PE-LLD: Polyethylene Linear Low Density

CTP

Commodity Thermoplastics

General Properties

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PE-LLD

Polyethylene Linear Low Density


Linear low density polyethylen (PE-LLD) is different from conventional low-density polyethylene (PE-LD, see previous page) in that it shows only short branching and significantly different rheological properties. PE-LLD is a copolymer with usually butylene, hexene or octene and is produced at lower temperatures and pressures than PE-LD.

Structural Formula


Properties

Glass Transition Temperature-130 to -100 / -70 to -25°C
Melting Temperature122 to 127°C
Melting Enthalpy-
Decomposition Temperature475 to 485°C
Young's Modulus250 to 700 MPa
Coefficient of Linear Thermal Expansion200 *10-6/K
Specific Heat Capacity-
Thermal Conductivity-
Density0.91 to 0.94 g/cm³
MorphologySemi-crystalline thermoplastic
General propertiesBalanced relationship of toughness and stiffness, good chemical resistance, good electrical insulating properties.
ProcessingExtrusion (films, profiles), injection moulding, blow moulding, extrusion-coating.
ApplicationsFilms (allows for lower film thickness than PE-LD), mainly in household and agriculture, packaging (e.g. containers and plastic bags), toys.

NETZSCH Measurement

InstrumentDSC 204 F1 Phoenix®
Sample Mass11.95 mg
Isothermal Phases20 min/2 min/20 min
Heating/Colling Rates10 K/min
CrucibleAl, pierced lid
AtmosphereN2 (40 ml/min)

Evaluation

The 1st heating (blue) exhibits a highly structured melting EndothermEin Phasenübergang oder eine Reaktion ist endotherm, wenn für die Umwandlung Wärme benötigt wird.endotherm with a main peak (at 119°C) and several upstream and downstream shoulders, reflecting the presence of stresses (thermomechanical history). In the 2nd heating (red), two peaks at approx. 112°C and 124°C remained. Due to side chain branching, different melting phases are formed which melt one after the other. The corresponding melting enthalpy in the 2nd heating amounts to approx. 137 J/g. Since PE-LLD is a semi-crystalline thermoplastic, the glass transition observed at -35°C (for both heatings) can be related to the amorphous component of the polymer. A second possible glass transition at approx. -100°C to -130°C, which could be due to the different crystallite structures, is not viewable in the plots shown.