SynopsisA device for measuring the elasticity of polymer melts: has been designed by one of us (B. Maxwell). The device was used to obtain the relaxation modulns in shear of a linear polyethylene melt. From these data a discrete relaxation spectrum was derived. The range of the obtained spect,rum was confirmed to correspond to the terminal zone of the "entanglement plateau" of the spectrum. The limiting dynamic viscosity (as frequency approaches zero) was obtained by integrating the relaxation modulus with respect to time. The viscosity and its activation energy were found to agree closely with the flow viscosity and the flow activation energy, respectively, involved in capillary flow.Even though it is well known that polymer melts are generally viscoelastic, in their flow studies they are often treated as if they are purely viscous liquids. This oversimplification is particularly serious in some materials where the elastic response to an external force is of the same magnitude as the viscous response. In processing polymeric materials, for example, there is a strong indication that the elastic energy plays an important role in melt the extent to which strains are frozen into the final product ifi also related to the elastic contribution and affects the mechanical properties of the solid.While there is a very large amount of data available on the flow viscosity of polyethylene melt^,^'-^ only a few investigations have been carried out on the viscoelastic properties within the linear range. ' We have constructed a device suitable for making measurements of stress relaxation on a polymer melt at elevated temperatures. In stress relaxation a strain is applied and held constant while the decaying stress is measured as a function of time. Hence, the possibility of errors arising from friction, as in a creep experiment, is eliminated. If the strain is kept small enough, the mathematics developed for linear viscoelasticity is applicable, thus simplifying the analysis and practical application of the data.The device for performing stress relaxation experinients in shear is shown in Figure 1. The sample is premolded in the form of two hollow cylinders. I t is then loaded in the apparatus and melted under nitrogen atmosphere. The shear strain is applied by rotating the inverted cup.