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The Polyethylene Family Tree How Density And Comonomer Define Every Pe Grade

The Polyethylene Family Tree: How Density and Comonomer Define Every PE Grade

Polyethylene is not a single material but a structural family in which solid-state density, short-chain branch architecture, and molar mass distribution determine processing behavior and end-use performance. The primary classification variables are density measured according to ISO 1183-1:2019 or ASTM D792, comonomer type and placement, and melt flow rate measured by ISO 1133-1:2022. Density extends from approximately 0.880 g/cm³ for very-low-density ethylene copolymers to 0.965 g/cm³ for high-density homopolymers. The phrase “The Polyethylene Family Tree: How Density and Comonomer Define Every PE Grade” identifies the central principle that short-chain branches reduce crystallinity and solid-state density, while long-chain branches alter shear thinning, extensional viscosity, and melt strength.

What Structural Variables Determine Family Membership in Polyethylene?

At the molecular level, high-density polyethylene grades typically contain fewer than 5 short-chain branches per 1000 backbone carbon atoms, while linear low-density polyethylene grades contain 10 to 30 short-chain branches per 1000 backbone carbon atoms introduced by alpha-olefin insertion. The alpha-olefin comonomer may be 1-butene, 1-hexene, or 1-octene. With Ziegler-Natta catalysts, comonomer incorporation is biased toward shorter chains, producing a broad chemical composition distribution and a measurable low molar mass extractable fraction. Metallocene catalysts produce a narrower chemical composition distribution, with comonomer distributed more uniformly across the molar mass distribution. This difference influences low-temperature seal performance, blocking, and compliance with FDA 21 CFR 177.1520 for food contact. Density is depressed approximately linearly with increasing comonomer content because each branch interrupts crystallizable ethylene sequences. The relationship is not only total comonomer but also branch length: longer branches create larger excluded volume and more effective disruption of orthorhombic crystalline unit cells, as observed by wide-angle X-ray scattering using the 110 and 200 reflections.

Table 1. Commercial polyethylene family boundaries based on density, comonomer, and melt flow rate
Grade Density range Typical comonomer Melt flow rate range Defining property
VLDPE/ULDPE 0.880–0.915 g/cm³ 1-butene, 1-hexene, 1-octene 0.5–25 g/10 min high dart impact, low modulus
LLDPE 0.915–0.940 g/cm³ 1-butene, 1-hexene, 1-octene 0.5–50 g/10 min tensile strength, tear, puncture resistance
LDPE 0.917–0.935 g/cm³ none; long-chain branching 0.2–70 g/10 min melt strength, optical clarity, processability
MDPE 0.926–0.940 g/cm³ 1-hexene 0.2–50 g/10 min balance of impact, stiffness, ESCR
HDPE 0.941–0.965 g/cm³ none or <1 mol% 0.1–80 g/10 min stiffness, chemical resistance, barrier

In high-pressure tubular and autoclave reactors operating at 150 MPa to 350 MPa and 150 °C to 350 °C, ethylene undergoes free-radical polymerization to low-density polyethylene. The resulting long-chain branch frequency, typically 0.5 to 3 long-chain branches per 1000 carbon atoms, generates broad molecular weight distribution and high melt strength without alpha-olefin comonomer. Density is controlled by reactor pressure, temperature, and chain-transfer agent concentration. Autoclave LDPE grades are used for extrusion coating because the broad molecular weight distribution delays draw resonance at line speeds above 300 m/min. Tubular LDPE grades are preferred for high-clarity film because higher conversion and lower gel contamination improve optical properties. The density range of 0.917 g/cm³ to 0.935 g/cm³ is therefore not defined by comonomer content but by long-chain branch concentration and molar mass distribution.

Bimodal Molar Mass Distribution and Slow Crack Growth Resistance in Pipe Grade PE 100

Pipe grade PE 100 is classified by hydrostatic design basis according to ISO 9080:2012 and material designation according to ISO 12162, requiring a minimum required strength of 10 MPa at 20 °C for 50 years. Commercial bimodal HDPE achieves this through a low molar mass, high-density fraction that reduces melt viscosity and a high molar mass fraction with 1-hexene or 1-butene comonomer to raise tie molecule concentration. The high molar mass fraction increases slow crack growth resistance because tie molecules bridge adjacent lamellae and restrain craze propagation. Slow crack growth is measured by the Pennsylvania Edge Notch Tensile test per ASTM F1473 at 80 °C and 2.4 MPa; PE 100 grades typically exceed 500 h to 1000 h before brittle failure, while older unimodal PE 80 grades may fail below 100 h under identical loading. Notched pipe testing per ISO 13479 and full-scale creep testing per ISO 9080 are used to validate the 50-year extrapolation. The comonomer type matters: 1-hexene produces longer short-chain branches than 1-butene, which improves the formation of tie molecules under slow crack growth. Production-scale observation on grooved-feed single-screw extruders with 30:1 to 36:1 L/D shows that bimodal PE 100 can exhibit melt pressure fluctuations below 1.5% when the feed zone is cooled to 60 °C to 80 °C and the metering zone is held at 190 °C to 220 °C.

When Short-Chain Branch Length Increases from Butene to Hexene to Octene

For blown film produced on a 250 mm die diameter line with 1.8 mm die gap, 2.5:1 blow-up ratio, and dual-lip air ring, interchanging comonomer at constant 0.918 g/cm³ density and 1.0 g/10 min melt flow rate changes the mechanical property balance. Longer branches increase the probability that a branch is incorporated into a tie molecule or entangled loop rather than rejected into the amorphous layer. This shifts dart impact strength measured by ASTM D1709 method A and Elmendorf tear measured by ASTM D1922 upward from butene to hexene to octene. Table 2 summarizes representative ranges compiled from resin supplier technical bulletins for 25 µm monolayer films containing standard antioxidant packages. Published data for specific additive packages and film line configurations is limited, but the direction of property change is consistent across suppliers.

