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Matrix composition, simulation

Specific balance equations for various polymer matrix composites manufacturing processes (i.e., RTM, IP, and AP) have been obtained by simplifying the balance equations. Particular attention has been paid to state all the assumptions used to arrive at the final equations clearly in order to clearly show the range of applicability of the equations. Moreover, appropriate numerical techniques for solution of these coupled partial differential equations have been briefly outlined and a few example simulations have been performed. [Pg.178]

Generator matrix methods are used to compute g, 0, and cp2 > 0 for PVB, PVC, and PS chains as function of the stereochemical composition. Simulations that permit introduction of excluded volume show that for all three chains Is insensitive to /0 unless the stereochemical composition is predominantly racemic. The response of to chain expansion is more dramatic in racemic PVC than in the other two polymers. [Pg.154]

K. L. Mote, P. F. Tortorelli, M. K. Ferber, L. R. Walker, J. R. Keiser, W. D. Bienmall, N. Miralya, J. B. Price, Exposure of Ceramic and Ceramic-Matrix Composites in Simulated and Actual Combustor Environments, Proceedings of International Gas Turbine and Aerospace Congress, Paper No. 99-GT-292 (1999). [Pg.163]

Sinsawat, A., Anderson, K. L., Vaia, R. A., and Farmer, B. L. 2003. Influence of polymer matrix composition and architecture on polymer nanocomposite formation Coarse-grained molecular d)mamics simulation. Journal of Polymer Science, Part B Polymer Physics 41 3272-3284. [Pg.327]

Zaitsev, Y. V., Ashrabov, A. A., Kazatski, M. B. (1986) Simulation of crack propagation in various concrete structures, in Brittle Matrix Composites 1, A. M. Brandt and I. H. Marshall, eds, London Elsevier Applied Science Publishing pp.549-57. [Pg.344]

Li S, Guo ZP, Wang CY, Wallace GG, Liu HK (2013c) Flexible cellulose based polypyrrole-multiwalled carbon nanombe films for bio-compatible zinc batteries activated by simulated body fluids. J Mater Chem A 1(45) 14300-14305 Li W, He D, Bai J (2013d) The influence of nano/micro hybrid structure on the mechanical and self-sensing properties of carbon nanombe-microparticle reinforced epoxy matrix composite. Compos A Appl Sci Manuf 54 28-36... [Pg.202]

In the first configuration, the CP/SPE/CP sandwich stracture is inserted inside the catheter walls. Polypyrrole doped with benzensulfonate anions (PPy/BS ) with an elastic modulus of450 MPa and active strain of 1 % was assumed to be the CP element, and a layer containing Cu(C104)2 with a modulus of 45 MPa was considered as the SPE. In the second configuration, the walls of the catheter are assumed to be made of the CP fibres/SPE matrix composite material. The CP fibres may be PPy or PANi extruded microfibres. In the simulation the fibres were assumed to have the same active and passive properties as their film form. The overall mechanical characteristics of the composite structure are as follows Young modulus 247 MPa, shear modulus 37 MPa and electrochemical strain 1 % [13]. [Pg.239]

Ganesh V V and Chawla N (2005) Effect of Particle Orientation Anisotropy on the Tensile Behavior of Metal Matrix Composites Experiments and Microstructure-Based Simulation, Mater Sci Eng A 391 342-353. [Pg.222]

Li, X.-G. (2014). Modeling and simulation of the gas-atomization process of metal melts for metal-matrix-composite production. Dissertation, University of Bremen, Shaker Verlag. ISBN 978-3-8440-3209-3. [Pg.745]

Another unique approach is to produce a dry aerosol from a standard aqueous solution with a pneumatic nebulizer and desolvator. The aerosol produced by this apparatus is combined with the aerosol from the ablation cell using a dual gas-flow sample introduction system and a gas-mixing cell. By varying the concentration of the analyte in the standard aqueous solution, calibration curves can be created by this procedure. The composition of the standard solution can be adjusted to match the matrix composition of the bulk material of the solid sample, thereby simulating the behavior of the ablated solid in the plasma. Secondary standards can be created by this technique from selected samples. Future calibration curves can be prepared from ablating these secondary standards. [Pg.85]

Most theoretical studies of electrical percolation in composite systems with rodlike fillers assume that the particles are rigid, straight cylinders or spherocylinders. However, this assumption offers a poor description of some important composite systems. For example, electron microscopy studies have revealed that nanotubes embedded in a polymer matrix are generally curved or wavy, rather than straight, as observed in Figure 9. Several authors have conducted theoretical studies to probe the effect of filler waviness on the percolation threshold of composite materials.The percolation threshold was found to increase with inaeasing filler waviness, and this effect was more pronounced for smaller aspect ratios. However, the reported increase in the percolation threshold due to waviness is still small relative the wide spread of experimental threshold values for CNT/polymer composites. Simulations of CNT/ polymer composites also show that filler waviness lowers the composite conductivity. These studies were conducted for highly idealized systems, so the extent of this reduction is not well established. [Pg.337]

The authors of a very recent work [259] simulated the filler effect by applying an effective tensile stress crz in the direction perpendicular to the direction of the tensile stress aT. To determine erz they relied on the condition of equality of the work of external forces which cause deformation of a unit volume of the composite and matrix subjected to the above-mentioned stresses (asymmetric tri-axial stretching). They came up with a formula of the form ... [Pg.37]


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See also in sourсe #XX -- [ Pg.48 ]




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