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Variations in displacements

Using the radical heats of formation published by Tsang [120a], the calculated regioselectivities do not overestimate the experimental values [79]. With the variation in displacements used to calculate fs for H abstractions, in all cycloadditions < , in agreement with their low values. [Pg.97]

Consider a film to a pressure distribution shown in Figure 39.5a. It is assumed that the variation in displacement in the z-direction is zero, that is, = 0 this is referred to as plane-strain deformation. (Note that this does not imply = 0.) First, consider platelike behavior, wherein the bending strain... [Pg.1129]

We have presented a method to analyze the composite displacement and rotation movements. On Tables 1 and 2 we can see the agreement between the experimental values and that obtained from equations (1) or (2). This technique allows to follow the movement in real time, observing directly on the PC screen the ring size and position variations. In this way, we can determine the center and the radius of the ring. [Pg.659]

The transfonnation matrix L is obtained from a nonnal-mode analysis perfonned in internal coordmates [59, ]. Thus, as the evolution of the nonnal-mode coordinates versus time is evaluated from equation (A3.12.49), displacements in the internal coordinates and a value for q are found from equation (A3.12.50). The variation in q with time results from a superposition of the nonnal modes. At a particular time, the... [Pg.1025]

Chambers A and B are separated by an elastic rubber membrane whose motion in response to pressure differences is transmitted to the needle N. Variations in the pressure difference can then be followed by observing the displacement of the point of the needle. Initially chamber A and the capillary are filled to the desired pressure by opening cocks and C, ... [Pg.56]

Fig. 6.9 Variation in mean squared displacement during the initial steps of a molecular dynamics simulation of argon. Fig. 6.9 Variation in mean squared displacement during the initial steps of a molecular dynamics simulation of argon.
The two principal elements of evaporator control are evaporation rate a.ndproduct concentration. Evaporation rate in single- and multiple-effect evaporators is usually achieved by steam-flow control. Conventional-control instrumentation is used (see Sec. 22), with the added precaution that pressure drop across meter and control valve, which reduces temperature difference available for heat transfer, not be excessive when maximum capacity is desired. Capacity control of thermocompression evaporators depends on the type of compressor positive-displacement compressors can utilize speed control or variations in operating pressure level. Centrifugal machines normally utihze adjustable inlet-guide vanes. Steam jets may have an adjustable spindle in the high-pressure orifice or be arranged as multiple jets that can individually be cut out of the system. [Pg.1148]

Note that because of the absence of the variations in in-plane displacements, 5u and 5v, the boundary conditions are much simpler than the general case in Equation (5.20). [Pg.303]

The solution to this fourth-order partial differential equation and associated homogeneous boundary conditions is just as simple as the analogous deflection problem in Section 5.3.1. The boundary conditions are satisfied by the variation in lateral displacement (for plates, 5w actually is the physical buckle displacement because w = 0 in the membrane prebuckling state however, 5u and 8v are variations from a nontrivial equilibrium state. Hence, we retain the more rigorous variational notation consistently) ... [Pg.304]

The presence of D g 26 governing differential equation and the boundary conditions renders a closed-form solution impossible. That is, in analogy to both bending and buckling of a symmetric angle-ply (or anisotropic) plate, the variation in lateral displacement, 5vy, cannot be separated into a function of x alone times a function of y alone. Again, however, the Rayleigh-Ritz approach is quite useful. The expression... [Pg.318]

Since niobates and tantalates belong to the octahedral ferroelectric family, fluorine-oxygen substitution has a particular importance in managing ferroelectric properties. Thus, the variation in the Curie temperature of such compounds with the fluorine-oxygen substitution rate depends strongly on the crystalline network, the ferroelectric type and the mutual orientation of the spontaneous polarization vector, metal displacement direction and covalent bond orientation [47]. Hence, complex tantalum and niobium fluoride compounds seem to have potential also as new materials for modem electronic and optical applications. [Pg.9]

In the pneumatic pumping system, the pressure (and not the flow rate) is maintained constant as variations in chromatographic conditions occur. Thus, a change in mobile phase viscosity (e.g. gradient elution) or column back pressure will result in a change in flow rate for these types of pumps. The gas displacement pump in which a solvent is delivered to the column by gas pressure is an example of such a pneumatic pump. The gas displacement system is among the least expensive pumps available and is found in several low cost instruments. While the pump is nonpulsating and hence, produces low noise levels with the detectors in current use, its flow stability and reproducibility are only adequate. In addition, its upper pressure limit is only 2000 psi which may be too low in certain applications. [Pg.232]

In a multiphase formulation, such as an oil-in-water emulsion, preservative molecules will distribute themselves in an unstable equilibrium between the bulk aqueous phase and (i) the oil phase by partition, (ii) the surfactant micelles by solubilization, (iii) polymeric suspending agents and other solutes by competitive displacement of water of solvation, (iv) particulate and container surfaces by adsorption and, (v) any microorganisms present. Generally, the overall preservative efficiency can be related to the small proportion of preservative molecules remaining unbound in the bulk aqueous phase, although as this becomes depleted some slow re-equilibration between the components can be anticipated. The loss of neutral molecules into oil and micellar phases may be favoured over ionized species, although considerable variation in distribution is found between different systems. [Pg.367]

Oil recovery can also be affected by extreme variations in rock permeability, such as when high-permeability thief zones between injectors and producers allow most of the injected drive fluid to channel quickly to producers, leaving oil in other zones relatively unrecovered. A need exists for a low-cost fluid that can be injected into such thief zones (from either injectors or producers) to reduce fluid mobility, thus diverting pressure energy into displacing oil from adjacent lower-permeability zones. [Pg.201]


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