An Introduction to Metal Matrix Composites (Cambridge Solid by T. W. Clyne

By T. W. Clyne

This e-book offers a entire, built-in insurance of steel matrix composites, together with the historical past to analytical-, experimental-, production-, and application-oriented elements. transparent pictorial descriptions are given of the elemental ideas governing quite a few homes and features. those surround mechanical, thermal, electric, environmental, and put on habit. assurance additionally extends to fabric processing and part fabrication facets and a survey of business utilization.

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An Introduction to Metal Matrix Composites (Cambridge Solid State Science Series)

This booklet supplies a complete, built-in insurance of steel matrix composites, together with the historical past to analytical-, experimental-, production-, and application-oriented facets. transparent pictorial descriptions are given of the elemental ideas governing numerous homes and features. those surround mechanical, thermal, electric, environmental, and put on habit.

Extra resources for An Introduction to Metal Matrix Composites (Cambridge Solid State Science Series)

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F. Nye (1985) Physical Properties of Crystals - Their Representation by Tensors and Matrices, Clarendon, Oxford. 4. T. W. Clyne (1990) A Compressibility-based Derivation of Simple Expressions for the Transverse Poissons Ratio and Shear Modulus of an Aligned Long Fibre Composite, J. Mat. Sci. , 9, pp. 336-9. 5. H. L. Cox (1952) The Elasticity and Strength of Paper and other Fibrous Materials, Brit. J. Appl. Phys. 3, pp. 73-9. 42 Basic composite mechanics 6. J. O. Out water (1956) The Mechanics of Plastics Reinforced in Tension, Modern Plastics, 33, pp.

F: \- \1 V L (a) £33= °- 2 5 £ 1°1 = 003 | •-* — - - (b) Fig. 4 A scaled diagram illustrating how the 5 tensor relates £T to sc for two inclusion shapes. In (a) a sphere and in (b) an aspect ratio 5 prolate ellipsoid (cigar shape) have undergone a 50% stress-free expansion in the '3'-direction. Note that in (b) the constrained axial strain is very small; this means that the compressive axial inclusion stress (CM(ec — £T)) will be much larger than for the sphere. The tensor S thus expresses the relationship between the final constrained inclusion shape and the natural shape mismatch (see Fig.

A. Levy and J. M. Papazian (1990) Tensile Properties of Short Fibre-Reinforced SiC/Al Composites, part II. , 21 A, pp. 411-20. References 43 28. O. C. Zienkiewicz and G. C. Huang (1989) Adaptive Modelling of Transient Coupled Metal Forming Processes, in Numerical Methods in Industrial Forming Processes (Proc. Numiform 89), E. G. ), A. A. Balkema, Rotterdam, pp. 3-10. 29. V. Tvergaard (1976) Effect of Thickness Inhomogeneities in Internally Pressurised Elasto-plastic Spherical Shells, J. Mech. Phys.

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