A novel computational technique is presented for embedding mass-loss due to burning into the ANSYS finite element modelling code. The approaches employ a range of computational modelling methods in order to provide more complete theoretical treatment of thermoelasticity absent from the literature for over six decades. Techniques are employed to evaluate structural integrity (namely, elastic moduli, Poisson’s ratios, and compressive brittle strength) of honeycomb systems known to approximate three-dimensional cellular chars. That is, reducing the mass of diagonal ribs and both diagonal-plus-vertical ribs simultaneously show rapid decreases in the structural integrity of both conventional and reentrant (auxetic, i.e., possessing a negative Poisson’s ratio) honeycombs. On the other hand, reducing only the vertical ribs shows initially modest reductions in such properties, followed by catastrophic failure of the material system. Calculations of thermal stress distributions indicate that in all cases the total stress is reduced in reentrant (auxetic) cellular solids. This indicates that conventional cellular solids are expected to fail before their auxetic counterparts. Furthermore, both analytical and FE modelling predictions of the brittle crush strength of both auxteic and conventional cellular solids show a relationship with structural stiffness. 1. Introduction Composite materials consist of two chemically distinct component materials mechanically bonded such that the overall amalgamate has more superior properties (in some sense) than the individual constituents. For example fibre-reinforced polymeric composites have a high strength and stiff fibrous (or particulate) reinforcement phase embedded within a matrix resin [1]. The matrix resin provides a uniform load distribution and environmental protection to the embedded material, resulting in a lightweight heterogeneous material. One major drawback is the relative ease with which organic materials support combustion and produce large amounts of smoke during burning. An example where enhanced thermal effects may be beneficial is in the fire retardant (FR) materials field. Here, improved mechanical resilience, reduced oxygen permeability, and reduced tendency to oxidation of very fragile or brittle charred structures formed under heat or fire conditions are desirable. Research has developed a barrier fabric containing cellulosic fibres dispersed with an intumescent [2]. Under heating conditions intumescent compounds (including phenolic, epoxy, and polyester) are known to form foamed chars which insulates
References
[1]
R. F. Gibson, Principles of Composite Material Mechanics, McGraw-Hill, 1994.
[2]
B. K. Kandola and A. R. Horrocks, “Complex char formation in flame-retarded fiber/intumescent combinations: physical and chemical nature of char,” Textile Research Journal, vol. 69, no. 5, pp. 374–381, 1999.
[3]
M. C. Yew and N. H. Ramli Sulong, “Fire-resistive performance of intumescent flame-retardant coatings for steel,” Materials and Design, vol. 34, pp. 719–724, 2012.
[4]
B. John, D. Mathew, B. Deependra, G. Joseph, C. P. R. Nair, and K. N. Ninan, “Medium-density ablative composites: processing, characterisation and thermal response under moderate atmospheric re-entry heating conditions,” Journal of Materials Science, vol. 46, no. 15, pp. 5017–5028, 2011.
[5]
S. Shawe, F. Buchanan, E. Harkin-Jones, and D. Farrar, “A study on the rate of degradation of the bioabsorbable polymer polyglycolic acid (PGA),” Journal of Materials Science, vol. 41, no. 15, pp. 4832–4838, 2006.
[6]
N. C. Chong, S. Nannaij, and P. S. Nam, “Negative thermal expansion ceramics,” Materials Science and Engineering, vol. 65, 1987.
[7]
J. P. M. Whitty, The thermo-mechanical properties of auxetic materials [Ph.D. thesis], Bolton Institute of Highe Education, Department of Mathematics, 2005.
[8]
S. P. Timoshenko, The Theory of Elasticity, Pergamon Press, New York, NY, USA, 2nd edition, 1954.
[9]
J. C. Anderson, R. D. Leaver, R. D. Rawlings, and J. M. Alexander, Material Science, Chapman & Hall, New York, NY, USA, 4th edition, 1989.
[10]
L. J. Gibson, M. F. Ashby, G. S. Schajer, and C. I. Roberson, “The mechanics of two-dimensional cellular solids,” Proceedings of the Royal Society A, vol. 382, pp. 25–42, 1982.
