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Functional instabilities

Another method of classifying instabilities is by the functional zone in which the instability originates. Thus, the following instabilities can be distinguished  [Pg.828]

Screw design changes that can improve the melting capahility are  [Pg.830]

Devolatilization instabilities can be caused by plugging of the vent port, variation in the vacuum level, or by variations of the volatile level in the feedstock. The efficiency of devolatilization can be improved by  [Pg.830]

The polymer melt has to be well mixed when it leaves the extruder screw and enters into the die. For this reason it is beneficial to have an efficient distributive mixing device at the very end of the screw. Mixing was discussed in detail in Section 7.7 and mixing devices and mixing screws in Section 8.7. [Pg.831]

In addition to have efficient mixing devices along the screw, there are several other issues that are important in achieving good mixing. The method of feeding plays an important role in the mixing action in the extruder. [Pg.831]


Another aspect of wave function instability concerns symmetry breaking, i.e. the wave function has a lower symmetry than the nuclear framework. It occurs for example for the allyl radical with an ROHF type wave function. The nuclear geometry has C21, symmetry, but the Cay symmetric wave function corresponds to a (first-order) saddle point. The lowest energy ROHF solution has only Cj symmetry, and corresponds to a localized double bond and a localized electron (radical). Relaxing the double occupancy constraint, and allowing the wave function to become UHF, re-establish the correct Cay symmetry. Such symmetry breaking phenomena usually indicate that the type of wave function used is not flexible enough for even a qualitatively correct description. [Pg.76]

A comparison of HF, MP2 and density functional methods in a system with Hartree-Fock wave function instabilities, ONO—OM (for M = Li, Na and K), shows that DFT methods are able to avoid the problems that ab initio methods have for this difficult class of molecules. The computed MP2 frequencies and IR intensities were more affected by instabilities than HF. The hybrid B3LYP functional reproduced the experimental frequencies most reliably. The cis,cis conformation of ONO—OM was highly preferred because of electrostatic attraction and was strongest in the case where M = Li. The small Li cation can fit in best in the planar five-membered ring. This is completely different from the nonionic... [Pg.9]

In contrast to dioxirane oxidation, the transition states for carbonyl oxide oxidation are not affected as much by RHF-UHF wave function instability problems, and there is good agreement between the MP2, MP4 and QCISD(T) barrier heights. Methyl substitution on the carbonyl oxide has very little effect on the barrier heights, but it can be anticipated that methyl substitution of the aUtene would lower the barriers significantly . The calculated changes in the barriers due to solvation are much smaller than for dioxirane oxidation, primarily because the differences between the reactant and transition state dipoles are smaller. [Pg.37]

Another aspect of wave function instability concerns symmeity r kmg, i.e. the wave fimction has a lower S5munetry than the nuclear framework. It occurs for example for the allyl radical with an ROHF type wave function. The nuclear geometry... [Pg.76]

It is not the presence of wave-function instabilities that poses problems for the calculation of molecular properties, but rather the presence of nearinstabilities. It is entirely possible to obtain quite satisfactory results with a highly unstable HF-SCF solution, and it is also entirely possible to obtain completely absurd results with a stable solution. The important issue is the smallest eigenvalue of the A matrix in magnitude, irrespective of sign.27... [Pg.124]

Gentile, M. E., Jessup, C. M., Nyman, J. L., Griddle, C. S. (2007). Correlation of functional instability and conamunity dynamics in denitrifying dispersed-growth reactors. Applied and Environmental Microbiology, 73(3), 680-690. [Pg.726]

Patients with chronic lateral ankle injuries and functional instability can have various problems that can cause confusion reaching a specific diagnosis. Although uncommon, PTD is one cause of lateral ankle dysfunction. PTD may include fissures, fraying, partial thickness tears, full thickness tears, subluxation, or complete... [Pg.168]

Clancy WG Jr (1983) Anterior cruciate ligament functional instability a static intra-articular and dynamic extra-articular procedure. Clin Orthop Relat Res 172 102-106... [Pg.171]

Fig. 16.6 The paced QRS complexes in this 12-lead ECG have an inferiorly directed mean frontal plane axis, and a left bundle branch block pattern. This suggests that pacing is occurring in the right ventricle, from the area of the outflow tract or high septum. This position is not associated with pacing function instability in permanent systems in temporary pacing systems, however, right ventricular outflow tract lead position is not stable and revision is required. Fig. 16.6 The paced QRS complexes in this 12-lead ECG have an inferiorly directed mean frontal plane axis, and a left bundle branch block pattern. This suggests that pacing is occurring in the right ventricle, from the area of the outflow tract or high septum. This position is not associated with pacing function instability in permanent systems in temporary pacing systems, however, right ventricular outflow tract lead position is not stable and revision is required.
The ti eatment of the Jahn-Teller effect for more complicated cases is similar. The general conclusion is that the appearance of a linear term in the off-diagonal matrix elements H+- and H-+ leads always to an instability at the most symmetric configuration due to the fact that integrals of the type do not vanish there when the product < / > / has the same species as a nontotally symmetiic vibration (see Appendix E). If T is the species of the degenerate electronic wave functions, the species of will be that of T, ... [Pg.589]

