Liquids
confined to sub-millimeter scales have remained poorly
understood. One of the most striking effects is the large elasticity
revealed using good wetting conditions, which grows upon further decreasing
the confinement length, L. These systems display
a low-frequency shear modulus in the order of 1–103 Pa, contrary to our everyday experience of liquids as bodies with
a zero low-frequency shear modulus. While early experimental evidence
of this effect was met with skepticism and abandoned, further experimental
results and, most recently, a new atomistic theoretical framework
have confirmed that liquids indeed possess a finite low-frequency
shear modulus G′, which scales with the inverse
cubic power of confinement length L. We show that
this law is universal and valid for a wide range of materials (liquid
water, glycerol, ionic liquids, non-entangled polymer liquids, isotropic
liquids crystals). Open questions and potential applications in microfluidics
mechanochemistry, energy, and other fields are highlighted.