The new low density polyethylene (LDPE) obtained under low pressure in the reactor, the so-called low pressure low density polyethylene (LLDPE), with a great many short branches seems to replace the conventional LDPE with long branches obtained in the reactor under high pressure (high pressure LDPE = HLDPE). It has a higher tensile strength, impact strength, elastic modulus, elongation at break, and resistance to heat and stress cracking. The replacement goes on in film extrusion, blow molding, and wire and cable coating. The material seems also to be a good mixing component in polymer blends. ' The most obvious physical differences between the short and long branch LDPE are the higher crystallinity and the narrower molecular weight distribution, higher melting temperature (122O instead of 108"), and a narrower melting range in the former than in the latter case.The thicker and more perfect crystals are the main cause of these changes. The higher melting point, however, means a higher processing temperature that may be more harmful to the material and require a higher energy input.The increased technical interest in this type of material prompted us to investigate the mechanical and transport properties of Dowlex 2045, a Dow Chemical made LLDPE with a density 0.9139 g/cm3 that corresponds to a, = 0.414. This is less than the density 0.9152 g/cm3 of the formerly investigated conventional HLDPE with a, = 0.423. The ratio 10-35 of side chain ends CH3 per 1000 CH2 on the backbone and side chains of the molecule indicates a large number of side chains. According to the producer the side chains are much shorter than in the conventional HLDPE. (Certain commercial material is identified in this paper in order to adequately specify the experimental procedure. In no case does such identification imply recommendation or endorsement by the National Bureau of Standards, nor does it imply that the material identified is necessarily the best available for the purpose.)The enormous elastic modulus of the crystals as compared with that of the amorphous component makes the mechanical properties of the semicrystalline polymer depend primarily on the fraction of taut tie molecules crossing the amorphous layers and on the mechanical properties of these layers. Although they are in the rubbery state, the amorphous molecules are so intimately bound to the crystals that the properties of the amorphous component substantially deviate from those of a completely amorphous rubber. In particular the specific volume of the amorphous component changes upon straining. Instead of the shear modulus G one must introduce the about 1000 times higher expansion modulus K of the rubber.The best method for the investigation of the amorphous component is the measurement of the transport properties. In first approximation they depend on the fractional free volume. It increases with the deformation if the specific volume does the same. The plastic deformation of drawing. however, reduces quite substantially the specific volume and hence the transport pr...