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Stressed material

Stress of Materials. Low stress materials are essential for dedicated device packaging. To achieve this property a low modulus material with a thermal coefficient of expansion (TCE) match is required. The stress is mainly a result of the following equation ... [Pg.192]

Non-Newtonian fluids include those for which a finite stress 1,. is reqjiired before continuous deformation occurs these are c ailed yield-stress materials. The Bingbam plastic fluid is the simplest yield-stress material its rheogram has a constant slope [L, called the infinite shear viscosity. [Pg.630]

The tubeside fluid must be clean or at least chemically cleanable. With a large number of tubes in the coil, cleaning of inside surfaces is not totally rehable. Fluids that attack stressed materials such as chlorides should be reviewed as to proper coil-material selection. Fluids that contain sohds can be a problem due to erosion of relatively thin coil materials unlike the thick plates in spiral-plate units and multiple, parallel, fluid passages compared to a single passage in spiral-plate units. [Pg.1086]

Stress in crystalline solids produces small shifts, typically a few wavenumbers, in the Raman lines that sometimes are accompanied by a small amount of line broadening. Measurement of a series of Raman spectra in high-pressure equipment under static or uniaxial pressure allows the line shifts to be calibrated in terms of stress level. This information can be used to characterize built-in stress in thin films, along grain boundaries, and in thermally stressed materials. Microfocus spectra can be obtained from crack tips in ceramic material and by a careful spatial mapping along and across the crack estimates can be obtained of the stress fields around the crack. ... [Pg.439]

For freely suspended bioparticles the most likely flow stresses are perceived to be either shear or normal (elongation) stresses caused by the local turbulent flow. In each case, there are a number of ways of describing mathematically the interactions between turbulent eddies and the suspended particles. Most methods however predict the same functional relationship between the prevailing turbulent flow stresses, material properties and equipment parameters, the only difference between them being the constant of proportionality in the equations. Typically, in the viscous dissipation subrange, theory suggests the following relationship for the mean stress [85] ... [Pg.97]

Yielding is a manifestation of the possibility that some of the atoms (or molecules) in the stressed material may slip to new equilibrium positions due to the distortion produced by the applied tensile force. The displaced atoms can form new bonds in their newly acquired equilibrium positions. This permits an elongation over and above that produced by a simple elastic separation of atoms. The material does not get weakened due to the displacement of the atoms since they form new bonds. However, these atoms do not have any tendency to return to their original positions. The elongation, therefore, is inelastic, or irrecoverable or irreversible. This type of deformation is known as plastic deformation and materials that can undergo significant plastic deformation are termed ductile. [Pg.15]

The candidate method is used to support drug synthesis, excipient compatibility, and ultimately to evaluate candidate formulations. Such support typically involves analyses of stressed materials to identify degradation trends. These studies are conducted in the solid state by exposing the DS and DP to relative humidity, temperature, light, and oxidizing... [Pg.163]

Incoherent Clusters. As described in Section B.l, for incoherent interfaces all of the lattice registry characteristic of the reference structure (usually taken as the crystal structure of the matrix in the case of phase transformations) is absent and the interface s core structure consists of all bad material. It is generally assumed that any shear stresses applied across such an interface can then be quickly relaxed by interface sliding (see Section 16.2) and that such an interface can therefore sustain only normal stresses. Material inside an enclosed, truly incoherent inclusion therefore behaves like a fluid under hydrostatic pressure. Nabarro used isotropic elasticity to find the elastic strain energy of an incoherent inclusion as a function of its shape [8]. The transformation strain was taken to be purely, dilational, the particle was assumed incompressible, and the shape was generalized to that of an... [Pg.469]

Polymer modification at the macroscopic level (either as a material subjected to mechanical processing or as a running object) consists of initiating the destructive phenomena at microdefects—that is, at submicroscopic cracks, statistically distributed on the surface or within the body of the stressed material. These cracks become centers where a detachment of intermolecular bonds occurs. This process might be called a mechanical disaggregation, the opposite of aggregation, a term that expresses (in this context) the assembly of various structural elements into polymers. [Pg.86]

