The purpose of this work is twofold. First we extend the derivation of Boltzmann’s equation in [26] to the periodic setting Td (d = 2,3). Second, we connect this kinetic limit to the hydrodynamic limit in the abovecited works, to obtain a full derivation of the fluid equations starting from Newton’s laws on the particle system, thereby completing Hilbert’s original program. We summarize the main theorems as follows: • Theorem 1: Derivation of the Boltzmann equation on Td (d = 2,3). Starting from a Newtonian hard-sphere particle system on the torus Td (d = 2,3) formed of N particles of diameter ε undergoing elastic collisions, and in the Boltzmann-Grad limit Nεd−1 = α, we derive the Boltzmann equation (1.1) as the effective equation for the one-particle density function of the particle system. • Theorem 2: Derivation of the incompressible Navier-Stokes-Fourier system from Newton’s laws. Starting from the same Newtonian hard-sphere particle system on the torus Td (d = 2,3) close to global equilibrium, and in an iterated limit where first N → ∞, ε → 0 with α = Nεd−1 f ixed and then α → ∞ separately (there are also other variants, see Theorem 2), we derive the incompressible Navier-Stokes-Fourier system as the effective equation for the macroscopic density and velocity of the particle system. • Theorem 3: Derivation of the compressible Euler equation from Newton’s laws. Starting from the same Newtonian hard-sphere particle system on the torus Td (d = 2,3), and in an iterated limit where first N → ∞, ε → 0 with α = Nεd−1 fixed and then α → ∞ separately (there are also other variants, see Theorem 3), we derive the compressible Euler equation as the effective equation for the macroscopic density, velocity, and temperature of the particle system.