Abstract
In this chapter we consider the results of incorporating a reinforcement (fibers, whiskers, particles, etc.) in a matrix to make a composite. It is of great importance to be able to predict the properties of a composite, given the properties of the components and the geometric arrangement of the components in the composite. We examine various micromechanical aspects of composites. A particularly simple case is the rule-of-mixtures, a rough tool that considers the composite properties as volume-weighted averages of the component properties. It is important to realize that the rule-of-mixtures works in only certain simple situations. Composite density is an example where the rule-of-mixtures is applied readily. In the case of mechanical properties, there are certain restrictions to its applicability. When more precise information is desired, it is better to use more sophisticated approaches based on the theory of elasticity.
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References
Arsenault RJ, Fisher RM (1983) Scripta Met 17:67
Behrens E (1968) J Composite Mater 2:2
Bhatt H, Donaldson KY, Hasselman DPH, Bhatt RT (1992) J Mater Sci 27:6653
Chamis CC (1983) NASA Tech. Memo. 83320, presented at the 38th annual conference of the Society of Plastics Industry (SPI), Houston, TX
Chamis CC, Sendecky GP (1968) J Compos Mater 2:332
Chawla KK (1973a) Metallography 6:155
Chawla KK (1973b) Philos Mag 28:401
Chawla KK (1974) In: Grain boundaries in engineering materials. Claitor’s Publishing Division, Baton Rouge, LA, p 435
Chawla KK (1976a) J Mater Sci 11:1567
Chawla KK (1976b) In: Proceedings of the international conference on composite materials/1975, TMS-AIME, New York. p 535
Chawla KK, Metzger M (1972) J Mater Sci 7:34
Clingerman ML, King JA, Schulz KH, Meyers JD (2002) J Appl Polym Sci 83:1341
Cox HL (1952) Brit J Appl Phys 3:122
Day RJ, Robinson IM, Zakikhani M, Young RJ (1987) Polymer 28:1833
Day RJ, Piddock V, Taylor R, Young RJ, Zakikhani M (1989) J Mater Sci 24:2898
Dow NF (1963) General Electric Report No. R63-SD-61
Eshelby JD (1957) Proc R Soc A241:376
Eshelby JD (1959) Proc R Soc A252:561
Fukuda H, Chou TW (1981) J Compos Mater 15:79
Galiotis C, Robinson IM, Young RJ, Smith BJE, Batchelder DN (1985) Polym Commun 26:354
Gladysz GM, Chawla KK (2001) Composites A 32:173
Hale DK (1976) J Mater Sci 11:2105
Halpin JC, Kardos JL (1976) Polym Eng Sci 16:344
Halpin JC, Tsai SW (1967) Environmental factors estimation in composite materials design. AFML TR 67-423
Hashin Z, Rosen BW (1964) J Appl Mech 31:233
Hasselman DPH, Johnson LF (1987) J Compos Mater 27:508
Hill R (1964) J Mech Phys Solids 12:199
Hill R (1965) J Mech Phys Solids 13:189
Kardos JL (1971) CRC Crit Rev Solid State Sci 3:419
Kelly A (1970) Chemical and mechanical behavior of inorganic materials. Wiley-Interscience, New York, p 523
Kelly A (1973a) Strong solids, 2nd edn. Clarendon, Oxford, p 157
Kerner EH (1956) Proc Phys Soc Lond B69:808
Lewis CA, Withers PJ (1995) Acta Metall Mater 43:3685
Love AEH (1952) A treatise on the mathematical theory of elasticity, 4th edn. Dover, New York, p 144
Marom GD, Weinberg A (1975) J Mater Sci 10:1005
Mori T, Tanaka K (1973) Acta Metall 21:571
Nardone VC, Prewo KM (1986) Scripta Met 20:43
Nielsen LE (1974) Mechanical properties of polymers and composites, vol 2. Marcel Dekker, New York
Nye JF (1985) Physical properties of crystals. Oxford University Press, London, p 131
Poritsky H (1934) Physics 5:406
Reuss A (1929) Z Angew Math Mech 9:49
Rosen BW (1973) Composites 4:16
Rosen BW, Hashin Z (1970) Int J Eng Sci 8:157
Schadler LS, Galiotis C (1995) Int Mater Rev 40:116
Schapery RA (1969) J Compos Mater 2:311
Schuster DM, Scala E (1964) Trans Met Soc-AIME 230:1635
Song M, He Y, Fang S (2010) J Mater Sci 45:4097
Termonia Y (1987) J Mater Sci 22:504
Timoshenko S, Goodier JN (1951) Theory of elasticity. McGraw-Hill, New York, p 416
Turner PS (1946) J Res Natl Bur Stand 37:239
Vaidya RU, Chawla KK (1994) Compos Sci Technol 50:13
Vaidya RU, Venkatesh R, Chawla KK (1994) Composites 25:308
Vogelsang M, Arsenault RJ, Fisher RM (1986) Metall Trans A 7A:379
Voigt W (1910) Lehrbuch der Kristallphysik. Teubner, Leipzig
Weber L (2005) Acta Mater 53:1945
Weber L, Dorn J, Mortensen A (2003a) Acta Mater 51:3199
Weber L, Fischer C, Mortensen A (2003b) Acta Mater 51:495
J.M. Whitney (1973). J. Struct. Div., 113.
