We consider energies on a periodic set ℒ of the form \sum_{i,j\in\mathcal{L}}a^{\varepsilon}_{ij}\lvert u_{i}-u_{j}\rvert, defined on spin functions u_{i}\in\{0,1\}, and we suppose that the typical range of the interactions is R_{\varepsilon} with R_{\varepsilon}\to+\infty, i.e., if \lvert i-j\rvert\leq R_{\varepsilon}, then a^{\varepsilon}_{ij}\geq c>0.
In a discrete-to-continuum analysis, we prove that the overall behavior as \varepsilon\to 0 of such functionals is that of an interfacial energy.
The proof is performed using a coarse-graining procedure which associates to scaled functions defined on \varepsilon\mathcal{L} with equibounded energy a family of sets with equibounded perimeter.
This agrees with the case of equibounded R_{\varepsilon} and can be seen as an extension of coerciveness result for short-range interactions, but is different from that of other long-range interaction energies, whose limit exits the class of surface energies.
A computation of the limit energy is performed in the case \mathcal{L}=\mathbb{Z}^{d}.