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Polymer Chains by the Numbers
Chain size, molar mass, solutions and melts for people who mould, join and clean plastic parts, worked through one polystyrene workshop
Use the physics of long chains to judge resin grades, regrind, solvent cements, cleaners and storage: molar mass averages, coil size, viscosity, phase separation and solvent attack.
Start readingAbout this book
Plastics are made of long chains, and almost everything a plastics engineer cares about follows from that. A resin’s melt flow, a moulding’s toughness, the strength of a solvent-cemented joint, the clouding of a cement in a cold store, the crazing of a part wiped with the wrong cleaner and the swelling of a container: each depends on how long the chains are, how they coil, and how they mix with other molecules. The physics that describes this is mature, much of it is surprisingly simple, and most of it is never taught to the people who mould, join and clean plastic parts.
This book teaches it for practical use. It starts with a chain as a random walk, which gives its size, and with the molar mass averages that describe a real resin, which is a mixture of chains of many lengths. It then follows the chains into solution, where the solvent swells them, their viscosity reveals their size, and above a certain concentration they overlap and entangle; into the melt, where viscosity rises steeply with chain length; and into mixtures, where they may separate, dissolve or survive depending on temperature and solvent. It ends with the measurements that tie all of this to a resin lot or a batch of cement.
It is for plastics engineers, moulders, product designers, quality and laboratory staff, and students who handle resins and solvents. It assumes algebra, logarithms and basic chemistry: molar mass, density and the idea of a solvent. Each chapter works the running case with real numbers, includes one plausible mistake and how it was found, and ends with an exercise and its worked answer.
The running case
Every chapter follows one fictional workshop. This is an illustration. The workshop moulds general-purpose polystyrene housings for small instruments, regrinds its sprues and rejects, and joins its housings with a solvent cement it makes itself by dissolving clean regrind.
- Virgin resin: a general-purpose polystyrene whose current lot has a number-average molar mass of 100,800 g/mol, a weight-average of 249,900 g/mol and a z-average of 419,600 g/mol.
- Regrind: after two passes through the moulding machine its weight-average molar mass has fallen to about 215,000 g/mol.
- Feedstock check: intrinsic viscosity in toluene at 25 °C, with an internal specification of 0.78 to 0.92 dL/g.
- Solvent cement: 16% polystyrene by mass in a 50:50 by volume blend of ethyl acetate and d-limonene, which replaced an older toluene-based cement; target viscosity 1,000 to 1,500 mPa·s at 20 °C.
- Storage and cleaning: solvents kept in high-density polyethylene containers in a shed that reaches 5 °C in winter and 40 °C in summer; housings wiped with isopropanol before assembly.
The workshop, its resin, its measurements and every specification are invented. The polymer constants used, such as Mark–Houwink and solubility parameters, are teaching values of a realistic size, chosen so that the arithmetic can be followed; they must be replaced by measured or tabulated values for real work. None of this describes KEVOS® work or a real business.
How to use the book
Read Chapters 1 to 3 in order: they describe a single chain, a real resin’s mix of chains, and the effect of the solvent on coil size. Chapters 4 to 6 deal with viscosity in dilute solution, in concentrated solution and in the melt. Chapters 7 to 9 deal with mixing: phase separation, solvent selection and the melting of crystals in a solvent. Chapter 10 brings the measurements together into a check that a workshop can actually run.
KEVOS® tools are linked where they perform a step of the method, with a note of exactly what each one calculates.
Source limits and professional responsibility
The models in this book, the random walk, Flory–Huggins theory, the Mark–Houwink relation, the Hansen sphere and Flory’s melting-point equation, are standard and useful but approximate, and each chapter states its limits. Teaching values of constants are labelled as such. Real resins vary from lot to lot, and real decisions need measured data, the resin supplier’s information and the relevant test standards.
Many of the solvents discussed are flammable, and some are harmful to breathe or to skin. Their storage, handling and use are governed by Australian work health and safety law, Safe Work Australia’s code of practice for hazardous chemicals, the safety data sheet for each product and, for flammable liquids, the applicable storage requirements. This book teaches the physics of chains in solvents and melts. It is educational and is not a formulation, a safety assessment or advice for any process.
