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Displacement Calculation

When the part is fully constrained in the mold, no calculation of the displacements is required. After the part is ejected, however, all strain components may be nonzero, and can be evaluated from the following elastic stress-strain relation  [Pg.101]

Alternatively, for simplicity, one can merge the free-quench thermal strains into the initial stresses term and perform an isothermal structural analysis at the room temperature. In this case, Eq. 6.59 is rewritten as [Pg.101]

Here the single term cr°. replaces (4 Cyki ) in Eq. 6.59. If Eq. 6.60 is to be used, the calculation procedure for the in-mold thermally and pressure-induced stress has to be continued to the room temperature. If the material has fully frozen [Pg.101]


Analytical models using classical reservoir engineering techniques such as material balance, aquifer modelling and displacement calculations can be used in combination with field and laboratory data to estimate recovery factors for specific situations. These methods are most applicable when there is limited data, time and resources, and would be sufficient for most exploration and early appraisal decisions. However, when the development planning stage is reached, it is becoming common practice to build a reservoir simulation model, which allows more sensitivities to be considered in a shorter time frame. The typical sorts of questions addressed by reservoir simulations are listed in Section 8.5. [Pg.207]

For a fluid, with no underlying regular structure, the mecin squared displacement gradually increases with time (Figure 6.9). For a solid, however, the mean squared displacement typically oscillates about a mean value. Flowever, if there is diffusion within a solid then tliis can be detected from the mean squared displacement and may be restricted to fewer than three dimensions. For example. Figure 6.10 shows the mean squared displacement calculated for Li+ ions in Li3N at 400 K [Wolf et al. 1984]. This material contains layers of LiiN mobility of the Li" " ions is much greater within these planes than perpendicular to them. [Pg.337]

Table 2.1 Diffusion coefficients and Brownian displacements calculated for uncharged spheres in water at 20°C... Table 2.1 Diffusion coefficients and Brownian displacements calculated for uncharged spheres in water at 20°C...
Using the EAM barriers, for typical parameters T = 320 K and Z = 401 the values for the return probabilities were peq = 1 — 2.4 x 10-7, p[Krp = 1.1 x 10 1, popp = 4.2 x 10 9, and the recombination probability prcc = 1.1 x 10 s. These values depend weakly on Z (e.g. the dependence of the mean square displacement, calculated later in this chapter from the return probabilities, is logarithmic (r2) a log (Z/Zo). This is a consequence of the fact that 2 is the marginal dimension for the return problem of the random walker. In higher-dimensional space the vacancy does not necessarily return and the return probability is asymptotically independent of the lattice size [43]. [Pg.360]

For characterization purposes, the Rf values of the alkaloids are given as Rc values, which are displacements calculated with respect to C-curarine, the most abundant and one of the most stable of the calabash curare alkaloids. Thus ... [Pg.519]

Three-dimensional drawings of normal modes, such as those shown in Chapter 2, can be made from the Cartesian displacement calculations obtained above. However, hand plotting of these data is laborious and complicated. Use of computer plotting programs greatly facilitates this process [95]. [Pg.88]

Figure 6. Evolution of mechanical displacement calculated by AECL and CTH for Section 2 Configuration 3 in the dipping fracture zone (Point I) and in the repository (Point 4). Figure 6. Evolution of mechanical displacement calculated by AECL and CTH for Section 2 Configuration 3 in the dipping fracture zone (Point I) and in the repository (Point 4).
To improve the modeling accuracy, the equivalent bimorph beam model of IPMC, as shown in Fig. 2.38, was developed. It assumes that IPMC has two virtual layers that have the same thickness, and under an imposed electric field, the upper and the lower layers expand or contract, opposing each other. Generally, blocking force and displacement calculations of a bimorph cantilevered beam assume outer layers and an elastic layer between [Wang et al. (1999)]. Here, however, no elastic layer is assumed. Then the relationship between input voltage, V, and induced tip displacement, s, can be written as [Wang et al. (1999)] ... [Pg.44]

Fig. 25. An "S" curve distortion of the rod is expected with shear displacements of L5. But a "C" curve distortion is expected with flexion. Some of both were seen in the rod displacement calculation in the PEA model... Fig. 25. An "S" curve distortion of the rod is expected with shear displacements of L5. But a "C" curve distortion is expected with flexion. Some of both were seen in the rod displacement calculation in the PEA model...
The shaft and the bush thermal displacements calculated in the mid-plane are presented in Fig. 13. Different scales are used on... [Pg.41]

The macroscopic energy and polarization in the field are then for equilibrium displacements calculable by the Lorentz argument with the Clausius Massotti formula as the result for cubic lattices or a uniform continuum with a ieq/Eo =... [Pg.67]

The reaction non-uniqueness is first evident for the partially polymerized phase. As illustrated in Fig, 3, the electron density peaks determined by x-ray diffraction are a consequence of the contributions from unpol)nnerized S2N2 molecules and from the two different types of chains which are equally likely to form from each S2N2 array. As is expected from the small atom displacements calculated for one-half of the sulfur and nitrogen atoms (Fig, 2), these chain atom positions are unresolved from those of unreacted S2N2 molecules (Fig, 3),... [Pg.212]

Cappelletti D, Candori P, Pirano F, Belpassi L, Tarantelli F (2011) Nature and stability of weak halogen bonds in the gas phase molecular beam scattering experiments and ab initio charge displacement calculations. Cryst Growth Des 11 4279-4283... [Pg.455]


See other pages where Displacement Calculation is mentioned: [Pg.206]    [Pg.112]    [Pg.144]    [Pg.124]    [Pg.263]    [Pg.56]    [Pg.124]    [Pg.6378]    [Pg.101]    [Pg.102]    [Pg.158]    [Pg.112]    [Pg.144]    [Pg.175]    [Pg.261]    [Pg.151]    [Pg.169]    [Pg.74]    [Pg.62]    [Pg.6377]    [Pg.323]    [Pg.338]    [Pg.482]    [Pg.15]    [Pg.337]    [Pg.467]    [Pg.570]    [Pg.649]    [Pg.101]    [Pg.249]    [Pg.331]    [Pg.152]    [Pg.140]    [Pg.32]   


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