# A Class 1 Tensegrity Robot

### Structural Systems and Control Laboratory

Home | Overview | Simulation of Concept | Experimental Hardware | Videos

## Overview

Tensegrity structures consist of tendons (in tension) and bars (in compression). Tendons are strong, light, and foldable, so tensegrity structures have the potential to be light but strong and deployable. Pulleys, NiTi wire, or other actuators to selectively tighten some strings on a tensegrity structure can be used to control its shape. This experiement shows the problem of asymmetric reconﬁguration of tensegrity structures and poses one method of ﬁnding the open loop control law for tendon lengths to accomplish the desired geometric reconﬁguration. In addition, a practical hardware experiment displays the readiness and feasibility of the method to accomplish shape control of the structure.

### Symmetrical Deployment

An interesting application of this tensegrity is the controlled deployment of the structure from a near zero initial height to a greater height. Moving along the equilibrium manifold (shown in Figure 1) consists of moving along symmetrical prestressable conﬁgurations. We use an open loop control strategy based upon slowly moving from one stable equilibrium to another. Stability along the deployment path is assured only if this movement is slow enough.

Figure 1 - Deployment Concept with Equilibrium Surface

### Asymmetrical Reconfiguration

Unfortunately, one shortcoming of the symmetrical parameterization for the two stage structure described is that the top and bottom triangles (top and bottom plates) are always parallel to each other and cannot deviate from that condition. In addition the center of mass of both plates is always aligned with the axis of symmetry. This is due to the fact that all bars are assigned the same parameter, therefore making the structure completely symmetric and representable by merely three parameters. If one wishes to modify the attitude or deviation of the top plate’s center of mass away from the axis of symmetry, one has to abandon the symmetrical parameterization and investigate the possibilities in the asymmetric space. The asymmetrical parameterization involves using the maximum number of parameters to describe the structure, as opposed to the minimal set previously. Therefore, six independent parameters will be assigned to each bar member, increasing the parameter space to thirty-six. An investigation into the allowable space for each parameter would result in an equilibrium manifold represented by thirty-six parameters which is not practical. (We assume later that bar length is constant for all bars, reducing to ﬁve parameters per bar or thirty parameters total.) Due to the increase in independent parameters, the equilibrium manifold has become immensely large and a search to characterize this space would most likely be fruitless and yield no special insight. It is obvious that the symmetric parameterization is a special case of the asymmetric one.

For further details consult the following publications: