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Book: Composites
Series: ASM Handbook
Volume: 21
Publisher: ASM International
Published: 01 January 2001
DOI: 10.31399/asm.hb.v21.a0003374
EISBN: 978-1-62708-195-5
... interphase thermodynamics surface energy contact angle solid surface energy wetting wicking glass fiber polymeric fiber carbon fiber composite laminate test mechanical properties composite on-axis properties composite off-axis properties composite fracture properties interfaces FIBER...
Abstract
Fiber-matrix adhesion is a variable to be optimized in order to get the best properties and performance in composite materials. This article schematically illustrates fiber matrix interphase for composite materials. It discusses thermodynamics of interphase in terms of surface energy, contact angle, work of adhesion, solid surface energy, and wetting and wicking. The article describes the change in interphase depending on the reinforcing fiber such as glass fiber, polymeric fiber, and carbon fiber. It emphasizes fiber-matrix adhesion measurements by direct methods, indirect methods, and composite laminate tests. The effects of interphase and fiber-matrix adhesion on composite mechanical properties, such as composite on-axis properties, composite off-axis properties, and composite fracture properties, are also discussed.
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Published: 31 October 2011
Fig. 5 (a) Plot of linear void density (LVD) versus five interfaces and (b) the corresponding optical image of interface number 5. The LVD point for each interface was taken at the high point, as shown in (a). Note: Linear void density is the inverse of linear weld density. Source: Ref 8
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Published: 01 January 1994
Fig. 12 Times required for interfaces of two steel parts of equal area but different mass to reach baking temperature of 150 °C (300 °F)
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Published: 01 January 1994
Fig. 1 Schematic of light reflected and transmitted at film interfaces. The outgoing beam is a combination of all of the rays emerging from film from the top interface. Each material is characterized by the index of refraction N 1 . The thickness of the film is d. Source: Ref 8
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Published: 01 December 2004
Fig. 2 Different types of interfaces. (a) and (b) Fully coherent. (c) and (d) Semicoherent showing lattice strain and the presence of dislocations. (e) and (f) Incoherent. Source: Ref 1
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in Metallography and Microstructures of Carbon and Low-Alloy Steels[1]
> Metallography and Microstructures
Published: 01 December 2004
Fig. 34 Microstructure of the interfaces between specimens mounted, polished, and etched in a steel clamp. Note the excellent edge retention. 2% nital etch. Original magnification 100×
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in Failure Analysis of Medical Devices
> Analysis and Prevention of Component and Equipment Failures
Published: 30 August 2021
Fig. 11 Optical micrographs showing fretting damage at the screw-plate interfaces of a titanium bone plate
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in Aluminum Alloy Design for Additive Manufacturing
> Additive Manufacturing Design and Applications
Published: 30 June 2023
Fig. 5 Log-scale proximity histogram for the six large interfaces identified with the Er + Yb 2.0 at.% isosurfaces. Negative distance is outside of the feature;
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Published: 30 June 2023
Fig. 19 Illustrative example of functional interfaces needing a support structure or being self-supported. (a) Circular cross section. (b) Tear-drop cross section
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Published: 30 June 2023
Fig. 22 Extract functional interfaces (FIs) and system boundaries (SBs) and establish function- FI mappings. (a) Candidacy assembly design. (b) Hollow shaft FI decomposition. (c) All FIs and SBs
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Published: 15 May 2022
Fig. 4 The Stribeck curve demonstrates how sliding interfaces with added liquid lubricant transition through the major lubrication regimes. As the fluid film thickness ratio increases, asperity contact and friction coefficient initially decrease until viscous forces begin to dominate over
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Published: 15 January 2021
Fig. 15 Illustration of the fretting wear process related to metal interfaces (incubation period related to the formation of tribological transformed structure, or TTS). Adapted from Ref 42 . Reprinted with permission from Elsevier
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Published: 30 September 2015
Fig. 11 SEM image of an embrittled WHA in which W-matrix interfaces were too weak to transfer sufficient stress to induce W cleavage. The matrix simply detached from the spheroids.
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Published: 01 June 2016
Fig. 23 Different types of interfaces. (a) and (b) Fully coherent. (c) and (d) Semicoherent showing lattice strain and the presence of dislocations. (e) and (f) Incoherent. Source: Ref 20
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Published: 01 June 2016
Fig. 13 Different types of interfaces. (a) and (b) Fully coherent. (c) and (d) Semicoherent showing lattice strain and presence of dislocations. (e) and (f) Incoherent. Source: Ref 41
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Published: 31 October 2011
Fig. 3 Calculated temperatures at weld interface (WI) and electrode interfaces (EI) for geometry shown in Fig. 2 as a function of molybdenum electrode polarity
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Published: 01 January 2000
Fig. 4 Crack growth rates along plain and patterned glass/copper interfaces in wet and dry gaseous nitrogen environments
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Published: 01 January 2000
Fig. 5 Hydrogen effects on strain energy release rates for Cu/Ti/SiO 2 interfaces
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in Heat-Transfer Interface Effects for Solidification Processes
> Fundamentals of Modeling for Metals Processing
Published: 01 December 2009
Fig. 3 Experimentally determined values of h ( t ) for interfaces in a tube-shaped casting of various aluminum alloys. AC8A is an aluminum-silicon (plus copper or magnesium) alloy, JIS H5205, similar to UNS A03360. (a) Outer interface. (b) Inner casting-mold interface. Source: Ref 5
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Published: 01 December 2009
Fig. 2 Graphical user interfaces of artificial neural-network software for simulation and prediction of various correlations in titanium alloys. (a) Time-temperature transformation (TTT) diagrams. (b) Mechanical properties of conventional titanium alloys. (c) Fatigue stress life diagrams. (d
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