We report the optical spectra and single crystal magnetic susceptibility of the one-dimensional antiferromagnet KFeS2. Measurements have been carried out to ascertain the spin state of Fe a ÷ and the nature of the magnetic interactions in this compound. The optical spectra and magnetic susceptibility could be consistently interpreted using a S = ½ spin ground state for the Fe 3 ÷ ion. The features in the optical spectra have been assigned to transitions within the d-electron manifold of the Fe 3 ÷ ion, and analysed in the strong field limit of the ligand field theory. The high temperature isotropic magnetic susceptibility is typical of a low-dimensional system and exhibits a broad maximum at ~ 565 K. The susceptibility shows a well defined transition to a three dimensionally ordered antiferromagnetic state at T N = 250 K. The intra and interchain exchange constants, J and J', have been evaluated from the experimental susceptibilities using the relationship between these quantities, and X,~ax, T~,x, and Ts for a spin ½ one-dimensional chain. The values are J = -440.71 K, and J' = 53"94 K. Using these values of J and J', the susceptibility of a spin ½ Heisenberg chain was calculated. A non-interacting spin wave model was used below T s. The susceptibility in the paramagnetic region was calculated from the theoretical curves for an J infinite S = ~ chain. The calculated susceptibility compares well with the experimental data of KFeS 2. Further support for a one-dimensional spin ½ model comes from the fact that the calculated perpendicular susceptibility at OK (2.75 × 10-4emu/mol) evaluated considering the zero point reduction in magnetization from spin wave theory is close to the projected value (2'7 × 10 -4 emu/mol) obtained from the experimental data.