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Micro-scale stress

A failure of a thermal-structural component is not only governed by the transient macro-scale thermal stress field induced by a transient temperature field, but also by its micro-scale stress field if the component material consists of several phases (such as a composite component, which often contains a reinforcement and a matrix). The experimental investigation of the nticrostmctural factors, which control the thermal shock resistance of a composite component, is very difficult. Some theoretical calculation of the thermal stress of various components upon heating/ cooling has been well documented, but these works mainly focus on the macro-scale... [Pg.510]

Micro-Scale Stress Field in the Composite Sample... [Pg.524]

Stresses acting on micro-organisms in (a) to (c) are derived on the premise that the flow forces originate from the turbulent motion of the carrier medium. In almost all cases, turbulence is assumed to be locally isotropic and homogeneous which greatly simplifies the analysis and allows the application of the Kolmogoroff s theory of turbulence to the problem [81]. The Kolomogoroff micro-scale of turbulence,... [Pg.96]

In an optical micrograph of a commercially available nitinol stent s surface examined prior to implantation, surface craters can readily be discerned. These large surface defects are on the order of 1 to 10 p.m and are probably formed secondary to surface heating during laser cutting. As mentioned above, these defects link the macro and micro scales because crevices promote electrochemical corrosion as well as mechanical instability, each of which is linked to the other. Once implanted, as the nitinol is stressed and bent, the region around the pits experiences tremendous, disproportionate strain. It is here that the titanium oxide layer can fracture and expose the underlying surface to corrosion (9). [Pg.350]

The importance of controlling the working electrode potential in electrosyntheses aiming at mechanistic studies has already been stressed (Sect. 4.4 ). In general, potential control seems to be indispensable for mechanistic investigations but in many cases one can do without it in synthetic work, once it has been established that the desired reaction is not sensitive towards the intermediates formed in the SSE decomposition process. Thus, the exploration of a reaction for synthetic purposes would follow the pattern 1) voltammetric studies in an inert SSE, 2) voltammetric studies in the SSE of interest (if possible), 3) cpe on a semi-micro scale at different potentials, and 4) constant current electrolyses on a large scale, if the cpe experiments have indicated that this is feasible. [Pg.32]

The modulus and yield kinetic parameters of the block polymer B can be related to those of the homopolymer in terms of a microcomposite model in which the silicone domains are assumed capable of bearing no shear load. Following Nielsen (10) we successfully applied the Halpin-Tsai equations to calculate the ratio of moduli for the two materials. This ratio of 2 is the same as the ratio of the apparent activation volumes. Our interpretation is that the silicone microdomains introduce shear stress concentrations on the micro scale that cause the polycarbonate block continuum to yield at a macroscopic stress that is half as large as that for the homopolymer. The fact that the activation energies are the same however indicates that aside from this geometric effect the rubber domains have little influence on the yield mechanism. [Pg.324]

Thermal residual stresses are inherent to fibre reinforced composites due to the heterogeneity of the thermo-mechanical properties of their two constituents. Such stresses build up when composite structures are cooled down from the processing temperature to the test temperature. Residual stresses will be present on both a fibre-matrix scale (micro-scale), and on a ply-to-ply scale (macro-scale) in laminates built up from layers with different orientations. It is recognised that these stresses should be taken into account in any stress analysis. [Pg.465]

The main micro-scale controls on dilatancy during shear failure in shales can be described by considering the processes taking place in a stressed rock element. Strain begins to localise in the sample at peak differential stress and this leads to the formation of undulating shear zones (shear fractures). Sliding on... [Pg.171]

Chemical reactions normally occur in the micro-scale range. In turbulent flow, almost all of the power dissipation occurs eventually in the micro-scale regime because that is the only place where the scale of the fluid fluctuations is small enough that viscous shear stress exists. At approximately 100 pm, the fluid does not know what type of impeller is used to generate the power continuing down to 10 pm and, even further, to chemical reactions, the actual impeller type is not a major vaii-... [Pg.1951]

In turbulent flow range, turbulence exists on the micro- and the macro-scale. The micro-scale 2 is responsible for the shear stress, which for a particle size (dp) which is significantly smaller than 2 (2/dp = 5-25), can influence the particle size of the dispersed phase. [Pg.17]

Performing macro-scale experiments it has been observed that the normal surface tension force induces higher normal stresses in the fluid on the concave side of the interface than on the other fluid on the convex side of the interface. In a micro-scale view we may say that this interfacial tension force is exerted by the interfacial material lying on the convex side of the surface upon the material lying on the concave side. The normal component of the surface force is thus frequently (not always ) defined positive into the mean curvature of the surface, in line with the physical observations. The direction of the normal component of the interface force given by (3.9) is determined by two factors, the interface normal unit vector n/ which we have defined positive into the curvature, and the mean curvature variable which we have chosen to define as an absolute value. That is, the variable used here determining the mean curvature of the surface Hi = ( i + K2)/ 2) is consistent with the definition... [Pg.348]

