If the attenuation function of strain is expressed as a power law, the formalism of
fractional calculus may be used to handle Eringen non-local elastic model. Aim of the present
paper is to provide a mechanical interpretation to this non-local fractional elastic model by
showing that it is equivalent to a discrete, point-spring model. A one-dimensional geometry is
considered; static, kinematic and constitutive equations as well as the proper boundary conditions
are derived and discussed