Who this book is for
Plastics engineers, moulders, product designers, quality and laboratory staff, and technical students who handle resins, regrind, solvent cements and cleaners and want to understand why polymer chains behave as they do.
What you will learn
- Estimate the size of a polymer coil from its molar mass and explain why chains are coils, not rods.
- Calculate number-, weight- and z-average molar masses and blend regrind with virgin resin to a target.
- Measure intrinsic viscosity and use it to check a resin grade or detect degradation.
- Predict how solution and melt viscosity change with concentration and molar mass, and where the scaling laws change.
- Screen solvents and cleaners for a plastic with solubility parameters, and check a solution or container against phase separation and melting.
- Build an incoming-resin and cement check that catches problems before they reach production.
Inside this book
Chapters
- 01A chain is a random walkCount the units and bonds in a polymer chain, estimate its coil size from a random walk with a characteristic ratio, and see why chains are coils a twentieth of their stretched length.
- 02Molar mass averages, dispersity and regrind blendsCalculate number-, weight- and z-average molar masses from a distribution, see which properties follow which average, and blend regrind with virgin resin to a target without averaging the wrong way.
- 03Good solvents, theta solvents and the Flory exponentSee why a chain swells in a good solvent and stays ideal in a theta solvent, estimate coil size with the self-avoiding-walk exponent 0.588, and judge solvent quality from what the chains do.
- 04Intrinsic viscosity and resin checksMeasure a resin's intrinsic viscosity from viscometer flow times, convert it to a viscosity-average molar mass with Mark–Houwink constants, and use it to check virgin resin, regrind and blends.
- 05Overlap, entanglement and the viscosity of a cementFind the overlap concentration where coils fill a solution, see why a cement's viscosity rises with about the fourth power of concentration, and set a cement's strength by fitting its own data.
- 06Melt viscosity, entanglement and the 3.4 powerSee why melt viscosity rises in proportion to chain length for short chains and with its 3.4 power above the entanglement threshold, and use that law to read melt flow rates, regrind and lot changes.
- 07Mixing and demixing: Flory–Huggins and the cold cementUse Flory–Huggins theory to see why long chains leave a marginal solvent, estimate χ from solubility parameters, find cloud, spinodal and critical temperatures, and check a cement for cold storage.
- 08Choosing solvents and cleaners with Hansen parametersScreen liquids against a plastic with Hansen solubility parameters, blend two liquids to reach or avoid a polymer, pick a cement solvent and a safe cleaner, and know what the sphere cannot predict.
- 09Crystals, diluents and melting-point depressionUse Flory's equation to find how far a solvent or plasticiser lowers the melting point of a semicrystalline polymer, judge solvent containers and hot dissolution, and see why crystals resist solvents.
- 10Measuring chains and building an incoming checkSize dissolved coils by dynamic light scattering, compare the methods that measure chains, and combine them into a practical check of resin lots, regrind, cement batches, cleaners and containers.
Apply This in Practice
Use these KEVOS® tools to try the method from this reading with your own numbers.
Applies this method
Linear Calibration Check (Straight-Line Fit, Calibrated Value, Calibration Interval)
Fits a least-squares line with standard errors; with logarithms of concentration and viscosity entered it gives the cement power-law exponent and the concentration for a target viscosity.
Applies this method
Mixture Cost and Blending (Alligation)
Gives the mass-weighted average of a mixture and the two-ingredient share for a target; used for the weight-average molar mass of regrind blends, which mixes linearly (Mn does not).
Applies this method
Particle and Polymer Coil Size from Dynamic Light Scattering (Decay Rate, Diffusion Coefficient, Stokes–Einstein)
Reduces a light-scattering decay rate to a diffusion coefficient and hydrodynamic size by Stokes–Einstein, with a qRh check; used to size dissolved polystyrene coils.
Applies this method
Polymer Intrinsic Viscosity and Molar Mass from One Viscometer Reading (Single-Point [η], Mark–Houwink)
Gives intrinsic viscosity from viscometer flow times by three single-point relations and a viscosity-average molar mass from Mark–Houwink constants, against specification limits.
Applies this method
Polymer Melting or Dissolution Temperature with a Diluent (Flory Melting-Point Depression)
Applies Flory's equation to give the melting or dissolution temperature of a semicrystalline polymer with a diluent and the margin to a service or process temperature.
