Figure 1.7 shows a sketch of the apparatus known as Lee's Disc. Its purpose is the measurement of the thermal conductivity of a poorly conducting material.
The material is in the form of a disc so that the surface area A is large, and the temperature gradient d
/ dx is also large.
Since the rate of heat transfer is given by ( dQ / dt ) = -( (k.A.d
) / (dx) ), and the thermal
conductivity k is small, making A and d
/ dx large enables there to be a sizeable
heat flow through the material. The source of heat can be steam or electricity. The disc is sandwiched between two highly conducting slabs make of brass or copper. It is assumed that all the heat passing through the thin disc of material is lost through the surface of the lower slab. To measure this heat loss, the disc is removed and the slabs suspended one on top of the other. They are in the same conditions as before, except that they are heated to temperature about 20°C above that of the lower slab during the main experiment. By measurments on the slabs as they cool, the rate of heat loss corresponding to that of the main experiment can be determined.