 7 ) |
| Loss of stability | Occurred when the zero-moment point moved outside the support polygon | Not reached |
Mobile Manipulation
Mobile manipulation studies robots that navigate through environments while using arms or other effectors to interact with objects.
See all 92 papers