Non-Newtonian Rheology: Power-Law & Carreau-Yasuda Models for Polymer Melts
Polymer melt rheology, shear-thinning pseudoplasticity, Ostwald-de Waele Power-Law model, Carreau-Yasuda model, zero-shear viscosity, and power-law index n.
01 · Why This Matters in Industry & GATE XE5
Applied directly across petrochemical refining, compounding plants, mold-flow simulations, and automotive part manufacturing (e.g., Reliance Industries, Supreme Petrochem, IOCL, CIPET testing protocols).
Molecular Mechanism: Master conformational physics, transition temperatures, and reaction kinetics.
Process & Quality: Predict viscosity behavior, solve moulding defects, and apply ASTM/ISO testing standards.
Non-Newtonian Rheology: Power-Law & Carreau-Yasuda Models for Polymer Melts
1. Why This Topic Matters
Polymer melts are non-Newtonian — their viscosity drops dramatically with shear rate (shear-thinning). This behaviour controls how melts flow through extruder dies, injection mould runners, and film blowing dies. Process engineers at Supreme Industries, Reliance Industries (RIL), and Berry Global use power-law and Carreau models to simulate melt flow in Moldflow, Moldex3D, and Ansys Polyflow. Selecting the wrong viscosity model leads to short shots, burn marks, excessive pressure drops, and warpage.
2. Learning Objectives
- Explain shear-thinning behaviour and its molecular origin in entangled polymer chains.
- Apply the Power-Law (Ostwald–de Waele) model to calculate apparent viscosity and pressure drop.
- Use the Carreau-Yasuda model and identify its parameters (η₀, λ, n, a).
- Calculate the Power-Law flow consistency index K and flow index n from capillary rheometer data.
- Identify ISO 11443 (capillary rheometry) as the primary standard for polymer melt viscosity.
3. Core Theory
3.1 Shear-Thinning — The Molecular Origin
At rest, entangled polymer chains form a random coil network with high viscosity. Under shear:
- Chains align in the flow direction (disentanglement).
- Coil dimensions collapse (reduced drag)
- Chain entanglement density drops — viscosity decreases.
This is shear-thinning (pseudoplastic) behaviour — the dominant rheological characteristic of all high-MW thermoplastic melts.
3.2 Power-Law (Ostwald–de Waele) Model
The simplest non-Newtonian viscosity model:
Or equivalently:
| Parameter | Symbol | Units | Physical Meaning |
|---|---|---|---|
| Flow consistency index | K | Pa·sⁿ | Viscosity at unit shear rate |
| Power-law flow index | n | dimensionless | n<1: shear-thinning; n=1: Newtonian; n>1: shear-thickening |
| Apparent viscosity | η | Pa·s | Shear-rate dependent viscosity |
For a typical HDPE: K ≈ 18,000 Pa·sⁿ, n ≈ 0.38 at 200°C For PP: K ≈ 8,000 Pa·sⁿ, n ≈ 0.35 at 230°C
Limitation of Power-Law: Predicts infinite viscosity at zero shear rate (unphysical). Cannot capture the Newtonian plateau at low shear rates.
3.3 Carreau-Yasuda Model
A more complete model capturing both Newtonian plateaus:
For polymers, η_∞ ≈ 0, so:
| Parameter | Physical Meaning | Typical Value (HDPE 200°C) |
|---|---|---|
| η₀ | Zero-shear viscosity (Newtonian plateau) | 50,000–200,000 Pa·s |
| λ | Relaxation time — onset of shear-thinning | 0.01–1 s |
| n | Power-law slope in shear-thinning region | 0.3–0.5 |
| a | Transition breadth (Yasuda parameter) | 0.5–2 |
3.4 Pressure Drop in a Tube (Power-Law Fluid)
For a power-law fluid in a cylindrical die (Hagen-Poiseuille modified):
Where: L = die length, R = die radius, Q = volumetric flow rate.
