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. 2016 Aug 12;113(35):9722–9727. doi: 10.1073/pnas.1604838113

Fig. S7.

Fig. S7.

Because the system is deformable, different values of d can be used along the length of the system, resulting in spatially varying energy barriers to propagation; this can be used to vary the velocity along the length of the chain, as it is here for a gradient structure (d is about d1=14.5 mm at the left end and about d2=19.0 mm at the right end, corresponding to measured speeds of 0.8 and 5.2 m/s, respectively).