Applies this method
Polymer Solution and Blend Phase Check (Flory–Huggins χ, Spinodal, Critical Point, Cloud Temperature)
Applies Flory–Huggins theory to give χ, the binodal, spinodal and critical values, the cloud temperature and the margin above it; used to check the cement for cold storage.
Used in Mixing and demixing: Flory–Huggins and the cold cement
Applies this method
Solvent Attack and Swelling Screen for Plastics and Elastomers (Hansen Distance Ra and RED)
Gives the Hansen distance and RED of a liquid or a two-liquid blend against a polymer, with a resist or dissolve verdict; used to choose cement solvents and safe cleaners.
Used in Choosing solvents and cleaners with Hansen parameters
References and source notes
The manuscript and worked examples are original KEVOS® writing. References inform particular concepts; their authors do not endorse this book. Web references were consulted on 31 October 2026.
- J. Cardy, Cambridge University Press, Cambridge (Cambridge Lecture Notes in Physics 5, ISBN 0 521 49959 3). Scaling and Renormalization in Statistical Physics (1996). Supplied source, in copyright. Read only as a subject map of random walks, the self-avoiding walk and polymer statistics, mean-field theory and critical points. No text, equations, figures, examples or exercises are reproduced or adapted; the engineering treatment, running case, numbers and checks in this book are original.
- N. Clisby, Physical Review Letters, vol. 104, 055702. Accurate estimate of the critical exponent ν for self-avoiding walks via a fast implementation of the pivot algorithm (2010). Source of the value ν = 0.587597(7) for three-dimensional self-avoiding walks used in Chapter 3, checked against the paper's abstract (arXiv:1002.0494).
- P. J. Flory, Cornell University Press, Ithaca. Principles of Polymer Chemistry (1953). Named as the origin of the Flory–Huggins mixing theory, Flory's estimate of the coil-size exponent and his equation for melting-point depression, used in Chapters 3, 7 and 9. Described, not quoted.
- P.-G. de Gennes, Cornell University Press, Ithaca. Scaling Concepts in Polymer Physics (1979). Named as the origin of the overlap concentration and the scaling description of semidilute solutions discussed in Chapter 5. Described, not quoted.
- G. C. Berry and T. G. Fox, Advances in Polymer Science, vol. 5, pp. 261–357. The viscosity of polymers and their concentrated solutions (1968). Named as a classic review of the dependence of melt and concentrated-solution viscosity on molar mass, including the change from a first-power to a 3.4-power law, discussed in Chapters 5 and 6.
- C. M. Hansen, CRC Press, Boca Raton. Hansen Solubility Parameters: A User's Handbook, 2nd edition (2007). Named as the reference for the three-parameter solubility method of Chapter 8 and as the place to find measured parameters. The parameter values in this book are teaching values and must be replaced by measured or tabulated ones for real work.
- V. J. Klenin, Elsevier, Amsterdam. Thermodynamics of Systems Containing Flexible-Chain Polymers (1999). Named as the source behind the KEVOS® polymer tools linked in Chapters 4, 7, 8, 9 and 10. Not quoted.
- National Institute of Standards and Technology. Thermophysical Properties of Fluid Systems, NIST Chemistry WebBook, SRD 69 (2026). Source of the viscosity of toluene at 25 °C, 0.5522 mPa·s, used for the light-scattering calculation in Chapter 10.
- National Institute of Standards and Technology, Physical Measurement Laboratory. Boltzmann constant, CODATA recommended value (2026). Source of the exact value k = 1.380 649 × 10⁻²³ J/K used in the Stokes–Einstein equation in Chapter 10.
- International Organization for Standardization. ISO 1628-1, ISO 1133-1, ISO 16014 and ISO 22412 (Current editions). Named by number and scope only: dilute-solution viscosity of polymers, melt mass-flow rate of thermoplastics, size-exclusion chromatography of polymers and dynamic light scattering. No values or procedures are quoted; laboratories should follow the editions they are accredited to.
- Safe Work Australia. Model Code of Practice: Managing risks of hazardous chemicals in the workplace (2021). Cited for the duty to manage the risks of the flammable and harmful solvents discussed in the running case. The book does not cover chemical safety; this code, safety data sheets and competent people do.