[11]
R. Lakes, “Negative Poisson's ratio materials,” Science, vol. 238, no. 4826, p. 551, 1987.
[12]
K. E. Evans, M. A. Nkansah, I. J. Hutchinson, and S. C. Rogers, “Molecular network design,” Nature, vol. 353, no. 6340, p. 124, 1991.
[13]
L. J. Gibson and M. F. Ashby, Cellular Solids: Structures and Properties, Cambridge University Press, Cambridge, Mass, USA, 2nd edition, 1997.
[14]
C. Brischke, C. R. Welzbacher, and T. Huckfeldt, “Influence of fungal decay by different basidiomycetes on the structural integrity of Norway spruce wood,” European Journal of Wood and Wood Products, vol. 66, pp. 433–438, 1991.
[15]
H. S. Allen and R. S. Maxwell, A Text-Book of Heat, Macmillan, New York, NY, USA, 1939.
[16]
S. P. Timoshenko, Strength of Materials Part 1, Elementary Theory and Problems, Van Nostrand, 3rd edition, 1955.
[17]
J. P. M. Whitty, F. Nazare, and A. Alderson, “Modelling the effects of density variations on the in-plane Poisson's ratios and Young's moduli of periodic conventional and re-entrant honeycombs—part 1: rib thickness variations,” Cellular Polymers, vol. 21, no. 2, pp. 69–98, 2002.
[18]
I. G. Masters and K. E. Evans, “Models for the elastic deformation of honeycombs,” Composite Structures, vol. 35, no. 4, pp. 403–422, 1996.
[19]
D. W. Overaker, A. M. Cuiti?o, and N. A. Langrana, “Elastoplastic micromechanical modeling of two-dimensional irregular convex and nonconvex (re-entrant) hexagonal foams,” Journal of Applied Mechanics, Transactions ASME, vol. 65, no. 3, pp. 748–757, 1998.
[20]
M. J. Silva and L. J. Gibson, “The effects of non-periodic microstructure and defects on the compressive strength of two-dimensional cellular solids,” International Journal of Mechanical Sciences, vol. 39, no. 5, pp. 549–563, 1997.
[21]
A. E. Simone and L. J. Gibson, “The effects of cell face curvature and corrugations on the stiffness and strength of metallic foams,” Acta Materialia, vol. 46, no. 11, pp. 3929–3935, 1998.
[22]
E. J. Staggs, Mathematical Modelling in Fire Retardant Textiles, Woodhead Publishing, Cambridge, Mass, USA, 2001.
[23]
S. Zhang, T. R. Hull, A. R. Horrocks et al., “Thermal degradation analysis and XRD characterisation of fibre-forming synthetic polypropylene containing nanoclay,” Polymer Degradation and Stability, vol. 92, no. 4, pp. 727–732, 2007.
[24]
G. Dimitriardus, Investigation of non-linear aeroelastic systems [Ph.D. thesis], University of Manchester, Department of Aerospace Engineering, July 1998.
[25]
J. P. M. Whitty, B. Henderson, P. Myler, and C. Chirwa, “Crash performance of cellular foams with reduced relative density part 2: rib deletion,” International Journal of Crashworthiness, vol. 12, no. 6, pp. 689–698, 2007.
[26]
K. E. Evans, A. Alderson, and F. R. Christian, “Auxetic two-dimensional polymer networks. An example of tailoring geometry for specific mechanical properties,” Journal of the Chemical Society, Faraday Transactions, vol. 91, no. 16, pp. 2671–2680, 1995.
[27]
G. Allaire and R. Brizzi, “A multiscale finite element method for numerical homogenization,” Multiscale Modeling & Simulation, vol. 4, no. 3, pp. 790–812, 2005.
[28]
ANSYS Inc. Ansys v13. Workbench 2.0 framework, 2012.
[29]
US Dept of Defence (DOD), I-Deas Masters Series 6, Structural Dynamics and Research Group, 1995.
[30]
A. Alderson, J. Rasburn, S. Ameer-Beg, P. G. Mullarkey, W. Perrie, and K. E. Evans, “An auxetic filter: A tuneable filter displaying enhanced size selectivity or defouling properties,” Industrial and Engineering Chemistry Research, vol. 39, no. 3, pp. 654–665, 2000.
[31]
H. S. Carslaw and J. C. Jaeger, Conduction of Heat in Solids, Oxford Science Publications, 1995.