Xu ZR, Chawla KK, Mitra R, Fine ME (1994) Scripta Met Mater 31:1525
Yang X, Hu X, Day RJ, Young RJ (1992) J Mater Sci 27:1409
Young RJ, Day RJ, Zakikhani M (1990) J Mater Sci 25:127
Young RJ (1994) In: Chawla KK, Liaw PK, Fishman SG (eds) High-performance composites: commonalty of phenomena. TMS, Warrendale, PA. p 263
Further Reading
Herakovich CT (1998) Mechanics of fibrous composites. Wiley, New York
Kelly A (1973b) Strong solids, 2nd edn. Clarendon, Oxford
Nemat-Nasser S, Hori M (1993) Micromechanics: overall properties of heterogenous materials. North-Holland, Amsterdam
Tewary VK (1978) Mechanics of fibre composites. Halsted, New York
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Problems
Problems
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10.1.
Describe some experimental methods of measuring void content in composites. Give the limitations of each method.
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10.2.
Consider a 40 % V f SiC whisker-reinforced aluminum composite. E f = 400 GPa, E m = 70 GPa, and (l/d) = 20. Compute the longitudinal elastic modulus of this composite if all the whiskers are aligned in the longitudinal direction. Use Halpin-Tsai-Kardos equations. Take ξ = 2(l/d).
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10.3.
A composite has 40 % V f of a 150 μm diameter fiber. The fiber strength is 2 GPa, the matrix strength is 75 MPa, while the fiber/matrix interfacial strength is 50 MPa. Assuming a linear build up of stress from the two ends of a fiber, estimate the composite strength for (a) 200 mm long fibers and (b) 3 mm long fibers.
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10.4.
Derive the load transfer expression Eq. (10.62) using the boundary conditions. Show that average tensile stress in the fiber is given by Eq. (10.63).
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10.5.
Consider a fiber reinforced composite system in which the fiber has an aspect ratio of 1,000. Estimate the minimum interfacial shear strength τ i, as a percentage of the tensile stress in fiber, σ f, which is necessary to avoid interface failure in the composite.
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10.6.
Show that as ξ → 0, the Halpin-Tsai equations reduce to
$$\begin{array}{ccccccc}l/p = {V_{{m}}}/{p_{{m}}} + {V_{{f}}}/{p_{{f}}}\\ {\hbox{while}}\;\,{\hbox{as}}\,\;\xi \to \infty, \;\,{\hbox{they}}\;\,{\hbox{reduce}}\;\,{\hbox{to}}\end{array} $$$$p = V_{{m}}{p_{{m}}} + {V_{{f}}}{p_{{f}}}. $$ -
10.7.
Consider an alumina fiber reinforced magnesium composite. Calculate the composite stress at the matrix yield strain. The matrix yield stress 180 MPa, E m = 70 GPa, and ν = 0.3. Take V f = 50 %.
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10.8.
Estimate the aspect ratio and the critical aspect ratio for aligned SiC whiskers (5 μm diameter and 2 mm long) in an aluminum alloy matrix. Assume that the matrix alloy does not show much work hardening.
