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Size modulus

Here, again, at fixed particle size, modulus is a function of both iodine number and structure, but extrusion swell is a function of structure only. The cross-hatched area is the quality control target area for that particular black to be in specification. [Pg.306]

Gaudin-Schuhmann equation, that is, y = 100 (x/k)a, where a (the distribution modulus) is aconstant for a particular size distribution, and k (the size modulus) is the 100 percent size, in microns, of the extrapolated straight-line portion of the plot. By applying least-squares curve fitting to the log-log plot, the values of a and k can be obtained, yielding y = 100(x/2251) 003. [Pg.469]

In summary, the stress (typically at the edge of the die) increases with die size, modulus of the adhesive, temperature, difference in expansion coefficients, and increasing bondline thickness." ... [Pg.67]

The distribution modulus (m) and the size modulus <763.2 must be known to determine the size distribution of a particular coal. [Pg.4]

Schu Mixer. A continuous mixer for powders or for powders and liquids (Schurmans Van Ginneken). Schuhmann Equation. An equation for the particle-size distribution resulting from a crushing process y = 100(a cumulative percentage finer than jc, a is the distribution modulus, and K is the size modulus a and K are both constants. (R. Schuhmann, Amer. Inst Min. Engrs., Tech. Paper, 1189,1940) cf. gaudin s equation). [Pg.274]

Matrix/rubber/ CTBN Silica Size Modulus Increment Gic Increment... [Pg.435]

Modulus It is the resistance to an applied force per unit area (stress/strain). It differs from stiffness only in that the sample geometry is taken into account. Therefore it has a constant value for a given material, irrespective of sample size. Modulus is a measure of how a material resists the application of stress i.e. small displacement means high modulus. Unit Pa or Pascals (N/m ). Modulus is given a different symbol dependent upon how it is measiued Yoimg s modulus (also Flexure or Tension deformation modes in DMA) are given the symbol E, Shear the symbol G, Bulk the symbol K. [Pg.455]

Coherent states and diverse semiclassical approximations to molecular wavepackets are essentially dependent on the relative phases between the wave components. Due to the need to keep this chapter to a reasonable size, we can mention here only a sample of original works (e.g., [202-205]) and some summaries [206-208]. In these, the reader will come across the Maslov index [209], which we pause to mention here, since it links up in a natural way to the modulus-phase relations described in Section III and with the phase-fiacing method in Section IV. The Maslov index relates to the phase acquired when the semiclassical wave function haverses a zero (or a singularity, if there be one) and it (and, particularly, its sign) is the consequence of the analytic behavior of the wave function in the complex time plane. [Pg.108]

Secondly, the ultimate properties of polymers are of continuous interest. Ultimate properties are the properties of ideal, defect free, structures. So far, for polymer crystals the ultimate elastic modulus and the ultimate tensile strength have not been calculated at an appropriate level. In particular, convergence as a function of basis set size has not been demonstrated, and most calculations have been applied to a single isolated chain rather than a three-dimensional polymer crystal. Using the Car-Parrinello method, we have been able to achieve basis set convergence for the elastic modulus of a three-dimensional infinite polyethylene crystal. These results will also be fliscussed. [Pg.433]

Fig. 6. The calculated Young s modulus as a function of cut-off energy (basis set size). Convergence is basically reached for a cut-off of 54 Ry. Fig. 6. The calculated Young s modulus as a function of cut-off energy (basis set size). Convergence is basically reached for a cut-off of 54 Ry.
Table II.1 which depends on the pellet size, so the familiar plot of effectiveness factor versus Thiele modulus shows how t varies with pellet radius. A slightly more interesting case arises if it is desired to exhibit the variation of the effectiveness factor with pressure as the mechanism of diffusion changes from Knudsen streaming to bulk diffusion control [66,... Table II.1 which depends on the pellet size, so the familiar plot of effectiveness factor versus Thiele modulus shows how t varies with pellet radius. A slightly more interesting case arises if it is desired to exhibit the variation of the effectiveness factor with pressure as the mechanism of diffusion changes from Knudsen streaming to bulk diffusion control [66,...
For nosetip materials 3-directional-reinforced (3D) carbon preforms are formed using small cell sizes for uniform ablation and small pore size. Figure 5 shows typical unit cell dimensions for two of the most common 3D nosetip materials. Carbon-carbon woven preforms have been made with a variety of cell dimensions for different appHcations (27—33). Fibers common to these composites include rayon, polyacrylonitrile, and pitch precursor carbon fibers. Strength of these fibers ranges from 1 to 5 GPa (145,000—725,000 psi) and modulus ranges from 300 to 800 GPa. [Pg.5]

