The crystal structure of the organic metal TTT2I 3 has been determined at room temperature from X-ray diffraction data collected on a diffractometer. The crystals are orthorhombic, Abam, with a = 18.394 (12), b = 4.962(5), c = 18.319(11) ,~, dm= 2.16, de = 2.156 g cm -3, Z = 2. Diffuse streaks on precession photographs indicate a disordered lattice incommensurate along b with b' = 9.54 A = 1.92 b. The structure was solved in the subcell by Patterson and Fourier methods and refined by full-matrix least-squares calculations to R 1 = 0-042. The structure consists of planar TTI" radical cations with 2/m crystallographic symmetry stacked uniformly along b, the axis of high electrical conductivity, with a 3.32 ,~, interplanar spacing and a ring-bond overlap. A short S... S contact [3-373 (2) A[ links stacks in (100)planes. The I atoms are present as triiodide ions lying in chains along 2b axes parallel to the TTT stacks. For some crystal domains the triiodide ions lie on the incommensurate lattice but for others they are forced to conform to the subcell dimensions by a close hydrogen approach. The dual nature of the triiodide ions also causes a possible disorder in the TTT moieties. These disorders are possibly the reason no metal-insulator transitions are observed down to3.3 K.