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Complete User Guide148 pages · 10 chapters · Updated 2026-09-18
Getting Started Handbook139 pages · 8 chapters · Updated 2026-09-18
Training & Exercise Manual386 pages · 115 chapters · all 104 exercises · Updated 2026-09-18
Complete Theory Manual255 pages · 56 chapters · Updated 2026-09-18
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05.6.4 / Structural

Process fields in progressive laminate failure

Map temperature, moisture, cure shrinkage, and crystallization shrinkage into each ply, form their laminate resultants, and superimpose them with static or progressive mechanical loading. Expand any equation for its physical meaning, variables, units, model connection, and theory source.

Enabled local free strains

Eq. 05.6.4-01Flag-controlled local free strain
εfreek = λTαkΔTk + λMβkΔCk + λcεck + λxεxk
Equation detailsExplanation · variables · model connection · reference

Adds the unconstrained strain caused by temperature change, moisture change, thermoset chemical shrinkage, and thermoplastic crystallization shrinkage. Independent binary switches let each contribution enter or leave the structural solve without changing the process solution.

Variablesεfreektotal enabled free strain in local ply direction kstrainλT, λM, λc, λxthermal, moisture, cure, and crystallization inclusion flags0 or 1αklocal coefficient of thermal expansion1/Kβklocal coefficient of moisture expansionstrain per percentage pointΔTk, ΔCktemperature and moisture changes from each ply reference stateK, percentage pointsεck, εxkcure and crystallization shrinkage strainsstrain

Model connectionEvaluated at mapped bottom, middle, and top structural recovery points for every ply. These are the same free strains subtracted during stress recovery and failure evaluation.

Theory basisNASA hygrothermal laminate mechanics

Eq. 05.6.4-02Local-to-global free-strain transformation
εfreexy,k(z) = Tεk) εfree12,k(z)
Equation detailsExplanation · variables · model connection · reference

Rotates each local engineering free-strain vector from material axes 1–2 into laminate axes x–y using the ply orientation.

Variablesεfreexy,kglobal in-plane free-strain vector [εx, εy, γxy]ᵀstrainεfree12,klocal in-plane free-strain vector [ε1, ε2, γ12]ᵀstrainTεk)engineering-strain transformation matrixdimensionlessθkorientation of ply kdegrees or radians consistently

Model connectionThe transformed field is multiplied by the ply’s damaged transformed stiffness Q̄d when process force and moment resultants are integrated.

Theory basisClassical lamina transformation relations

Mapping the process mesh to three structural nodes per ply

The transport mesh may contain any user-selected number of cells per ply, whereas structural visualization and field output retain exactly three recovery nodes per ply. R15 least-squares fits each process field to a linear function within its owning physical ply, then evaluates that fit at the bottom, middle, and top coordinates.

Eq. 05.6.4-03Per-ply linear process-field fit
[ak, bk]T = (ZkTZk)−1ZkTfkk(z) = ak + bkz
Equation detailsExplanation · variables · model connection · reference

Finds the best constant and gradient for temperature, moisture, cure shrinkage, and crystallization shrinkage within one ply from all transport cells belonging to that ply.

Variablesfk,jprocess quantity at transport node j of ply kfield-dependentak, bkleast-squares intercept and through-thickness gradientfield unit, field unit/mZkdesign matrix with rows [1, zj]mixedzk,jtransport-node coordinatemk(z)linear field reconstructed at a structural coordinatefield-dependent

Model connectionPreserves both the ply-average process state and its first through-thickness gradient while keeping the stress/strain field histories and animation mesh fixed at three structural nodes per ply.

Theory basisReduced-order process-to-structure mapping

Damaged laminate stiffness and process resultants

Eq. 05.6.4-04Damaged ABD stiffness integrals
Ad = Σkzk−1zk dk dzBd = Σkzk−1zk zdk dz,   Dd = Σkzk−1zkdk dz
Equation detailsExplanation · variables · model connection · reference

Integrates the current transformed stiffness of every ply through the laminate thickness. Progressive failure changes Q̄d and therefore rebuilds A, B, and D.

VariablesAd, Bd, Dddamaged extensional, coupling, and bending stiffness matricesN/m, N, N·mdkdamaged transformed reduced stiffness of ply kPazk−1, zkbottom and top coordinates of ply km

Model connectionThe same damaged stiffness used for mechanical equilibrium also weights the process resultants, so a new ply failure changes load redistribution and residual-stress restraint at the same accepted load.