Spandex fibers are available as fine as 1.1 tex (10 den), and the finest extmded latex thread available is about 16 tex (140 den). The availabihty of spandex fibers in such fine sizes and their unique properties compared to mbber, eg, dyeabiUty, high modulus, abrasion resistance, and whiteness, has allowed extensive penetration into hosiery and sportswear markets. [Pg.310]

Density and polymer composition have a large effect on compressive strength and modulus (Fig. 3). The dependence of compressive properties on cell size has been discussed (22). The cell shape or geometry has also been shown important in determining the compressive properties (22,59,60,153,154). In fact, the foam cell stmcture is controlled in some cases to optimize certain physical properties of rigid cellular polymers. [Pg.412]

Fig. 4. Schematic representation of a two-dimensional model to account for the shear modulus of a foam. The foam stmcture is modeled as a coUection of thin films the Plateau borders and any other fluid between the bubbles is ignored. Furthermore, aH the bubbles are taken to be uniform in size and shape. Fig. 4. Schematic representation of a two-dimensional model to account for the shear modulus of a foam. The foam stmcture is modeled as a coUection of thin films the Plateau borders and any other fluid between the bubbles is ignored. Furthermore, aH the bubbles are taken to be uniform in size and shape.
Ultrasonic Microhardness. A new microhardness test using ultrasonic vibrations has been developed and offers some advantages over conventional microhardness tests that rely on physical measurement of the remaining indentation size (6). The ultrasonic method uses the DPH diamond indenter under a constant load of 7.8 N (800 gf) or less. The hardness number is derived from a comparison of the natural frequency of the diamond indenter when free or loaded. Knowledge of the modulus of elasticity of the material under test and a smooth surface finish is required. The technique is fast and direct-reading, making it useful for production testing of similarly shaped parts. [Pg.466]

Although sealant manufacturer s Hterature commonly reports modulus values, these values must be interpreted carefully. Specimen sizes, test rate, cure conditions, and the time a sealant has been allowed to cure when tested can all have a significant effect on modulus. Therefore, for a tme comparison, sealants should be evaluated by a standard test that examines all sealants by the same procedure. In general, the longer a sealant has been allowed to cure, the more reaUstic the modulus data. [Pg.309]

Empirical attempts have been made to relate strip and grab test results, particularly for cotton fabrics, so that if one strength is known, the other can be calculated. The relationship is complex, depending on fiber strength and modulus, yam size and crimp, yam-to-yam friction, fabric cover factor, weave, weight, and other factors (19). [Pg.459]

Copolymerisation also affects morphology under other crystallisation conditions. Copolymers ia the form of cast or molded sheets are much more transparent because of the small spheruHte size. In extreme cases, crystallinity cannot be detected optically, but its effect on mechanical properties is pronounced. Before crystallisation, films are soft and mbbery, with low modulus and high elongation. After crystallisation, they are leathery and tough, with higher modulus and lower elongation. [Pg.432]

In addition to chemical analysis a number of physical and mechanical properties are employed to determine cemented carbide quaUty. Standard test methods employed by the iadustry for abrasive wear resistance, apparent grain size, apparent porosity, coercive force, compressive strength, density, fracture toughness, hardness, linear thermal expansion, magnetic permeabiUty, microstmcture, Poisson s ratio, transverse mpture strength, and Young s modulus are set forth by ASTM/ANSI and the ISO. [Pg.444]


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See also in sourсe #XX -- [ Pg.524 ]




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Bulk modulus size dependence

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