4. Worked Example
Non-Newtonian Rheology: Power-Law & Carreau-Yasuda Models for Polymer Melts — Industrial Process Flow Diagram (PFD)
ISO 10628 Unit Operations & Thermodynamic Control Sequence
Raw Material Feed & Metering
Drying to < 0.02% moisture and gravimetric dosing
Reaction & Polymer Melt Processing
Controlled thermal shear dissipation and phase transition
Shaping & Solidification
Die extrusion or mold cavity pressure packing
Quality Inspection & Testing
ASTM D638 / ISO 527 tensile & MFI compliance check
Problem Statement:
Problem: PP melt at 230°C has power-law parameters K = 8000 Pa·sⁿ, n = 0.35. A capillary die has L = 50 mm, R = 1.5 mm. Volumetric flow rate Q = 5 × 10⁻⁷ m³/s. Calculate the pressure drop.
Step 1: Apparent shear rate at die wall:
Step 2: Corrected (Rabinowitsch) shear rate:
Step 3: Wall shear stress:
Step 4: Pressure drop:
5. Indian Industry Context
Non-Newtonian Rheology: Power-Law & Carreau-Yasuda Models for Polymer Melts — CAD Tooling & Machine Geometry Blueprint
Critical Geometric Dimensions & Tolerances (GD&T)
- Primary Processing Tolerance:± 0.02 mm (ISO 20457 Class M1)
- Thermal Expansion Allowance:1.5% (Volumetric Shrinkage)
- Draft Angle Minimum:1.0° - 1.5° (Core/Cavity Ejection)
Tooling Fabrication Notes
- • Fabricated according to ISO 20457 plastic molding tolerance standards.
- • EDM finish SPI C-1 applied across cavity optical contact faces.
- • Conformal cooling lines pressure tested at 12 bar water flow.
Supreme Industries (Mumbai) runs twin-screw compounding lines at 350–450 kg/h throughput. Their process engineers use Power-Law models to estimate screw pressure profiles and motor torque requirements for 30% talc-filled PP compounds — ensuring the gearbox is not overloaded at production line speeds.
Reliance Industries Jamnagar uses Carreau-Yasuda viscosity models in their proprietary die design software for HDPE blown film dies — the low-shear Newtonian plateau (η₀) is critical for predicting bubble stability at the frost line.
6. Key Takeaways & Glossary
- Shear-thinning (pseudoplastic): Viscosity decreases with increasing shear rate — universal for high-MW polymers.
- Power-law index n: n < 1 = shear-thinning; n = 1 = Newtonian; n > 1 = shear-thickening (dilatant).
- K (consistency index): Viscosity magnitude at unit shear rate — higher K = more viscous melt.
- η₀ (zero-shear viscosity): Newtonian plateau — sensitive to molecular weight (η₀ ∝ MW³·⁴).
- Rabinowitsch correction: Converts apparent capillary shear rate to true wall shear rate for non-Newtonian fluids.
- ISO 11443: Standard for capillary rheometry of polymer melts.
7. Standards Reference
- ISO 11443:2021 — Determination of the fluidity of plastics using capillary and slit-die rheometers
- ASTM D3835 — Determination of properties of polymeric materials by means of a capillary rheometer
- ISO 6721-10 — Complex shear viscosity using a parallel-plate oscillatory rheometer
- ASTM D4440 — Plastics — Determination of dynamic mechanical properties using oscillatory shear
8. GATE / University Practice Questions
- HDPE at 220°C: K = 15,000 Pa·sⁿ, n = 0.40. Calculate apparent viscosity at shear rate 500 s⁻¹.
- Explain why the Power-Law model is inadequate at very low shear rates for polymer melts.
- What does a higher power-law index n (closer to 1.0) indicate about the degree of shear-thinning?
Non-Newtonian Rheology: Power-Law & Carreau-Yasuda Models for Polymer Melts · Engineering Triad
Material Synthesis · Processing Hardware · Commercial Application
Standard Engineering Thermoplastic Resin
—[Monomer Backbone]ₙ— (Calibrated Molecular Weight & PDI)
Industrial Polymer Processing & Tooling System
Computer-Controlled Extrusion / Injection Moulding Hardware
Commercial Engineering Parts & Quality-Inspected Components
Automotive, Electrical, Medical & Packaging Applications
Test Your Conceptual Understanding
In polymer science and processing thermodynamics, which factor most directly controls the critical transition temperature?
- Always evaluate molecular weight distribution (MWD) alongside zero-shear viscosity when calculating mold shear rates.
- Differential Scanning Calorimetry (DSC) provides $T_g$, $T_c$, and $T_m$ to define optimal processing temperatures.
- Comply with ASTM D638 / ISO 527 tensile specimen sizing to prevent premature necking artifacts.
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