Theory basisNASA classical laminate ABD formulation

Eq. 05.6.4-05Process force and moment resultants
Np = Σkdk εfreek(z) dzMp = Σk ∫ z dk εfreek(z) dz
Equation detailsExplanation · variables · model connection · reference

Converts an otherwise free process strain into equivalent in-plane forces and moments representing the restraint imposed by the bonded laminate. A gradient contributes directly to process bending moment.

VariablesNp, Mpprocess-induced membrane force and bending moment resultantsN/m, Ndkcurrent damaged transformed ply stiffnessPaεfreek(z)enabled global free-strain field in ply kstrainzcoordinate measured from the laminate reference planem

Model connectionRecomputed after any new damage state before same-load re-equilibration. The process-resultant history reports each component over the structural increments.

Theory basisHygrothermal force and moment resultants

Combined generalized equilibrium

Eq. 05.6.4-06Damaged mechanical–process equilibrium
[Ad Bd; Bd Dd] {ε0, κ}T = {Nmech+Np, Mmech+Mp}T
Equation detailsExplanation · variables · model connection · reference

Solves simultaneously for mid-plane strains and curvatures under the sum of enabled mechanical and process-equivalent resultants. This is the governing superposition step, not a postprocessed stress offset.

Variablesε0laminate mid-plane strain vectorstrainκlaminate curvature/twist vector1/mNmech, Mmechapplied mechanical membrane and moment resultantsN/m, NNp, Mpenabled process force and moment resultantsN/m, NAd, Bd, Ddcurrent damaged laminate stiffness blocksN/m, N, N·m

Model connectionUsed for a static mechanical state or at every progressive load increment. The mechanical-load flag may remove Nmech and Mmech while retaining process-only residual response.

Theory basisNASA generalized laminate equilibrium

Eq. 05.6.4-07Through-thickness strain and stress recovery
ε(z) = ε0 + zκσk(z) = dk[ε(z) − εfreek(z)]
Equation detailsExplanation · variables · model connection · reference

Recovers the compatible global strain at any z and subtracts the enabled free strain before applying the current damaged stiffness. The result is the actual constrained ply stress used by failure criteria.

Variablesε(z)total compatible global in-plane strainstrainε0, κmid-plane strain and curvature from generalized equilibriumstrain, 1/mσk(z)global stress in ply kPadkdamaged transformed ply stiffnessPaεfreek(z)enabled global free strainstrain

Model connectionEvaluated at the bottom, middle, and top of every ply and then transformed to local 1–2 axes. Top and bottom surface states govern the progressive failure check.

Theory basisClassical laminate stress recovery with hygrothermal strain

Eq. 05.6.4-08Auditable contribution decomposition
ytot = ymech + yT + yM + yc + yx
Equation detailsExplanation · variables · model connection · reference

Reports total fields together with separately evaluated mechanical, thermal, moisture, cure-shrinkage, and crystallization-shrinkage contributions at the same increment and damaged material state.

Variablesytotreported total stress or strain fieldPa or strainymechmechanical contributionPa or strainyT, yMthermal and moisture contributionsPa or strainyc, yxcure- and crystallization-shrinkage contributionsPa or strain

Model connectionSupports the global, local, principal, and process-only field histories so CDS can display each contribution without reconstructing it outside the solver.

Theory basisProcess-induced residual-response decomposition

Progressive same-load update

At each accepted increment the solver recovers all three structural nodes per ply; checks both surfaces; evaluates the independent criterion assigned to that ply; degrades only newly activated stiffness families; rebuilds damaged ABD and process resultants; and re-equilibrates at the same combined mechanical–process load until no new event occurs.

Coupling boundary. The process solver is one-way with respect to structural damage in r15: process fields create structural strains and stresses, while ply damage changes the stiffness that restrains those fields. Damage does not yet change k3, cp, diffusivity, cure kinetics, or crystallization kinetics.

Auditable outputs

  • Stress and strain histories: total, mechanical, thermal, and moisture contributions.
  • Transport histories: mesh, fields, state, rates, heat, shrinkage, and surface interpolation.
  • Structural process mapping: mapped states and active physical components.
  • Process-only fields: global and local stress and strain.
  • Process resultants: force and moment components at every structural increment.

Theory references

  1. Nettles, Basic Mechanics of Laminated Composite Plates, NASA RP-1351, including ABD and hygrothermal effects.
  2. NASA, Composite Cure Process Modeling and Simulations using Finite Element Analysis (2016).
  3. NASA/TM–20205009287, cure-induced residual stress development.

Workbench availability: released models, inputs and compatible study paths. The wider theory library includes reference formulations not available in every Workbench solve.