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shape- memory effect, the chains stop moving in a par- tially oriented conformation. In an entropy wheel41, a reversible contraction and elongation of a series of rub- ber spokes generates mechanical energy from a ther- mal gradient. The scale of the coordinated molecular reorientation of an amorphous domain provides a suf- ficient driving force to generate macroscale deformation without the need for crystallizable actuation domains. The actuation is caused purely by entropic change. The function of geometry- determining domains, supply- ing the network anisotropy required to link molecular orientation to macroscale movement, is substituted by constant external stress on the system. This analogy raises the question of whether crys- tallization is necessary for a free- standing reversible shape- memory actuator. In the entropy wheel and in numerous other LCE materials7,42,43, a sufficient energetic gain can be generated by macromolecular entropic changes without the need for crystallization and melting. However, the key challenge is to ensure that this energy release results in a macroscopic shape change. Orientation needs to direct the volume change; otherwise, crystallization does not result in coordinated network deformation. The entropy wheel uses external stress, which makes actuation neither programma- ble within the same material nor free- standing. As an alternative to crystallizable geometry- determining domains, molecular switches may provide the network anisotropy necessary to guide the alignment of the actu- ation domains while also enabling programmable and reprogrammable deformation. Characterization One- way shape- memory effect. Macroscale mechan- ical testing can be performed to quantify the shape- memory effect. The shape- recovery ratio Rr and shape fixity ratio Rf are two of the most important character- istic quantities for one- way shape- memory materials. The shape- recovery ratio Rr indicates the effectiveness of the recovery process, given by the amplitude ratio of the original shape to the recovered shape. The shape fixity ratio Rf provides an indication of the program- ming efficacy, given by the amplitude ratio of the fixed deformation εu to the total deformation εm. Cyclic thermomechanical testing is the most widely applied method for the determination of these values. Using a conventional mechanical testing apparatus equipped with a thermochamber, a single, fixed exper- imental setup can be used to simultaneously control the stress, strain and temperature during programming and recovery5. Three approaches to material deformation, known as compression44,45, bending46,47 and tensile test- ing, are the most prevalent for shape- memory materials. Combined with more complicated approaches, such as shear deformation48 and torsion49, these tests can provide a thorough thermomechanical description of a single material. The relative simplicity and unidirectional nature of tensile testing further make this method applicable to modelling50,51 and have led to its widespread use. The results of cyclic thermomechanical testing are usually presented in a stress–temperature–strain graph, allowing the visualization of mechanical behaviour at a b c d One-way shape-memory effect Time (min) T (° C ) ε ( % ) 60 40 20 0 Time (min) 1,000 800 1,200 200 600 400 100 100 400300200 100 400300200 Recovered shape T reset T low Temporary shape Temperature (°C) ε ( % ) σ (M Pa ) σ max σ m σ max σ Tσ,inf Tσ,max Tσ,max ΔT rec ε u ε ΔT rec T SW Temperature (°C) Covalent network Thermoplast Covalent network Thermoplast ε p ε p T low T reset T→ 2 3 4 ε u ε m ε p 1 ε Stress-free recovery Constant-strain recovery 1 2 3 41 2 3 4 T low T reset T reset T reset T reset T low T low T low Fig. 3 | Quantification of a one- way shape- memory effect. a | The stress (σ)–temperature (T )–strain (ε) graph of a cyclic thermomechanical tensile test illustrates the complete one- way shape- memory cycle, including programming, fixation and recovery , as obtained by macroscale measurements. For programming (shape- memory creation procedure (SMCP)), the sample is heated to Treset with an elongation- to-extension εm (resulting in stress σm) (1) and then cooled to Tlow, while εm is kept constant for fixation of the temporary shape (2); the fixed temporary shape at εu is obtained from the unloading of the sample to zero stress at Tlow (3); after the temporary shape is fixed, the recovery process can be initiated by heating the sample to Treset (4); and the recovery strain εp is obtained after full recovery of the sample. b | Cyclic testing. The reliability of the programming and recovery cycle for a one- way shape- memory effect can be tested by repetitive measurements. ε and T cycles of the temporary and recovered shapes are shown. c | A schematic programming procedure with stress- free recovery is shown in orange. The black arrows in the sample schemes indicate the applied strain ε. Schematic recovery curves are shown for a thermoplastic polymer and a covalent network with no external stress applied during the recovery process. The switching temperature TSW is the inflexion point, representing the highest recovery rate (ΔTrec). d | Schematic SMCP with constant strain is shown in green. The red arrows indicate the direction of recovery of the material. Constant strain is applied during the recovery process. The maximum strain σmax and the temperature at maximum strain Tσ,max can be determined from the temperature–stress diagram. Tσ,inf is defined as the temperature at the inflexion point of the stress curve. Panels a, c and d are adapted from Sauter, T. et al. Quantifying the shape- memory effect of polymers by cyclic thermomechanical tests. Polymer Rev. 53, 6–40 (2013) reF.128, by permission of the publisher (Taylor & Francis). Panel b is adapted with permission from reF.129, Wiley- VCH. Nature reviews | Materials R e v i e w s http://www.tandfonline.com Reprogrammable recovery and actuation behaviour of shape-memory polymers Characterization One-way shape-memory effect. Fig. 3 Quantification of a one-way shape-memory effect.
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