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. 2015 Sep 29;112(41):12563–12568. doi: 10.1073/pnas.1502642112

Fig. 2.

Fig. 2.

Bulging profile ψ of thin skin of an elastic film embedded with liquid-filled channels. (A) Curves 1–7 represent liquids: (1) acetonitrile (filled-in channel of diameter d=450 µm, embedded in film of thickness h=467 µm and minimum skin thickness, t0=17 µm); (2) nitromethane (d=450 µm, h=480 µm, and t0=30 µm); (3) DMSO (d=180 µm, h=185 µm, and t0=5 µm); (4) perflurooctane, (d=180 µm, h=204 µm, and t0=24 µm); (5 and 6) ethylene glycol, air (d=450 µm, h=468 µm, and t0=18 µm); and (7) water (d=450 µm, h=480 µm, and t0=30 µm), respectively. (B) Two liquids are injected alternatively into the channel. Bulging deflection ψ of the channel skin flips from 1 to 1′ as nitromethane, initially present in the channel, is replaced by injecting water into it. The profile flips back to 2 as water is similarly replaced by nitromethane. This process is repeated 4–5 times, without any signature of irreversibility or hysteresis. A film embedded with channel of diameter d=550 µm and minimum skin thickness t=35 µm is used in this experiment.