This notes sheet looks at composite structures & types as well as critical fibre length, volume fraction and loading.

Pure materials and alloys are good for standard applications, but often a very specific set of properties is required from a material. In this instance, a composite may be used or even designed in order to maximise the best properties of a number of materials combined.

A composite is a material that employs multiple different phases to attain better specific properties than either phase alone.

There has to be a noticeable boundary between the two phases, and one needs to be introduced to the other rather than the two phases forming simultaneously – a two-phase slow cooled metal alloy is not a composite, then.

Composites occur naturally as well as artificially. Good examples are bones and carbon fibre respectively.

Composite Structure

There are two main phases in a composite:

  • the continuous matrix phase is the weaker phase that transfers applied loads to the reinforcement. It also acts as protection for the reinforcement.
  • the dispersed reinforcement phase adds the desired property (strength, stiffness, hardness etc.) to the material by delaying crack dispersion.

The matrix could be a metal, ceramic or a polymer. The reinforcement is generally a ceramic (carbon is especially common), but could take a number of forms:

Particulate composite, particle composite, composites

Particulate reinforced composites use small particles, like spheres or flakes.

Fibre reinforced composites, carbon fibre structure, composite structure

Fibre reinforced composites contain fibres. These could be very short, fairly long, or even continuous throughout the structure.

Structural composites

Structural Composites may use particles, fibres, or even both for reinforcement, arranged in specific forms to maximise strength: honeycombs, layers and sheets are common.

Types of Composites

Metal Matrix Composites (MMCs)

  • A cermet is a ceramic-metal composite.
  • Typically used for cutting tools and dies.
  • Advantages include high elastic modulus, toughness, and ductility.
  • Disadvantages include the high density and expense.
  • Standard matrix materials include:
  • Aluminium & aluminium-lithium alloys
  • Magnesium
  • Copper
  • Titanium
  • Super-alloys.
  • Standard reinforcement materials include:
  • Graphite
  • Alumina (aluminium oxide)
  • Silicon carbide
  • Boron
  • Tungsten carbide

Ceramic Matrix Composites (CMCs)

  • Generally used for temperature and corrosion sensitive applications, like engine components and deep-sea mining, or extremely hard cutting tools.
  • Advantages include the excellent corrosion and temperature resistance.
  • Disadvantages are the extreme brittleness and expense.
  • Standard matrix materials include:
  • Silicon carbide
  • Silicon nitride
  • Aluminium oxide
  • Standard reinforcement materials include:
  • Carbon
  • Aluminium oxide

Polymer Matrix Composites (PMCs)

  • Generally used for lightweight structures, like aircraft, vehicles, sporting, and marine equipment.
  • Advantages include low density, easy processing, and specific properties
  • Disadvantages include poor temperature and chemical resistance.
  • Standard matrix materials include:
  • Nylon
  • Polypropylene (PP)
  • Epoxy
  • Phenolic
  • Polyester
  • Standard reinforcement materials include:
  • Glass
  • Carbon
  • Boron
  • Aramid (Kevlar)

Critical Fibre Length

The length of fibres makes a huge difference to the composite’s performance.

  • Too short, and the adhesive bond between the fibre and the matrix will break before the fibre itself breaks, so the fibre pulls out of the structure
  • Too long, and the adhesive bond between matrix and fibre transmits too much load, breaking the fibre.

As with most things, a fine balance is required between the two. This is known as the critical fibre length.

Critical fibre length, composite fibre length, how long should fibres be, carbon fibre lengths

For a uniform circular cross-section fibre of half-length x, the shear force at the fibre-matrix boundary, F_s, is given by:

F_s=\tau_B \pi Dx

The force required to break the fibre is given by:

F_f=\frac{\pi D^2}{4}\times\sigma_f

The critical half-length is when these two forces equal one another:

\tau_B \pi Dx_c=\frac{\pi D^2}{4}\times\sigma_f

x_c=\frac{D\sigma_f}{4\tau_B}

The critical length is therefore:

l_c=2x_c=\frac{D\sigma_f}{2\tau_B}

Standard fibre lengths are:

  • 0.2mm for a carbon fibre in an epoxy matrix
  • 0.5mm for a glass fibre in a polyester matrix
  • 1.8mm for a glass fibre in a polypropylene matrix

Fibre Volume Fraction

Fibre composites are generally described in terms of fibre volume fraction: this is (you guessed it) the proportion of the materials volume that is taken up by fibres not matrix.

V_f = \frac{V_{fibres}}{V_{fibres} + V_{matrix}}

For fully aligned fibres, the volume fraction could be up to around 65%. Generally, it is lower.

  • For uniform cross-sectional and continuous fibres, the area fraction is the same as the volume fraction.

Loading Fibre Composites

Isostrain

Isostrain, isostrain composites, parallel strain, composite stress parallel to fibres

When the fibres are parallel to the applied load, and the fibre-matrix adhesive bond does not break, the matrix and fibres experience the same strains:

\varepsilon = \varepsilon_f = \varepsilon_m

The total force is thus the sum of the forces in the fibres and matrix:

F = \sigma A = V_f \sigma_f A + (1-V_f) \sigma_m A

When both the fibres and the matrix are in the linear elastic region, Hooke’s Law applies to both:

\sigma = E_f \varepsilon

\sigma_m = E_m \varepsilon

Therefore:

\sigma = V_f E_f \varepsilon + (1-V_f)E_m \varepsilon

E_{composite} = V_f E_f + (1-V_f) E_m

Isostress

Isostress, perpendicular strain, stress perpendicular to fibres, composites stress strain

When the fibres are perpendicular to the applied stress, the stress in the fibres and matrix are the same:

\sigma = \sigma_f = \sigma_m

Therefore:

\frac{1}{E_{composite}} = \frac{V_f}{E_f} + \frac{1-V_f}{E_m}

Comparing Isostrain and Isostress

Comparing isostress and isostrain, parallel vs perpendicular fibres composites carbon fibres

Stress-Strain Behaviour

stress-strain graph composites

It is harder to predict the strength of a composite without empirical investigation, however we can predict the behaviour by assuming it will initially perform similar to the fibre, but deform uniformly once the matrix begins to undergo plastic deformation.

  • A composite is a material that employs multiple different phases to attain better specific properties than either phase alone.
  • There are two phases:
    • the continuous matrix phase is the weaker phase that transfers applied loads to the reinforcement. It also acts as protection for the reinforcement.
    • the dispersed reinforcement phase adds the desired property (strength, stiffness, hardness etc.) to the material by delaying crack dispersion.
  • Composites may be reinforced by fibres, particles or structures.
  • Critical fibre length
    • If the fibres are too short, the adhesive bonds break, so the fibres pull out of the structure.
    • If the fibres are too long, the adhesive bonds transmit too much force to the fibres, breaking them.