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The Insertion Mode

The central point in the scheme is the non-uniform distribution of the non-crystallizable units in the primary stack, being higher in the thinner and lower in the thicker amorphous layers. The necessary prerequisite for this is a suppression of any transport of non-crystallizable units through the crystallites, so that the difference in concentrations is maintained and an equilibration prevented. For branched polyethylene this condition is obviously fulfilled, which appears reasonable considering the size of the short-chain branches. [Pg.210]


In cases where a block of sugar irnits is transferred it is usually inserted at the nonreducing end of the polymer, which may be covalently attached to a protein. Notice that the insertion mode of chain growth exists for lipids, polysaccharides, and proteins. [Pg.995]

Markownikoff s rule is frequently applied to this problem, and one of the insertion modes is designated as Markownikoff mode, and the other as anti-Markowni-koff mode. There is, however some confusion in the literature as to which is which. [Pg.108]

The hydroformylation of propylene provides two types of products, n- and isobutyraldehydes depending on the insertion modes of propylene into the M-H bond. As shown in Scheme 1.18a and b, where R = H, the anti-Markovnikov type addition of M-H to the double bond in (a) gives the linear propyl, whereas the Markovnikov type addition gives the isopropyl group bound with the metal. Further insertion of CO yields the linear and branched acyl groups. [Pg.22]

A major difference between the emulsion and solution SBR materials is the relative ratio of the insertion modes and geometric isomers derived from butadiene [6], which makes... [Pg.411]

It is a general phenomenon in polymers that, after completion of the primary crystallization at the first fixed temperature, crystallization does not come to an end but continues upon further cooling. The temperature range where crystallization occurs and, consequently, also the range of melting during a subsequent heating are always broad. There are two different processes which can contribute to this secondary crystallization , the insertion mode and the surface crystallization , and they will be discussed in Sect. 4.3. [Pg.158]

Surface crystallization and melting being the exception, the insertion mode is the rule and is indeed mainly responsible for the generally observed secondary crystallization. As it does not require a mobile crystalline phase, it can always occur. [Pg.188]

Open the Aspen user interface and then click on the Pressure Changes tab on the model library and select compressor. Click anywhere in the process flow sheet area. Click on Material Streams in the model library and connect inlet and exit stream lines. Click on the arrow on the left of the model library to cancel the insert mode. Click on Component on the toolbar, and select methane, ethane, COj, and Nj. [Pg.92]

Figure A3.13.12. Evolution of the probability for a right-handed ehiral stmetnre (fiill eiirve, see ( equation (A3,13.69))) of the CH eliromophore in CHD2T (a) and CHDT2 ( ) after preparation of ehiral stnietures with multiphoton laser exeitation, as diseussed in the text (see also [154]). For eomparison, the time evolution of aeeording to a one-dimensional model ineluding only the bending mode (dashed enrve) is also shown. The left-hand side insert shows the time evolution of within the one-dimensional ealeulations for a longer time interval the right-hand insert shows the time evolution within the tln-ee-dimensional ealeulation for the same time interval (see text). Figure A3.13.12. Evolution of the probability for a right-handed ehiral stmetnre (fiill eiirve, see ( equation (A3,13.69))) of the CH eliromophore in CHD2T (a) and CHDT2 ( ) after preparation of ehiral stnietures with multiphoton laser exeitation, as diseussed in the text (see also [154]). For eomparison, the time evolution of aeeording to a one-dimensional model ineluding only the bending mode (dashed enrve) is also shown. The left-hand side insert shows the time evolution of within the one-dimensional ealeulations for a longer time interval the right-hand insert shows the time evolution within the tln-ee-dimensional ealeulation for the same time interval (see text).
Silaallene 73"" was synthesized in an manner analogous to that of 70. Compound 73 was stable at room temperature over I month, but in the presence of any protic source (i.e., water, methanol), it underwent a rearrangement different than that observed for 70, inserting into a methyl C—H bond (74) on the octamethylfluorenyl moiety rather than into one of the groups on silicon (Eq. (6)). It is believed that the favored mode of rearrangement for these groups is that of silaallene 73, but 70... [Pg.21]

