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Straining composite

Stress—Strain Curves. The tensile stress-strain behavior of the blends in which PC is the continuous phase (blends with 5, 10, 20, and 25 wt% PST) also has been investigated. Some preliminary results regarding the influence of composition, strain rate, and temperature on the yield and fracture behavior of these blends will be reported. [Pg.353]

Fig. 5.2 Comparison of creep behavior and time-dependent change in fiber and matrix stress predicted using a 1-D concentric cylinder model (ROM model) (solid lines) and a 2-D finite element analysis (dashed lines). In both approaches it was assumed that a unidirectional creep specimen was instantaneously loaded parallel to the fibers to a constant creep stress. The analyses, which assumed a creep temperature of 1200°C, were conducted assuming 40 vol.% SCS-6 SiC fibers in a hot-pressed SijN4 matrix. The constituents were assumed to undergo steady-state creep only, with perfect interfacial bonding. For the FEM analysis, Poisson s ratio was 0.17 for the fibers and 0.27 for the matrix, (a) Total composite strain (axial), (b) composite creep rate, and (c) transient redistribution in axial stress in the fibers and matrix (the initial loading transient has been ignored). Although the fibers and matrix were assumed to exhibit only steady-state creep behavior, the transient redistribution in stress gives rise to the transient creep response shown in parts (a) and (b). After Wu et al 1... Fig. 5.2 Comparison of creep behavior and time-dependent change in fiber and matrix stress predicted using a 1-D concentric cylinder model (ROM model) (solid lines) and a 2-D finite element analysis (dashed lines). In both approaches it was assumed that a unidirectional creep specimen was instantaneously loaded parallel to the fibers to a constant creep stress. The analyses, which assumed a creep temperature of 1200°C, were conducted assuming 40 vol.% SCS-6 SiC fibers in a hot-pressed SijN4 matrix. The constituents were assumed to undergo steady-state creep only, with perfect interfacial bonding. For the FEM analysis, Poisson s ratio was 0.17 for the fibers and 0.27 for the matrix, (a) Total composite strain (axial), (b) composite creep rate, and (c) transient redistribution in axial stress in the fibers and matrix (the initial loading transient has been ignored). Although the fibers and matrix were assumed to exhibit only steady-state creep behavior, the transient redistribution in stress gives rise to the transient creep response shown in parts (a) and (b). After Wu et al 1...
In Fig. 5.4a and b, the initial creep rate of each phase (Eqn. (7)) is represented by the intersection of the monolithic creep curve for that phase and the elastic stress and strain (vertical line). After initial loading, the total strain rate (elastic + creep) of each phase, which remains equal to the total strain rate of the composite (for compatibility), decreases. The only exception arises if ki 0 = 2,0 (= c,o), so that ec 0 = c ss (see Fig. 5.4c). In this instance, the initial condition matches the steady-state condition—the composite strain rate remains unchanged. The applied stress for this condition is given by... [Pg.172]

If the composite strain rate is known, the composite stress during steady-state isothermal creep can be computed from the rule of mixtures for the stress, Eqn. (9). This gives... [Pg.314]

The latter result indicates that the volumetric strains can be relaxed to some extent by matrix creep. This contrasts with the 3-D case where complete compatibility of strains precludes such relaxation. The extent to which the relaxation occurs has not yet been calculated. However, if it is assumed that the relaxation can be complete so that the matrix volumetric strain is zero, then the fiber stress tends towards aal3lf and, therefore, the composite strain approaches... [Pg.317]

Raman scattering behavior germane to semiconductor nanowires (NWs) and the application of Raman spectroscopy to characterize the structure, composition, strain, and temperature of individual semiconductor nanowires with submicron resolution are discussed. [Pg.477]

In this chapter, we have discussed the unique interactions of electromagnetic radiation with semiconductor NWs that lead to resonant absorption and scattering, the importance of Raman selection rules and phonon confinement in determining the crystal structure of NWs, and the ways in which Raman spectroscopy can be used to measure composition, strain, and temperature quantitatively with submicron resolution. These qualities of Raman spectroscopy are already commonly employed in the characterization of semiconductor NWs, and one may anticipate Raman spectroscopy to be used even more widely as the applications to NW... [Pg.502]

Lattice dynamics in bulk perovskite oxide ferroelectrics has been investigated for several decades using neutron scattering [71-77], far infrared spectroscopy [78-83], and Raman scattering. Raman spectroscopy is one of the most powerful analytical techniques for studying the lattice vibrations and other elementary excitations in solids providing important information about the stmcture, composition, strain, defects, and phase transitions. This technique was successfully applied to many ferroelectric materials, such as bulk perovskite oxides barium titanate (BaTiOs), strontium titanate (SrTiOs), lead titanate (PbTiOs) [84-88], and others. [Pg.590]

