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Chain crystals

The effect of different types of comonomers on varies. VDC—MA copolymers mote closely obey Flory s melting-point depression theory than do copolymers with VC or AN. Studies have shown that, for the copolymers of VDC with MA, Flory s theory needs modification to include both lamella thickness and surface free energy (69). The VDC—VC and VDC—AN copolymers typically have severe composition drift, therefore most of the comonomer units do not belong to crystallizing chains. Hence, they neither enter the crystal as defects nor cause lamellar thickness to decrease, so the depression of the melting temperature is less than expected. [Pg.431]

Fig. 31 Trajectories of seven crystallizing chains (thick lines) selected at random from 640 chains during crystallization at 330 K a at 0.128 ns, b at 6.4 ns, c at 12.8 ns, and d at 19.2 ns. Also shown are the growing crystalline domains (thin parallel lines). Pictures are all side view along the x-axis... Fig. 31 Trajectories of seven crystallizing chains (thick lines) selected at random from 640 chains during crystallization at 330 K a at 0.128 ns, b at 6.4 ns, c at 12.8 ns, and d at 19.2 ns. Also shown are the growing crystalline domains (thin parallel lines). Pictures are all side view along the x-axis...
The end-to-end vector r of any non-crystallized chain portion comprising n skeletal bonds with a length l will be taken as Gaussian-distributed, i.e.,... [Pg.127]

Figure 2.46 Model of packing of conformationally disordered chains of sPP in disordered modifications of form II presenting kink bands.189,190 Chains drawn with thick and thin fines are at 0 and 0.5 along b. In the ordered portion of crystal chains are in ordered twofold (T2G2)B helical conformation, whereas in the defective portion (delimited by dashed lines) chains are in T2G2T6 conformation. Figure 2.46 Model of packing of conformationally disordered chains of sPP in disordered modifications of form II presenting kink bands.189,190 Chains drawn with thick and thin fines are at 0 and 0.5 along b. In the ordered portion of crystal chains are in ordered twofold (T2G2)B helical conformation, whereas in the defective portion (delimited by dashed lines) chains are in T2G2T6 conformation.
Many semicrystalline polymers are polymorphic and exist in different crystal forms. When PBT fiber is uniaxially stretched [75], the contracted gauche-trans-gauche a-crystal chain is extended to a fully trans conformation of a y-crystal. Above 20% strain, the crystal form is 100% y-crystal with a longer c-axis triclinic cell dimension. Thus, it is reasonable to ask whether the... [Pg.381]

AMI calculations on dimers of nitroanilines are of interest in investigating the inter-molecular forces which orientate the individual molecules in crystal chains. Dimerization in solid crystal may be considered responsible for the differences in molecular geometry between solid and gas phases97. [Pg.435]

The. folded-chain lamella theory arose in the last 1950s when polymer single crystals in the form of thin platelets termed lamella, measuring about 10,000 A x 100 A, were grown from polymer solutions. Contrary to previous expectations, X-ray diffraction patterns showed the polymer chain axes to be parallel to the smaller dimension of the platelet. Since polymer molecules are much longer than 100 A, the polymer molecules are presumed to fold back and forth on themselves in an accordionlike manner in the process of crystallization. Chain... [Pg.24]

If the growth front is frozen, the crystallization at the growth front depends crucially on the commensurability between the thickness of the growth front and the length of crystallizing chains. For details, see Ref. 49. A collection of polydisperse chains gets effectively fractionated at the growth front. [Pg.55]

Thus, they are in rather close contact with each other. In crystals chains of hydrogen-bonded atoms may be formed. In phosphatidylethanolamine the phosphate and -NH3+ ions may alternate in these chains.132... [Pg.396]

The crystal structure of I strongly resembles the relaxed crystal dimer structure (B). In the case of II, structure IIB would require a bend in the crystal chain that might be very difficult to accommodate. [Pg.466]

AMI calculations on the dimers of nitroanilines and substituted benzoic acids are of considerable value in predicting their crystal structures. In particular, the intermolecular forces that dictate the relative orientations of the individual molecules in the crystal chains can be understood. It is likely that this methodology will be useful for modelling the kinds of interactions that might occur in other crystals. [Pg.470]

Conditions required to generate A- and B-type crystal conformations are reasonably well-understood. Under cool, wet conditions (such as in a potato tuber), B-type starch crystals form, while in warmer, drier conditions (e.g. in a cereal grain), the A allomorph is preferred. Chain length also affects the selection of crystal form, chains of DP <10 do not crystallize, chains with a DP from 10 to 12 tend to form A-type crystals, and chains with a DP >12 tend to yield the B form.37,38 This is likely the result of differences in loss of entropy on crystallization experienced by chains of different lengths.39 An irreversible transition from B-type starch to A-type starch can be accomplished under conditions of low humidity and high temperature. This so-called... [Pg.157]

The answer is very simple. Putting aside crystal chains which terminate at the interface (only significantly available in low molecular weight material) there are two possibilities (fig. 2). [Pg.201]

Philpotts A. R., Shi J., and Brustman C. (1998) Role of plagioclase crystal chains in the differentiation of partly crystallized basaltic magma. Nature 395, 343-346. [Pg.1455]