In the early 1990s Raman spectroscopy was applied to the characterization of TS-1 catalysts [55,56]. In such experiments, beside the 960 cm band, already observed by IR spectroscopy (see Sect. 3.5), a new component at 1125 cm was detected by Scarano et al. [55] (see Fig. 2f). The 1125 cm band was recognized to be a fingerprint of the insertion of Ti atoms in the ze-olitic framework [55]. This band could not be observed in the IR studies as totally overshadowed by an extremely intense band around 1000 cm due to Si02 framework modes (Fig. 2e). [Pg.46]

Figure 26. Constant current mode STM image of isolated (A), self-organized in close-packed hexagonal network (C) and in fee structure (E) of silver nanoclusters deposited on Au(l 11) substrate (scan size (A) 17.1 x 17.1 nm, f/t=—IV, /t=ltiA, (C) 136 X 136 nm, f/t = — 2.5 V, /t = 0.8 tiA, (E) 143 x 143 nm, = —2.2 V, /, = 0.72 nA). I U) curves and their derivatives in the inserts of isolated (B), self-organized in close-packed hexagonal network (D) and in fee structure (F) of silver nanoclusters deposited on Au(l 11) substrate. (Reprinted with permission from Ref. [58], 2000, Wiley-VCH.)... Figure 26. Constant current mode STM image of isolated (A), self-organized in close-packed hexagonal network (C) and in fee structure (E) of silver nanoclusters deposited on Au(l 11) substrate (scan size (A) 17.1 x 17.1 nm, f/t=—IV, /t=ltiA, (C) 136 X 136 nm, f/t = — 2.5 V, /t = 0.8 tiA, (E) 143 x 143 nm, = —2.2 V, /, = 0.72 nA). I U) curves and their derivatives in the inserts of isolated (B), self-organized in close-packed hexagonal network (D) and in fee structure (F) of silver nanoclusters deposited on Au(l 11) substrate. (Reprinted with permission from Ref. [58], 2000, Wiley-VCH.)...
Potential differences between the nitrobenzene and aqueous phases at the interfaces in the presence [Fig. 2(B)] and absence of surfactant (C) were measured simultaneously. KCl salt bridges were inserted into the octanol phase to monitor potential. Oscillation measurement data across the nitrobenzene membrane are given in Fig. 2(A) for comparison. The oscillation mode in Fig. 2(C) is virtually the same as that in (A) with respect to oscillatory period and amplitude but quite different with that in (B). Although the potential across the nitrobenzene membrane (A) was not recorded simultaneously with that between nitrobenzene-water phases (B) and (C) but successively, it was noted that the algebraic sum of (B) and (C) should be essentially the same as (A). This is an indication that potential oscillation across the nitrobenzene membrane is likely generated at the interface between the nitrobenzene phase and aqueous phase initially containing no surfactant. [Pg.699]


See other pages where The Insertion Mode is mentioned: [Pg.646]    [Pg.165]    [Pg.646]    [Pg.320]    [Pg.181]    [Pg.14]    [Pg.207]    [Pg.208]    [Pg.853]    [Pg.646]    [Pg.165]    [Pg.646]    [Pg.320]    [Pg.181]    [Pg.14]    [Pg.207]    [Pg.208]    [Pg.853]    [Pg.1560]    [Pg.2528]    [Pg.181]    [Pg.342]    [Pg.235]    [Pg.86]    [Pg.92]    [Pg.107]    [Pg.29]    [Pg.48]    [Pg.199]    [Pg.204]    [Pg.30]    [Pg.348]    [Pg.176]    [Pg.558]    [Pg.145]    [Pg.52]    [Pg.566]    [Pg.567]    [Pg.310]    [Pg.701]    [Pg.129]    [Pg.465]    [Pg.271]    [Pg.353]    [Pg.37]   


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Insertion modes

The mode

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