The mean energy dissipation rate can be calculated directly from the energy spectrum using (1.332). Moreover, for isotropic turbulence, the energy dissipation rate and the micro scale are related as expressed by (1.323). Caution is required using the dissipation rate calculated from a turbulence model like the k-e model as in this model the dissipation quantity is merely a tuning variable for the shear stresses in a pipe and not necessarily a true physical dissipation rate. The latter approach requires validation for any applications. [Pg.703]

Electrochemical tree growth, the electrical equivalent of environmental stress cracking (Chapter 10), occurs at lower electric stresses. The chemical species vary. Lead salts from petroleum entered a cable buried near a petrol station, whereas hydrogen sulphide from the decomposition of seaweed entered an undersea cable. The whole gamut of polyethylene degradation reactions occur on a micro-scale inside such trees. To avoid such failures, the cable can be fitted with an impervious outer layer, such as a lead sheath. [Pg.360]

The SCC properties are typically anisotropic properties. Most cases of SCC in high-strength aluminium alloys have been connected with stresses in the short transverse direction. The cracks in A1 alloys may be branched on a macro or micro scale depending on the load level. SCC in aluminium alloys may be prevented by cathodie protection. [Pg.169]

It is well established in the literatme, that the incorporation of rigid micro-scaled fillers usually increases composite stiffness, but at the expense of ductility. This is due to the stress concentration regions that exist in close proximity of the reinforcement. In the case of nanoscaled fillers, in contrast, the stress concentrations are significantly reduced. Hence, composite ductility can be retained at a constant level or even improved, in comparison to neat polymer [8]. It has been shown that some nanocomposites may lead to significant and simultaneous improvements in stiflhess, fracture toughness, impact energy absorption and vibration damping. These characteristics could be of particular importance in some structural apphca-tions such as in the automotive and aircraft industries [4]. [Pg.509]

The structure of the closure laws used for the shear stresses in two-fluid models bears crucial consequences on the capability of two-fluid models to predict the stability characteristics of the presumed flow configuration. Quasi-steady closure laws for the interfacial shear stresses, which are widely used in stability analyses of the stratified flow configuration, are insufficient for capturing the physical phenomena involved during the evolution of waves over a liquid interface sheared by a turbulent gas phase. Modification of the interfacial shear stress model to include a dynamic term is essential for rendering a closure law which is capable of bridging the gap between the micro-scale phenomena at the vicinity of the phases interface and the macro-averaged representation of the flow. [Pg.370]

One effect that sustained exposure to elevated temperature has is to stabilize the structure of the material. The processing of polymer materials frequently leaves residual stresses of various types in the material. In addition, the cooling rate on a polymer with a crystalline structure may be such that the equilibrium is not reached during processing. Sustained exposure to heat will result in relaxation of the residual frozen-in stresses and/or the recrystallization of the material. Both of these effects involve movement of the material on a molecular or micro scale with a consequent distortion of the overall shape of the object. In the case of a quenched polyethylene film which has a high degree of clarity, the effect of the recrystallization would be to increase the haze level so that the material becomes opalescent or even opaque. [Pg.20]

Table 12 The values of micro-scale creep jumps L at different deformations e for two semicrystalline samples with different spherulite sizes (T = 20°C, compressive stress cr = 70MPa) [320]... Table 12 The values of micro-scale creep jumps L at different deformations e for two semicrystalline samples with different spherulite sizes (T = 20°C, compressive stress cr = 70MPa) [320]...
A review of Slow Crack Growth (SCG) results obtained for different oxide and nonoxide ceramics at ambient temperature, under different enviromnents, is presented. They are analyzed on the basis of their crack velocity (V) versus stress intensity factor (Ki) diagrams. The aim of this paper is to consider mechanisms acting at the crack tip (i.e. at the nano-scale) and microstructural mechanisms occurring in the crack wake or at the crack front (i.e. at the micro-scale) to rationalize the approach of SCG. [Pg.513]

Figure 7.4. (a) Visualizing the interphase considering only the micro-scale. Interphase is a continuum layer with a gradient of properties reflecting variations in its structure. The main role of the micro-scale interphase is to provide stable and effective ineans for stress transfer between inclusions and polymer matrix even under adverse conditions, (b) Visualizing the structure of a micro-composite considering also the nano-scale structural features when the discrete structure of the matrix and inclusions becomes evident [169]... [Pg.265]


See other pages where Micro-scale stress is mentioned: [Pg.44]    [Pg.511]    [Pg.44]    [Pg.511]    [Pg.1633]    [Pg.27]    [Pg.97]    [Pg.97]    [Pg.99]    [Pg.1454]    [Pg.365]    [Pg.131]    [Pg.374]    [Pg.501]    [Pg.1637]    [Pg.209]    [Pg.199]    [Pg.713]    [Pg.508]    [Pg.393]    [Pg.234]    [Pg.323]    [Pg.19]    [Pg.220]    [Pg.259]    [Pg.262]    [Pg.264]    [Pg.264]   
See also in sourсe #XX -- [ Pg.510 , Pg.524 ]




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