In classical systems, we reexamine how macroscopic structures in equilibrium state connect with spatial constraint on the systems: e.g., volume and density as the constraint for liquids in rigid box, and crystal lattice as the constraint for crystalline solids. We reveal that in disordered states, equilibrium macroscopic structure, depending on temperature and on multibody interactions in the system, is characterized by a single special microscopic structure independent of temperature and of interactions. The special microscopic structure depends only on the spatial constraint. We demonstrate the present findings providing (i) significantly efficient and systematic prediction of macroscopic structures for possible combination of constituents in multicomponent systems, and (ii) unique and accurate determination of multibody interactions in given system from measured macroscopic structure, without performing trial-and-error simulation.Introduction.-Consider a classical system, where total energy (E) is the sum of kinetic energy (K) and potential energy (U) that is a function of positions for constituents. In equilibrium state, macroscopic structure can be uniquely specified when we define a complete set of coordinations (i.e., corresponding complete orthonormal basis functions), q 1 , . . . , q g . Statistical physics tells us that Q r , macroscopic structure along a chosen coordination of q r , can be typically given by canonical average: