The crystal structure of the so-called potassium decamolybdate, the formula of which has to be written as KMosOlsOH. 2H20, was determined from single-crystal diffractometer data. The compound crystallizes with hexagonal symmetry in the space group P63/m, the cell parameters being a= 10.550 (8), c--3-727 (3) ,~ and Z= 1. The structure has been solved from the Patterson function and chemical considerations and refined by full-matrix least squares to a conventional R of 0.042 based on 335 independent reflexions. The structure consists of double chains made of edge-sharing, strongly distorted MoO6 octahedra. The double chains are linked by common corners of octahedra to form a threedimensional network. The double chains are not perfect due to statistical non-occupation of one of the six equivalent Mo positions in the unit cell. Along the short c axis the polymeric structure forms tunnels in which the potassium ions are located. Mo-O bond lengths in the MoO6 octahedra are: 1.698, 1.701, 1.955 (2 x ), 2.190 and 2.373/~. The chemical composition and the observed interatomic distances lead to a plausible model of the structural disorder: In the neighbourhood of a vacant Mo position the O atoms are partially replaced by coordinated H20 molecules, isolated H20 molecules (crystal water), and OH groups. The statistical distribution of the Mo vacancies can be interpreted as resulting in smaller sub-units of edge-sharing octahedra linked in the direction of the double chains only by common corners. The structure is only weakly related to the structures of the other typical polymolybdates crystallizing from aqueous solutions. Closer relations are found to the structures of ~-MoO3.H20 and of MOO3.