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Multiscale modeling of Liquid
Crystalline/Nanotube composites

          Sharil Patrale

            Guided by:
       Dr. Gregory Odegard
Outline

•   Introduction
•   Motivation
•   Application
•   Method
•   Accomplishments
•   Current work
•   Future work
Introduction
• Composite material is a material composed of
  two or more distinct phases.

• Types of composites
   – Metal matrix composites
   – Ceramic matrix composites
   – Polymer matrix composites
Polymer Matrix Composites
• Material consisting of a polymer matrix combined
  with a reinforcing phase of fibers.

• Exhibit high strength and stiffness

• Light in weight.

• Show directional strength properties

• Carbon fiber reinforced polymer composites.
Liquid crystalline polymer
• Obtained by dissolving a polymer in solvent or
  heating to its melting point

• High mechanical strength
  at high temperatures
   – High strength to weight ratio
     when combined with
     nanotubes
                                     Material : Liquid Crystal
                                     Polymer LCP 304T40
• Used for electrical
  and mechanical parts
Why Carbon Nanotubes?
• Very high strength-
  Stronger than the sp3
  bonds in Diamond

• High stiffness

• High thermal conductivity

• Extremely light weight-
  about 1/5th of the weight
  of steel
Motivation

• Ability of LC molecules (matrix) to be oriented in
  preferred direction using electric or magnetic
  fields

• Surface tension aligns the nanotubes

• Resulting mechanical and thermal properties
Applications
• Vehicle and aircraft components
  – Surfacing, engine components


• Sport goods
  – Racquets, Helmets, Bikes


• Electronic sensor components

• High temperature applications
The Research
• To develop the nano-composite forming
  process.

• To optimize the mechanical and thermal
  properties of the nano-composites.

→ To implement a mathematical modeling
  approach for efficiently predicting the
  composite’s mechanical properties.
Mechanical/elastic properties

•   E1 – longitudinal young’s modulus
•   E2 – transverse young’s modulus
•   v12 – longitudinal poisson’s ratio
•   v23 – transverse poisson’s ratio
•   G12 – longitudinal shear modulus
Micromechanics
• Analysis of a composite at the level of its individual
  constituent

• Can predict the multi-axial properties of anisotropic
  composites

• Typically based on continuum mechanics
   – Response of anisotropic materials


→ Focus on Mori-Tanaka modeling approach
Mori-Tanaka modeling approach
• Calculating the average internal stress in the
  material

• More efficient than any other method with
  anisotropic matrix

• Predicting elastic properties as a function of
   – Nanotube orientation
   – LC orientation
   – Nanotube volume fraction
   – Interfacial conditions
Eshelby’s Tensor

• Fourth order tensor, Sijkl (   ij   =   ji)



• Relates the average fiber strain to the average
  matrix strain.
      c=S        T
   ij     ijkl kl


• Depends on the properties of the matrix material
Numerical integration using Gaussian Quadrature:
Accomplishments
• Mathematical model to determine elastic
  properties of LaRC-SI/nanotube composite.

• Relationship between various moduli and fiber
  volume fractions at different aspect ratios.

• Model to calculate Eshelby’s tensor for
  anisotropic matrix

• Corresponding graphs are shown.
Moduli for various nanotube lengths
Aligned fibers
Randomly oriented fibers
Future work

• Searching for properties of LC polymer (RM-
  257)

• Using various fiber/matrix orientations and
  aspect ratios

• Optimizing the model
Thank you

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Modeling Liquid Crystal Polymer Nanotube Composites

  • 1. Multiscale modeling of Liquid Crystalline/Nanotube composites Sharil Patrale Guided by: Dr. Gregory Odegard
  • 2. Outline • Introduction • Motivation • Application • Method • Accomplishments • Current work • Future work
  • 3. Introduction • Composite material is a material composed of two or more distinct phases. • Types of composites – Metal matrix composites – Ceramic matrix composites – Polymer matrix composites
  • 4. Polymer Matrix Composites • Material consisting of a polymer matrix combined with a reinforcing phase of fibers. • Exhibit high strength and stiffness • Light in weight. • Show directional strength properties • Carbon fiber reinforced polymer composites.
  • 5. Liquid crystalline polymer • Obtained by dissolving a polymer in solvent or heating to its melting point • High mechanical strength at high temperatures – High strength to weight ratio when combined with nanotubes Material : Liquid Crystal Polymer LCP 304T40 • Used for electrical and mechanical parts
  • 6. Why Carbon Nanotubes? • Very high strength- Stronger than the sp3 bonds in Diamond • High stiffness • High thermal conductivity • Extremely light weight- about 1/5th of the weight of steel
  • 7. Motivation • Ability of LC molecules (matrix) to be oriented in preferred direction using electric or magnetic fields • Surface tension aligns the nanotubes • Resulting mechanical and thermal properties
  • 8. Applications • Vehicle and aircraft components – Surfacing, engine components • Sport goods – Racquets, Helmets, Bikes • Electronic sensor components • High temperature applications
  • 9. The Research • To develop the nano-composite forming process. • To optimize the mechanical and thermal properties of the nano-composites. → To implement a mathematical modeling approach for efficiently predicting the composite’s mechanical properties.
  • 10. Mechanical/elastic properties • E1 – longitudinal young’s modulus • E2 – transverse young’s modulus • v12 – longitudinal poisson’s ratio • v23 – transverse poisson’s ratio • G12 – longitudinal shear modulus
  • 11. Micromechanics • Analysis of a composite at the level of its individual constituent • Can predict the multi-axial properties of anisotropic composites • Typically based on continuum mechanics – Response of anisotropic materials → Focus on Mori-Tanaka modeling approach
  • 12. Mori-Tanaka modeling approach • Calculating the average internal stress in the material • More efficient than any other method with anisotropic matrix • Predicting elastic properties as a function of – Nanotube orientation – LC orientation – Nanotube volume fraction – Interfacial conditions
  • 13. Eshelby’s Tensor • Fourth order tensor, Sijkl ( ij = ji) • Relates the average fiber strain to the average matrix strain. c=S T ij ijkl kl • Depends on the properties of the matrix material
  • 14. Numerical integration using Gaussian Quadrature:
  • 15. Accomplishments • Mathematical model to determine elastic properties of LaRC-SI/nanotube composite. • Relationship between various moduli and fiber volume fractions at different aspect ratios. • Model to calculate Eshelby’s tensor for anisotropic matrix • Corresponding graphs are shown.
  • 16. Moduli for various nanotube lengths
  • 19. Future work • Searching for properties of LC polymer (RM- 257) • Using various fiber/matrix orientations and aspect ratios • Optimizing the model