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05.1.3 / Materials

PEEK/PEKK crystallization pipeline

Represent calibrated semicrystalline thermoplastic evolution with single- or double-branch Nakamura/Avrami-style kinetics, latent heat, and anisotropic crystallization shrinkage. Expand any equation for its physical meaning, variables, units, model connection, and theory source.

State normalization and temperature window

Select thermoplastic crystallization for a semicrystalline polymer. Crystallinity X is bounded between its initial value and the user-supplied maximum Xmax. Kinetics are active only when the current nodal temperature lies strictly between the calibrated glass-transition and melting temperatures.

Eq. 05.1.3-01Normalized crystallinity
ξ = X/Xmax,   0 ≤ ξ ≤ 1
Equation detailsExplanation · variables · model connection · reference

Expresses current absolute crystallinity as a fraction of the maximum crystallinity available to the selected thermoplastic grade.

Variablesξnormalized crystallinitydimensionless, 0–1Xcurrent absolute crystallinitydimensionless mass or volume fractionXmaxcalibrated maximum crystallinitydimensionless mass or volume fraction

Model connectionThe normalized state is used by both Nakamura branches and the bounded integration rule; the crystallinity history retains the absolute crystallinity X.

Theory basisNakamura nonisothermal crystallization

Eq. 05.1.3-02Temperature and undercooling factor
Kj(T) = K0j exp[−Exj/(R T)] [(Tm−T)/(Tm−Tg)]p
Equation detailsExplanation · variables · model connection · reference

Combines Arrhenius temperature dependence with a calibrated undercooling function that vanishes at the melting temperature and is evaluated only inside the Tg–Tm process window.

VariablesKjcrystallization rate coefficient for branch js⁻¹K0jbranch pre-exponential coefficients⁻¹Exjbranch activation energyJ/molTg, Tmglass-transition and melting temperaturesKpundercooling exponentdimensionlessR, Tgas constant and local absolute temperatureJ/(mol·K), K

Model connectionEvaluated at every active thermoplastic transport node using the current thermal iterate. Outside Tg<T<Tm, R15 sets the crystallization rate to zero.

Theory basisPEEK dual-mechanism crystallization model

Nakamura/Avrami evolution

Eq. 05.1.3-03Single-branch normalized crystallization rate
ξ̇j = njKj(T)(1−ξ)[−ln(1−ξ)](nj−1)/nj
Equation detailsExplanation · variables · model connection · reference

Differentiates the Nakamura form of Avrami crystallization to obtain an instantaneous nonisothermal rate in the normalized state. Numerical floors protect the logarithm near ξ=0 and ξ=1.

Variablesξ̇jnormalized crystallization rate of branch js⁻¹njAvrami exponent for branch jdimensionlessKj(T)temperature-dependent branch coefficients⁻¹ξnormalized crystallinitydimensionless

Model connectionThe single-branch crystallization law uses its calibrated rate directly. The rate is then advanced using the irreversible bounded update.

Theory basisNakamura rate formulation

Eq. 05.1.3-04Double-branch crystallization rate
ξ̇ = w ξ̇1 + (1−w) ξ̇2
Equation detailsExplanation · variables · model connection · reference

Blends two independently calibrated Nakamura branches to represent two-stage crystallization with one bounded weighting factor.

Variablesξ̇combined normalized crystallization rates⁻¹ξ̇1, ξ̇2normalized rates of branches 1 and 2s⁻¹wbranch-1 weightdimensionless, 0–1

Model connectionThe dual-branch crystallization law. The same combined rate controls crystallinity growth, latent heat release, and the subsequent shrinkage state.

Theory basisVelisaris–Seferis dual-mechanism PEEK model

Eq. 05.1.3-05Bounded irreversible crystallinity update
rξ = 1−ξnξn+1 = min[1, max(ξn, ξn + rξ{1−exp(−ξ̇nΔt/rξ)})],   Xn+1 = Xmaxξn+1
Equation detailsExplanation · variables · model connection · reference

Integrates the normalized rate over the process step without consuming more than the remaining crystallizable fraction, then maps the state back to absolute crystallinity.

Variablesξn, ξn+1old and new normalized crystallinitydimensionlessrξremaining crystallizable fraction, 1−ξⁿdimensionlessξ̇nselected single- or double-branch rates⁻¹Δttransport time incrementsXn+1new absolute crystallinitydimensionless fraction

Model connectionApplied independently at every active thermoplastic node. The crystallization-rate history reports (Xⁿ⁺¹−Xⁿ)/Δt rather than the normalized branch rate.

Theory basisNonisothermal Nakamura state evolution

Latent heat and crystallization shrinkage

Eq. 05.1.3-06Crystallization heat source
qx = ρ Hx
Equation detailsExplanation · variables · model connection · reference

Converts absolute crystallinity growth and the calibrated heat of crystallization into a volumetric heat source.

Variablesqxvolumetric crystallization heat generationW/m³ρlocal effective ply densitykg/m³Hxheat of crystallization per unit massJ/kgabsolute crystallinity rates⁻¹

Model connectionIncluded in the heat equation only when the crystallization-exotherm option is enabled and reported as crystallization heat generation.

Theory basisPEEK crystallization calorimetry basis

Eq. 05.1.3-07Local crystallization-shrinkage free strain
εxk = −sxk(X−X0)/Xmax
Equation detailsExplanation · variables · model connection · reference

Maps crystallinity gained after the initial state into an anisotropic contraction in each ply material direction.

Variablesεxkcrystallization free strain in local direction kstrainsxkfull-crystallization shrinkage magnitudestrainX0initial absolute crystallinitydimensionless fractionXmaxmaximum absolute crystallinitydimensionless fractionklocal ply direction 1, 2, or 3index

Model connectionStored in the process-shrinkage history, fitted through each ply, and optionally added to the laminate process resultants and local failure-stress recovery.

Theory basisProcess-shrinkage residual-stress framework

Material-grade calibration is required. PEEK and PEKK grade, molecular architecture, cooling history, prior melt state, reinforcement, and measurement method change the fitted kinetics. The pipeline is a model family, not a generic property card.

Required evidence

  • DSC-derived crystallization rate and heat over relevant cooling/heating histories.
  • Tg, Tm, and maximum crystallinity for the selected grade.
  • Dilatometry or dimensional data for local crystallization shrinkage.
  • Verification against nonisothermal process cycles before residual-stress use.

Theory references

  1. Nakamura et al., “Some aspects of nonisothermal crystallization of polymers. I,” Journal of Applied Polymer Science 16 (1972) 1077–1091.
  2. Velisaris and Seferis, “Crystallization kinetics of polyetheretherketone (PEEK) matrices,” Polymer Engineering & Science 26 (1986) 1574–1581.
  3. NASA composite process modeling reference for coupled heat generation, shrinkage, and residual response.

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