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. 2018 May 8;8(30):16674–16689. doi: 10.1039/c8ra01302k

Fig. 4. (a) Evolution, with the aging time upon a tensile-unloading (to zero stretch) cycle, of the hysteresis loop re-formed from the cycle for a poly(vinyl alcohol) (PVA)/alginate sequential, hydrogen-bonded-ionic dual-physical double-network (DN) hydrogel of maximum mechanical properties (tensile strength, elongation at break and toughness) having a mole ratio of the PVA- to Na alginate repeat units of 60/1 and Ca-dicarboxylate ionic cross-links of the minor dispersed alginate networks dramatically denser than the hydrogen bond cross-links of the major global PVA network. To conduct the experiments, five fresh parallel specimens of the gel first undergo a tensile-unloading cycle of 1.0 mm mm−1 stretch at a crosshead speed of 50 mm min−1 at room temperature (RT) (∼25 °C), then stand in a large amount of CaCl2 aqueous solution of 1.0 mol L−1 (i.e. age at the sacrifice of neither their water content nor cross-link morphology) at RT for increasing times of 0, 2, 10, 25 and 60 min, respectively, and are finally subjected to the tensile-unloading cycle again. Since the five fresh parallel specimens exhibit similar hysteresis loop profiles to each other, only the hysteresis loop of the fresh specimen to be subsequently aged for 0 min is shown as the initial one (i.e. control) for analysis; and, exceptionally, the hysteresis loop of the gel on 0 min of aging is realised by the tensile-unloading cycle run in situ immediately after the control, with the specimen kept gripped as it is and actually not immersed into the CaCl2 solution for aging. (b) Percent recoveries of the Young's (i.e. tensile elastic) modulus, E, and dissipated energy, Uhys, towards those of the control as functions of the aging time for the PVA/alginate DN hydrogel of the maximum mechanical properties, where the E of all the loops (including the control) was read as the slope at the onset (i.e. non-zero stress) point of their tensile curve and the Uhys estimated as their area from (a).

Fig. 4