Table 2. Representative property ranges for LLDPE film grades at 0.918 g/cm³ and 1.0 g/10 min
Comonomer Dart impact, ASTM D1709 method A Elmendorf tear MD Elmendorf tear TD Seal initiation temperature
1-butene 80–150 g 150–250 gf/25 µm 250–350 gf/25 µm 105–115 °C
1-hexene 120–250 g 200–350 gf/25 µm 300–450 gf/25 µm 100–110 °C
1-octene 200–400 g 250–450 gf/25 µm 350–550 gf/25 µm 95–105 °C

Seal initiation temperature in Table 2 is determined according to ASTM F88 with 0.5 s dwell and 2.8 bar jaw pressure. The reduction in seal initiation temperature from butene to octene is caused by greater melting point depression at equivalent density. Hot tack strength follows a similar trend, although additive migration and film slip agents can mask differences on high-speed packaging lines. Film processors also observe that octene-grade LLDPE generates higher melt elasticity than butene-grade resin at fixed melt index, requiring wider die gaps or higher melt temperature to control bubble stability.

For thick-wall HDPE pressure pipe extruded on grooved-feed single-screw machines with 30:1 to 36:1 L/D and screw diameters from 75 mm to 150 mm, the melt flow rate typically ranges from 0.2 g/10 min to 0.5 g/10 min for PE 100. Low melt index increases sag resistance during vacuum-tank sizing, but also raises melt fracture risk. Capillary rheometry per ISO 11443 shows that the onset of sharkskin for linear HDPE occurs at wall shear stresses of 0.1 MPa to 0.3 MPa. Pipe producers control this by raising die temperature, lowering line speed, or widening the die gap; melt temperature above 230 °C accelerates thermo-oxidative degradation if the antioxidant package is insufficient. Melt pressure before the screen pack is often held below 35 MPa to prevent screen rupture. Field failure modes include annular weld-line weakness from poorly designed spiral mandrel dies and sag-induced wall thickening at the pipe invert.

Density and flexural modulus rise together, but environmental stress crack resistance moves in the opposite direction

Blow molding grades for industrial containers are formulated in a narrow density window of 0.949 g/cm³ to 0.955 g/cm³ and melt flow rates of 0.2 g/10 min to 0.35 g/10 min at 190 °C and 2.16 kg load. Raising density from 0.949 g/cm³ to 0.955 g/cm³ increases flexural modulus by approximately 150 MPa to 200 MPa as measured by ASTM D790, but reduces environmental stress crack resistance measured by ASTM D1693 condition B in 10% Igepal CO-630. For a 25 L HDPE jerrican, a resin with density 0.951 g/cm³ typically provides a flexural modulus near 1100 MPa and ESCR values above 100 h; increasing density to 0.958 g/cm³ may drop ESCR below 30 h. The addition of 1-butene or 1-hexene at low levels restores ESCR by increasing tie molecule density but lowers top-load crush strength. Blow molding machine behavior further depends on parison swell: broad unimodal resins produce higher die swell and improved pinch-off weld strength, while bimodal resins provide better parison hang strength and allow 5% to 10% weight reduction without wall-thickness variation.

Selecting Melt Index and Comonomer Type for Rotational Molding Versus Injection Molding

Rotational molding uses ground powder with particle size typically 35 mesh to 50 mesh and melt flow rates between 3 g/10 min and 6 g/10 min at 190 °C and 2.16 kg. The low melt index is needed to prevent pinholes during the long oven cycle, while the narrow particle size distribution prevents skinning defects on the mold surface. A mold temperature of 200 °C to 250 °C for 30 min requires thermal stabilizers with high extraction resistance, typically validated under FDA 21 CFR 177.1520 for potable water tanks. Injection molding of thin-wall caps and closures uses higher melt flow rate HDPE or LLDPE, typically 20 g/10 min to 50 g/10 min, to fill short flow lengths at clamp pressures of 8000 kN to 12000 kN. The higher melt flow rate reduces molecular weight and tensile strength but permits cycle times below 10 s. Shrinkage measured by ISO 294-4 increases with density and decreases with flow direction; for HDPE at 0.952 g/cm³, typical parallel shrinkage is 1.8% to 2.2% and perpendicular shrinkage is 1.2% to 1.6%. Warpage in shallow caps occurs when density gradients from differential cooling exceed 0.002 g/cm³ across the part, a field tolerance derived from cavity-pressure and thermal imaging on production tools. Using 1-hexene at constant density improves impact strength in closures but may reduce top-load stiffness if density is not adjusted upward.

In extrusion coating of paperboard, low-density polyethylene grades with density 0.918 g/cm³ and melt flow rate 7 g/10 min to 15 g/10 min are processed through flat dies at melt temperatures of 290 °C to 320 °C. High melt strength from long-chain branching suppresses draw resonance and edge neck-in. High melt temperature increases low molecular weight oxidation products that can affect organoleptic performance; coatings intended for direct food contact require hexane extractables below 2.6 mg/dm² under FDA 21 CFR 177.1520. Moisture barrier performance measured by water vapor transmission rate per ISO 15106-3 at 23 °C and 85% RH is controlled by coating thickness and density, not by comonomer length.

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