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The snap-through phenomenon scenario is analyzed.
The arch motion exhibits a snap-through motion.
The snap-through piezoelectric energy harvester possesses the bistability.
Snap-through experiments are conducted and the ABAQUS finite element software is used to predict snap-through behavior.
We examined the mechanism of the snap-through mathematically.
No snap-through buckling is possible in this case.
Both snap-through and remote coexisting equilibria are observed.
The boundaries that separate the snap-through and no snap-through regions in the forcing parameters space are identified.
We call such a sharp transition the snap-through instability of graphene.
The h' is the 'enlarged' thickness, the result of smaller snap-through phenomenon.
The insets illustrate the two distinct states of graphene morphology at the snap-through instability.
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