Laminate Bending

Bending a laminate in 3-point or 4-point: where it fails, and why the span decides

1Material
Ply thickness

2Laminate
Layup
3Specimen and fixture
Loading

4Failure properties

IM7/8552 ply data. Everything else is calculated from these; an empty box uses the value in grey;

Strength

Fracture energy between plies (delamination)
5Equations and sourcesLaminate beam theory

The specimen is a narrow beam: only the bending moment Mx acts (My = Mxy = 0, no axial force). Laminate theory with the bending stiffness matrix D gives the curvature, the strain ε = ε0 + zκ through the thickness and the stress in every ply.

3-point (Procedure A): M = PL/4, V = P/2. 4-point (Procedure B, load span L/2): M = PL/8 between the noses, V = P/2 outside them.

Flexural stress (ASTM D7264): σ = 3PL/(2bh²) for 3-point, σ = 3PL/(4bh²) for 4-point.

Surface strain from the midspan deflection δ: ε = 6δh/L² for 3-point, ε = 4.36δh/L² for 4-point.

Deflection, bending plus shear: 3-point δ = PL³/(48EI) + PL/(4κGA); 4-point δ = 11PL³/(768EI) + PL/(8κGA); κ = 5/6, A = bh.

EI comes from the laminate (EI = b/d11, d = D−1). The fibers are stiffer in tension than in compression (E1 158.5 against 138.2 GPa for IM7/8552, NCAMP), so the plies on the compression side use the compression modulus and the neutral axis moves toward the tension side; each ply is split in 8 layers and the stiffness of each follows the sign of its fiber strain. The transverse shear modulus G is the through-thickness (series) average of the plies: G13 along the fibers, G23 across them.

Interlaminar shear from equilibrium: τxz(z) = −V ∫−h/2z σx/M dz (and τyz from σxy). A homogeneous beam gives the parabola with its peak 1.5V/(bh) = 0.75P/(bh).

Ply failure, from the shared failure engine used on every test page: fiber σ1/XT or −σ1/XC; matrix √[(σ2/Y)² + (τ12/S)²] with the in-situ strengths of the ply's block (Camanho et al. 2006) and Y = YC in compression; delamination √(τxz² + τyz²)/SILS.

Each ply's stress is the bending stress plus the cure residual stress of the laminate (cool-down from the stress-free temperature, the same as on the Tension page; none for an estimated material). The bending stress chart shows the bending part only. Ply properties also come from the shared engine.

Ultimate rule: the beam fails when any ply breaks its fibers (σ1 reaches XT or −XC), or a delamination runs, whichever load is lower. Only when no ply lies within 15° of 0° can matrix failure also end the test: of the ±45° plies (shear), or, without those, of any ply. This is the same rule as on the other test pages. Matrix cracks in other plies are drawn and marked on the curve but do not end the test. The beam is linear elastic up to failure; the load drop after it and the damage drawings are illustrative. Not modelled: contact stresses under the nose, large deflection, cure residual stresses, free-edge stresses.

Delamination, two mechanisms. On short spans the shear force is large compared with the moment, and the beam delaminates near mid-thickness by interlaminar shear, checked against the measured short-beam strength SILS. A delamination can also grow from matrix cracks in a block of off-axis plies, the mechanism of the tension and open-hole tests; for it every test page uses the same fitted form σd = √(Ex GIIc / (0.47 tblock)), with the constant 0.47 fitted to the ply-block tension tests of Wisnom, Khan and Hallett (2008) and tblock the thickest same-angle off-axis block. Here it is checked on the tension side of the beam: a run of off-axis plies with two or more angles delaminates once one of its plies has cracked and the laminate strain at the run's outer edge reaches σd/Ex. It is not checked on the compression side, where the matrix cracks are closed, nor for an estimated material, which has no GIIc. The fitted form comes from uniform tension; using it with the bending strain at the run is this page's assumption.

Material data
Sources
  • ASTM D7264/D7264M-21, flexural properties of polymer matrix composites. doi:10.1520/D7264_D7264M-21
  • ASTM D2344/D2344M-22, short-beam strength of polymer matrix composites. doi:10.1520/D2344_D2344M-22
  • NCAMP report NCP-RP-2009-028 Rev B, 8552 IM7 unidirectional prepreg qualification statistics (2019): ply properties, SBS (Table 4-12), SBS1 (Table 5-25), E1c (Table 4-7). Per-specimen data: NCAMP report CAM-RP-2009-015 Rev B.
  • NCAMP report NCP-RP-2010-008 Rev D, 8552 AS4 unidirectional prepreg qualification statistics: ply properties, SBS (Table 4-12), LSBS (Table 5-25), E1c (Table 4-7). Per-specimen data: NCAMP report CAM-RP-2010-002 Rev A.
  • M.R. Wisnom, B. Khan and S.R. Hallett, Size effects in unnotched tensile strength of unidirectional and quasi-isotropic carbon/epoxy composites, Compos. Struct. 84 (2008) 21.
  • J.M. Whitney, C.E. Browning and A. Mair, Analysis of the flexure test for laminated composite materials, ASTM STP 546 (1974) 30. doi:10.1520/STP34856S
Laminate bending

Top in compression, bottom in tension, shear in between

A bent laminate fails where its plies reach their limit first. The layup and the span decide whether that is the top, the bottom or a delamination in the middle.

Choose a material and layup on the left, then select Run test.