Broadly speaking, the mechanical properties can be divided into two classes bulk and interfacial . Within the bulk properties are included the shear and extensional viscosities, moduli and yield stresses (material constants that relate stress to strain or strain rate), and within interfacial rheology are included the wall-slip and friction effects. The interfacial properties are independent of bulk mechanical properties and governed by the frictional or surface forces which are thought to operate at relatively... [Pg.278]

Mass balance is also useful in method validation (1,3,4). In order to demonstrate that analytical methods are stability indicating, unstressed and stressed materials are often compared. An increase in degradation products that correlates well with loss of parent drug aids in demonstrating that the methods can be used to accurately assess degradation. [Pg.182]

Can mixing of thermally stressed material with fresh material be excluded ... [Pg.331]

It is also interesting to briefly consider online measurements of variables different from temperature [5], Since pressure is defined as the normal force per unit area exerted by a fluid on a surface, the relevant measurements are usually based on the effects deriving from deformation of a proper device. The most common pressure sensors are piezoresistive sensors or strain gages, which exploit the change in electric resistance of a stressed material, and the capacitive sensors, which exploit the deformation of an element of a capacitor. Both these sensors can guarantee an accuracy better than 0.1 percent of the full scale, even if strain gages are temperature sensitive. [Pg.34]

Creep is the term used to describe the tendency of a material to move or to deform permanently to relieve stresses. Material deformation occurs as a result of long term exposure to levels of stress (physics) that are below the yield strength or ultimate strength of the material. Creep is more severe in materials that are subjected to heat for long periods and near melting point. Creep is often observed in glasses. Creep is a monotonically increasing function of temperature. [Pg.52]

The exact laws, based on continuum analysis of the fibers and the matrix, would be very complicated. The analysis would involve equilibrium of stresses around, and in, the fibers and compatibility of matrix deformation with the fiber strains. Furthermore, end and edge effects near the free surfaces of the composite material would introduce complications. However, a simplified model can be developed for the interior of the composite material based on the notion that the fibers and the matrix interact only by having to experience the same longitudinal strain. Otherwise, the phases behave as two uniaxially stressed materials. McLean5 introduced such a model for materials with elastic fibers and he notes that McDanels et al.6 developed the model for the case where both the fibrous phase and the matrix phase are creeping. In both cases, the longitudinal parameters are the same, namely... [Pg.310]

This technique was employed in calculating the reliability contours depicted in Fig. 11.4. The reliability contours represent a homogeneously stressed material element, and for dimensionless , the Weibull parameter /3 has units of stress (volume)1/a. Here a, = 5, j3, = 0.2, ac = 35, /3C = 2, abc — 35, and f bc = 2.32. The three surfaces correspond to 0tj = 0.95, 0.5, and 0.05. Note that the reliability contours retain the general behavior of the deterministic failure surface from which they were generated. In general, as the a values increase, the spacing between contours diminishes. Eventually the contours would not be distinct and they would effectively map out a... [Pg.381]

Stress is the forceAinit area applied to the material, while strain is the dimensionless ratio of the iength of the stressed material to its unstressed length. [Pg.12]


See other pages where Stressed material is mentioned: [Pg.188]    [Pg.192]    [Pg.762]    [Pg.439]    [Pg.490]    [Pg.657]    [Pg.986]    [Pg.118]    [Pg.5]    [Pg.324]    [Pg.511]    [Pg.455]    [Pg.98]    [Pg.104]    [Pg.519]    [Pg.129]    [Pg.342]    [Pg.411]    [Pg.188]    [Pg.192]    [Pg.192]    [Pg.59]    [Pg.490]    [Pg.241]    [Pg.56]    [Pg.37]    [Pg.59]    [Pg.586]    [Pg.86]   


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Stress material

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