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Laminate generator

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Problem. The generator turns a ply lay-up into section stiffness. The shear integral, the beam formula and the equilibrium identities are tested on a homogeneous section, and the rolling shear in the cross plies on CLT.

Reference document. Classical lamination theory is taken from Jones, Mechanics of Composite Materials. The transverse shear stiffness is built from energy equivalence. For a homogeneous rectangle the shear factor must come out as five sixths.

In classical lamination theory the membrane, coupling and bending matrices are built by summing the contributions of the layers.

A=∑Qˉktk,B=∑Qˉktkzˉk,D=∑Qˉk(tkzˉk2+tk312)A = \sum \bar{Q}_k t_k,\qquad B = \sum \bar{Q}_k t_k \bar{z}_k,\qquad D = \sum \bar{Q}_k \left(t_k \bar{z}_k^2 + \dfrac{t_k^3}{12}\right)

The transverse shear stiffness of a layered section is computed from this relation. S(z)S(z) is the first moment of area above the level.

GA=(EI)2∫S(z)2G(z) dzGA = \dfrac{(EI)^2}{\displaystyle\int \dfrac{S(z)^2}{G(z)}\,dz}

The integral of the layer stresses through the thickness must equal the section forces and moments.

∫σxx dz=Nxx,∫σxx z dz=Mxx,∫τxz dz=Qx\int \sigma_{xx}\,dz = N_{xx},\qquad \int \sigma_{xx}\,z\,dz = M_{xx},\qquad \int \tau_{xz}\,dz = Q_x

Numerical model. There is no finite element model, and the compared quantities are read directly from the section matrices and ply stresses. The CLT lay-up is five 20 mm plies, 0/90/0/90/0.

Homogeneous section, layered shear integral

Parameters. t = 0.18 · layer = 3

Published source. The Timoshenko shear correction factor, rectangular section

κ=5/6\kappa = 5/6
QuantityReferenceComputedDeviation
Shear stiffness GAGA, per unit width576,923576,9230%

Note. A homogeneous section divided into three equal plies is used.

Five-layer CLT, along the longitudinal layer direction

Parameters. layup = 0/90/0/90/0 · layer thickness = 0.02

Published source. Classical lamination theory

D=∑Qˉk (tz2+t3/12)D = \sum \bar{Q}_k\,(t z^2 + t^3/12)
QuantityReferenceComputedDeviation
Bending stiffness D11D_{11}765.413765.4130%

Note. With the Poisson ratio taken as zero, Qˉ11=E\bar{Q}_{11} = E. The cross layers enter with the transverse modulus.

CLT strip section, mass consistency

Parameters. layup = 0/90/0/90/0

Closed form. Conservation of mass

∑ρktkb\sum \rho_k t_k b
QuantityReferenceComputedDeviation
Equivalent density times the transformed area0.420.420%

Homogeneous section, layer stress

Parameters. t = 0.2 · N = 250 · M = 30

Closed form. The beam formula

N/A+Mc/IN/A + Mc/I
QuantityReferenceComputedDeviation
Stress in the topmost fibre5,7505,7500%

Note. A homogeneous section divided into four equal layers is used.

Homogeneous section, transverse shear distribution

Parameters. t = 0.2 · Q = 40

Closed form. The maximum shear stress in a rectangular section

τmax=3V/2A\tau_{max} = 3V/2A
QuantityReferenceComputedDeviation
Shear stress at the mid-plane3003000%

Note. The value comes out exactly zero at the faces.

Equilibrium identities, CLT section

Parameters. layup = CLT

Closed form. An equilibrium equation independent of the constitutive relation

QuantityReferenceComputedDeviation
∫σ dz\int \sigma\,dz as a ratio of NxxN_{xx}1201200%

Equilibrium identities, homogeneous section

Parameters. layup = homogeneous

Closed form. An equilibrium equation independent of the constitutive relation

QuantityReferenceComputedDeviation
∫σ dz\int \sigma\,dz as a ratio of NxxN_{xx}1201200%

Five-layer CLT, continuity of the transverse shear

Parameters. Q = 30 · layup = 0/90/0/90/0

Closed form. Equilibrium requires the shear stress to be continuous across the interface

QuantityReferenceComputedDeviation
Jump at the layer interface01.137×10−131.137 \times 10^{-13}0%

Note. The peak rolling shear is 366.4 in the cross ply and 388.9 in the longitudinal ply, and it is zero at the faces.