Figure 4.10 shows a plot of He as a function of f for different PE and paraffin samples crystallized from the melt. The calculated continuous curve was derived using b = 20 nm. The deviation of the experimental data from the calculated curve is due to the wide range of b values obtained (b = 6-26 nm), corresponding to the widely different structures examined (CEPE crystals, chain-folded lamellae, low-density (LD) PE and linear paraffins). Comparison of experimental and calculated He data for PE emphasizes the parallel increase in the b parameter derived from mechanical data (14-26 nm) and in determined thermodynamically (79-91 mJ m ) for a series of samples with different molecular weights (56000-307000) (Balta Calleja et al, 1990b) (see also Section 4.3). [Pg.95]

Figure 15. Aggregated nanoparticles of titania forming a single-crystal chain, an example of oriented aggregation. From Penn and Barrfield (1999) with permission from Elsevier, pubhshers of... Figure 15. Aggregated nanoparticles of titania forming a single-crystal chain, an example of oriented aggregation. From Penn and Barrfield (1999) with permission from Elsevier, pubhshers of...
Figure 51. A series of fluctuations at the crystal growth face. The squares represent crystallized chain segments, (a) Steps allowed in the Frank-Tosi model,226 (b and c) some other possible steps (after ref 4). Figure 51. A series of fluctuations at the crystal growth face. The squares represent crystallized chain segments, (a) Steps allowed in the Frank-Tosi model,226 (b and c) some other possible steps (after ref 4).
Keywords Block copolymers, Crystallization, Chain folding... [Pg.113]


See other pages where Chain crystals is mentioned: [Pg.237]    [Pg.72]    [Pg.78]    [Pg.124]    [Pg.256]    [Pg.69]    [Pg.158]    [Pg.464]    [Pg.33]    [Pg.73]    [Pg.126]    [Pg.259]    [Pg.105]    [Pg.133]    [Pg.28]    [Pg.610]    [Pg.202]    [Pg.719]    [Pg.82]    [Pg.136]    [Pg.42]    [Pg.126]    [Pg.58]    [Pg.487]    [Pg.26]   
See also in sourсe #XX -- [ Pg.232 ]




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Actual chain conformations and crystal structures

Chain branching, polyethylene crystal structure

Chain crystallization

Chain crystallization

Chain entropy, polymer crystal nucleation

Chain folding in crystallization

Chain folding structure, single crystals

Chain growth, polymer crystal nucleation

Chain-folded crystallization

Chain-folded crystals

Chain-folded lamellar crystals

Chain-folded single crystal

Chain-folded single crystal morphology

Chains crystallization from dilute solution

Chiral thermotropic liquid crystal main chain

Chiral thermotropic liquid crystal side chain

Conformation of Polymer Chains in Crystals and Conformational Polymorphism

Conformation of Single Chains in Crystals

Crystal chain disorder

Crystal chain-folding principle

Crystal growth chain folding

Crystal growth periodic bond chains

Crystal lamella chain folding

Crystal lattices chains

Crystal polymorphism, methylene chain

Crystal structure Chain

Crystal structure chain direction repeat

Crystal structure, fats double chain

Crystal structures chain folded

Crystal, defect, point extended-chain

Crystallinity extended-chain crystals

Crystallization chain folding

Crystallization from dilute solution flexible chains

Crystallization of Much Longer Chains from the Melt

Crystallization single-chain behavior

Diffraction Structures and Chain Packing in the Crystal

Extended Chain Crystallization

Extended chain-type crystal

Extended-chain crystals

Folded chain-type crystal

Globular-chain crystal

Lamellae single crystals, chain folding

Lamellar single crystals, chain organization

Laterally-attached side chain liquid crystal polymers

Liquid crystals main-chain

Liquid crystals side-chain packing

Lyotropic main-chain liquid crystal

Lyotropic main-chain liquid crystal order

Lyotropic main-chain liquid crystal polymers

Lyotropic side-chain polymer liquid crystals

Main chain liquid crystal polymers MCLCP)

Main-chain polymer liquid crystal

Many chain crystals

Network chains crystallization

Non-periodic crystallization from a side-chain bearing copolyester

Of thermotropic main chain polymer liquid crystals

Parallel-chain crystal

Periodic bond chain models, crystal

Phase behaviour of lyotropic side chain polymer liquid crystals

Polyethylene extended-chain crystals

Polymer crystals chain-direction moduli

Polymer single crystals chain folds

Polymer thermotropic main-chain liquid crystal

Polymers, chain type spherulitic crystal, growth

Polyoxymethylene extended-chain crystals

Polysiloxane side-chain liquid crystal optical

Polytetrafluoroethylene extended-chain crystals

Rod-Like Liquid Crystals Combining RH- and RF-Chains Monolayer Smectic Phases

Rod-Like Liquid Crystals with Fluorinated Chains

Rod-Like Liquid Crystals with Two Fluorinated Chains at Opposite Ends Layer Frustration

Segmented-chain polymer liquid crystals

Side Chain Polymeric Liquid Crystals

Side-Chain Thermotropic Liquid Crystal Polymers

Side-chain Crystallization in Poly(n-octadecylmethacrylate)

Side-chain crystallization

Side-chain liquid crystal polymers

Side-chain liquid crystal polymers SCLCPs)

Side-chain liquid crystals

Side-chain polymer liquid crystals structural considerations

Single chain crystal

Single chain models, polymer crystal nucleation

Single crystals chain folding

Static Displacements of Chains Against Crystal Lattices

Synthesis of lyotropic side chain polymer liquid crystals

Three-Dimensional Crystallization of a Single Chain from Vapor

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