Exhuded LiF ribbons (3.1 x 3.1 x 0.9 mm') and rods (6 x 1 x I mm3) we commonly used thermoluminescence dosimeters (n dosimeters) for clinical dosimetry in radiotherapy. The dose distribution in these crystals was investigated in a 6 MV x-ray beam using s d e z LiF n dosimeter types (thin ribbons with a thickness of 0.14 mm and small cubes with 1 nun side length). Using the thin ribbons, the effective depth of measurement in the normal ribbons was found to be shifted towards the surface. Measuring on the surface of a solid water phantom in a IO x 10 emz field it was found to be at a depth of 0.4 mm as compared to the physical centre of the ribbons of 0.44 mm. In the investigations with small cubes assembled in form of ribbons and rods it was found that a higher &se was deposited in the centre of the ribbons and mds. Accordingly it was found that n. dosimeters in close contact w i t h each other increase their respective reading. Using two ribbons in contact with each other on the surface of a phantom leads to an overestimation of dose of about 1%. The specific dose response of LiF increases with dosimeter size. this is most likely due to increased e l m " scatter from the additional LiF material with density higher than unity. This emphasizes the role of n dosimeters as relative dosimeters where siandards of equal size and geamey should be used to evaluate the readings.