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10.9.
Alumina whiskers (density = 3.8 g/cm3) are incorporated in a resin matrix (density = 1.3 g/cm3). What is the density of the composite? Take V f = 0.35. What is the relative mass of the whiskers?
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10.10.
Consider a composite made of aligned, continuous boron fibers in an aluminum matrix. Compute the elastic moduli, parallel, and transverse to the fibers. Take V f = 0.50.
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10.11.
Fractographic observations on a fiber composite showed that the average fiber pullout length was 0.5 mm. If V fu = 1 GPa and the fiber diameter is 100 μm, calculate the strength of the interface in shear.
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10.12.
Consider a tungsten/copper composite with following characteristics: fiber fracture strength = 3 GPa, fiber diameter = 200 μm, and the matrix shear yield strength = 80 MPa. Estimate the critical fiber length which will make it possible that the maximum load bearing capacity of the fiber is utilized.
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10.13.
Carbon fibers (V f = 50 %) and polyimide matrix have the following parameters:
$$ \begin{array}{ccccccc} {{E_{{f}}} = 280\,{\hbox{GPa}}} \hfill & {{E_{{m}}} = 276\,{\hbox{MPa}}} \hfill \\{{v_{{f}}} = 0.2} \hfill & {{v_{{m}}} = 0.3} \hfill \\\end{array} $$-
(a)
Compute the elastic modulus in the fiber direction, E 11, and transverse to the fiber direction, E 22.
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(b)
Compute the Poisson ratios, ν 12 and ν 21.
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(a)
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10.14.
Copper or aluminum wires with steel cores are used for electrical power transmission. Consider a Cu/steel composite wire having the following data:
inner diameter = 1 mm
outer diameter = 2 mm
$$ \begin{array}{ccccccc} {{E_{\rm{Cu}}} = 150\,\,{\hbox{GPa}}} \hfill & {{\alpha_{\rm{Cu}}} = 16 \times {{10}^{{ - 6}}}\,{{\hbox{K}}^{{ - 1}}}} \hfill \\{{E_{\rm{steel}}} = 210\,\,{\hbox{GPa}}} \hfill & {{\alpha_{\rm{steel}}} = 11 \times {{10}^{{ - 6}}}\,{{\hbox{K}}^{{ - 1}}}} \hfill \\{{\sigma_{{y{\rm{Cu}}}}} = 100\,\,{\hbox{MPa}}} \hfill & {{v_{\rm{Cu}}} = {v_{\rm{steel}}} = 0.3} \hfill \\{{\sigma_{\rm{ysteel}}} = 200\,\,{\hbox{MPa}}} \hfill & {} \hfill \\\end{array} $$-
(a)
The composite wire is loaded in tension. Which of the two components will yield plastically first? Why?
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(b)
Compute the tensile load that the wire will support before any plastic strain occurs.
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(c)
Compute the Young’s modulus and CTE of the composite wire.
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(a)
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10.15.
A composite is made of unidirectionally aligned carbon fibers in a glass-ceramic matrix. The following data are available:
$$ \begin{array}{ccccccc} {E_{{{\rm{f}}1}}} = 280\,\,{\hbox{GPa,}} & \,\,{E_{\rm{f2}}} = 40\,\,{\hbox{GPa,}}\,\,\,{E_{{m}}} = 70\,\,{\hbox{GPa}} \hfill \\{\nu_{{{\rm{f}}1}}} = 0.2\,\,\,\,\,\,{\nu_{{m}}} = 0.3 \hskip -70pt\hfill \\{G_{{{\rm{f}}12}}} = 18\,\,{\hbox{GPa}}\hskip -57pt \hfill \end{array}$$-
(a)
Compute the elastic modulus in the longitudinal and transverse directions.
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(b)
Compute the two Poisson’s ratios.
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(c)
Compute the principal shear modulus, G 12.
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(a)
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Chawla, K.K. (2012). Micromechanics of Composites. In: Composite Materials. Springer, New York, NY. https://doi.org/10.1007/978-0-387-74365-3_10
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DOI: https://doi.org/10.1007/978-0-387-74365-3_10
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