W, g potential functions, k 1, has been discussed in various papers (see, for example, [6, 11, 9, 16, 3]). It has been pointed out that, for step-sizes /j > e = 1/ /k, the midpoint method can become unstable due to resonances [9, 16], i.e., for specific values of k. However, generic instabilities arise if the step-size k is chosen such that is not small [3, 6, 18], For systems with a rotational symmetry this has been shown rigorously in [6j. This effect is generic for highly oscillatory Hamiltonian systems, as argued for in [3] in terms of decoupling transformations and proved for a linear time varying system without symmetry. [Pg.282]

Chemical conversion of compounds to intermediates of known absolute configuration is a method routinely used to determine absolute configuration (86). This is necessary because x-ray analysis is not always possible suitable crystals are required and deterrnination of the absolute configuration of many crystalline molecules caimot be done because of poor resolution. Such poor resolution is usually a function of either molecular instability or the complex nature of the molecule. For example, the relative configuration of the macroHde immunosuppressant FK-506 (105) (Fig. 8), which contains 14 stereocenters, was determined by x-ray crystallographic studies. However, the absolute configuration could only be elucidated by chemical degradation and isolation of L-pipecoUc acid (110) (80). [Pg.249]

Phase Diagram (Zenz and Othmer) Zenz and Othmer (op. cit.) have graphically represented (Fig. 17-2) all gas-solid svstems in which the gas is flowing counter to gravity as a function o pressure drop per unit of height versus velocity. Note that line OAB in Fig. 17-2 is the pressure-drop versus gas-velocity curve for a packed bed and BD the cui ve for a fluid bed. Zenz indicates an instability between D and H because with no sohds flow all the particles will be entrained from the bed however, if sohds are added to replace those entrained, system JJ prevails. The area DHJJ will be discussed further. [Pg.1560]

Silyl-derived protective groups are also used to mask the thiol function. A complete compilation is not given here since silyl derivatives are described in the section on alcohol protection. The formation and cleavage of silyl thioethers proceed analogously to simple alcohols. The Si—S bond is weaker than the Si—O bond, and therefore sulfur derivatives are more susceptible to hydrolysis. For the most part silyl ethers are rarely used to protect the thiol function because of their instability. Silyl ethers have been used for in situ protection of the — SH group during amide formation. ... [Pg.297]

It is noteworthy that eq. (4.15a) is nothing but the linearized classical upside-down barrier equation of motion (8S/8x = 0) for the new coordinate x. Therefore, while x = 0 corresponds to the instanton, the nonzero solution to (4.15a) describes how the trajectory escapes from the instanton solution, when it deviates from it. The parameter X, referred to as the stability angle [Gutzwil-ler 1967 Rajaraman 1975], generalizes the harmonic-oscillator phase co, which would appear in (4.15), if CO, were a constant. The fact that X is real indicates the aforementioned instability of the instanton in two dimensions. Guessing that the determinant det( — -I- co, ) is a function of X only,... [Pg.63]

Errors in advection may completely overshadow diffusion. The amplification of random errors with each succeeding step causes numerical instability (or distortion). Higher-order differencing techniques are used to avoid this instability, but they may result in sharp gradients, which may cause negative concentrations to appear in the computations. Many of the numerical instability (distortion) problems can be overcome with a second-moment scheme (9) which advects the moments of the distributions instead of the pollutants alone. Six numerical techniques were investigated (10), including the second-moment scheme three were found that limited numerical distortion the second-moment, the cubic spline, and the chapeau function. [Pg.326]

The polymers which have stimulated the greatest interest are the polyacetylenes, poly-p-phenylene, poly(p-phenylene sulphide), polypyrrole and poly-1,6-heptadiyne. The mechanisms by which they function are not fully understood, and the materials available to date are still inferior, in terms of conductivity, to most metal conductors. If, however, the differences in density are taken into account, the polymers become comparable with some of the moderately conductive metals. Unfortunately, most of these polymers also have other disadvantages such as improcessability, poor mechanical strength, instability of the doped materials, sensitivity to oxygen, poor storage stability leading to a loss in conductivity, and poor stability in the presence of electrolytes. Whilst many industrial companies have been active in their development (including Allied, BSASF, IBM and Rohm and Haas,) they have to date remained as developmental products. For a further discussion see Chapter 31. [Pg.120]


See other pages where Functional instabilities is mentioned: [Pg.475]    [Pg.269]    [Pg.46]    [Pg.46]    [Pg.46]    [Pg.140]    [Pg.62]    [Pg.828]    [Pg.17]    [Pg.473]    [Pg.475]    [Pg.269]    [Pg.46]    [Pg.46]    [Pg.46]    [Pg.140]    [Pg.62]    [Pg.828]    [Pg.17]    [Pg.473]    [Pg.2612]    [Pg.43]    [Pg.274]    [Pg.590]    [Pg.604]    [Pg.771]    [Pg.24]    [Pg.241]    [Pg.288]    [Pg.294]    [Pg.120]    [Pg.668]    [Pg.84]    [Pg.196]    [Pg.384]    [Pg.601]    [Pg.2]    [Pg.15]   
See also in sourсe #XX -- [ Pg.828 ]




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