The important point is that Ic is a maximum when the stress on the NbaSn reaction layer is approximately zero. The exact amount of total composite strain needed to bring NbaSn out of compression varies considerably, from specimen to specimen, depending on the properties of the bronze layer surrounding the NbsSn, the bronze-to-NbsSn area ratio, reaction heat treatment conditions, and bending strain introduced by spooling the conductor. [Pg.311]

Nb3Sn bronze Nb3Sn Jc degradation onset Up to 1% composite strain (depending on compressive prestress) 0.2% intrinsic Nb3Sn strain... [Pg.315]

Cap Capela, C., Costa, J. D., Ferreira, J. A. M. Test conditions effect on the fracture toughness of hollow glass micro-sphere filled composites. Strain 44 (2008) 141-146. [Pg.551]

Superposition techniques may also be used to correlate stress-strain behavior in the rubbery state. In their study of styrene-acrylonitrile copolymers filled with glass beads, Narkis and Nicolais (1971) obtained stress-strain curves at temperatures above 7. Stress-strain curves were plotted for different fractions of filler, and in terms of both the polymer and composite strain. At a given strain, the stress increased with increasing filler concentration, as expected. It was possible to shift curves of stress vs. polymer strain along the stress axis to produce a master curve (Figure 12.12). In addition to the empirical measurements, an attempt was made to calculate stress-strain curves from the strain-independent relaxation moduli (see Section 1.16 and Chapter 10) by integrating the following equation ... [Pg.395]

Where is composite average stress, is fibers average stress and is matrix average stress. Similarly to the composite stress, the composite strain is defined as the volume average strain, and is obtained as ... [Pg.225]

Xiaoping Shui, Chung DDL, Piezoresistive carbon filament pol5mer-matrix composite strain sensor. Smart Mater Struct, 5, 243-246, 1996. [Pg.1039]

Filammrt which do not exhibit a longitudinal composite strain capability at failure of at least + 0.(X)5 to 0.007 or more cannot be used as a geno engineering... [Pg.327]

Minor amounts of thermally stable neoalkoxy titanate and zirconate additives may provide a means for postreactor, in situ metallocene-like repolymerization catalysis of a filled or unfilled polymer during the plasticization phase. This may result in the creation of metallocene-like (titanocene or zirconocene) behavior associated with effects such as increased composite strain to failure resulting in increased impact toughness or enhanced polymer foamabUity. Other effects to be discussed below with specific examples are related to enhanced processability, reduced polymer chain scission, shortened polymer recrystallization time, and compatibilization of dissimilar polymers. [Pg.92]

Figure 8. Variation of fibre strain, e, measured using Raman spectroscopy with applied composite strain, e for a specially prepared HMS4/PEEK prepreg. The dashed line is for the expected behaviour of an ideal composite where e = e. The solid line is a least squares fit of the experimental data with a slope of 0.92 and an intercept of -0.28%. Figure 8. Variation of fibre strain, e, measured using Raman spectroscopy with applied composite strain, e for a specially prepared HMS4/PEEK prepreg. The dashed line is for the expected behaviour of an ideal composite where e = e. The solid line is a least squares fit of the experimental data with a slope of 0.92 and an intercept of -0.28%.
A side-by-side comparison was made between a implanted polymer strain gauge and a Micro-Measurements precision metal composite strain gauge [26]. The... [Pg.1026]

FIGURE 12 The electrical resistance response to a mechanical impulse of an implanted polymer strain gauge (bottom) and a metal composite strain gauge (top). [Pg.1028]

Fig. 21. Uniaxial tensile stress-strain behavior of HIPS/PS/PXE blends at 20°C showing the effects of matrix composition. Strain rate 4 x 10 s (29). To convert MN/m to psi, multiply by 145. Courtesy of Applied Science Publisher Ltd. Fig. 21. Uniaxial tensile stress-strain behavior of HIPS/PS/PXE blends at 20°C showing the effects of matrix composition. Strain rate 4 x 10 s (29). To convert MN/m to psi, multiply by 145. Courtesy of Applied Science Publisher Ltd.
Laws (1971) indicated that in the pre-cracking stage the composite strain around fibres should be accounted for and the formula for the limit case when was ... [Pg.220]

Calvert, P, et al., 2008. Conducting polymer and conducting composite strain sensors on textiles. Mol. Cryst. Liq. Cryst. 484 (1), 291-657. [Pg.95]


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