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Properties dynamic

Micelles of low molecular weight surfactants are known to be very dynamic structures, although the various fragments of the molecules within a micelle are subject to some restrictions of mobility in comparison to molecular solution [23, 379-381]. As the hydrophilic head groups are anchored at the micellar surface , NMR-studies show that the mobility and the order parameter decreases along the alkyl tail from its end towards the head group [379-385]. [Pg.40]

The restricted mobilities of the hydrophobic segments and the dynamic profile are also reflected in the shape of NMR-spectra of vinylic polysoaps in aqueous solution. The signals of protons in the proximity of the polymer backbone are strongly broadened [193, 258, 303, 355] or virtually invisible [39, 227] (Fig. 31). This effect decreases with decreasing density of the hydrophobic tails [193, 303, 355, 357] and with decreasing molecular weight. [Pg.40]

The problem of restricted mobility not only concerns the various fragments of the polysoap itself, but the mobility of solubilized material is affected as well ( microviscosity ). Studying the motion of the ESR-spin probe, polysoaps [Pg.40]

It has been demonstrated that polymers can exhibit fluid as weU as solid behavior. The viscous fluid behavior of polymers becomes evident under dynamic loading where the viscous damping property reduces the amplitude of free vibrations. It is also observed that the strain will lag the stress and that there can be an energy loss through heat dissipation during periodic loading. [Pg.40]

It is part of our common experience that a plastic beaker, when struck, emits a dull note of short duration, which is quite different from the ringing note emitted by a bell or a crystal wine glass. This property of high mechanical damping is another manifestation of viscoelasticity. It is a property that is frequently of value, for instance in shock absorbers. In plastic structures subject to forced oscillation, mechanical vibrations at the natural frequencies of the structure do not easily build up, due to the high [Pg.128]

We describe next the characteristics, or parameters, used to quantify dynamic viscoelastic properties and introduce briefly some of the methods of measurement The close relationship between the (tynamic parameters (for which the variable is frequenty) and the parameters from step-function experiments (with time as variable) is described later. [Pg.129]

Suppose an oscillatory shear strain of angular frequenty , [Pg.129]

4n Vector representation of an alternating stress leading an alternating strain by phase angle S. [Pg.129]

The relationship between stress and strain in this fynamic case be defined by writing [Pg.130]


Methfessel M, Rodriguez C O and Andersen O K 1989 Fast full-potential calculations with a converged basis of atom-centered linear muffIn-tIn orbitals structural and dynamic properties of silicon Phys. Rev. B 40 2009-12... [Pg.2232]

Molecular dynamics consists of the brute-force solution of Newton s equations of motion. It is necessary to encode in the program the potential energy and force law of interaction between molecules the equations of motion are solved numerically, by finite difference techniques. The system evolution corresponds closely to what happens in real life and allows us to calculate dynamical properties, as well as thennodynamic and structural fiinctions. For a range of molecular models, packaged routines are available, either connnercially or tlirough the academic conmuinity. [Pg.2241]

Also we must bear in mind that the advancement of the coordinates fidfds two fiinctions (i) accurate calculation of dynamical properties, especially over times as long as typical correlation times x (ii) accurately staying on the constant-energy hypersurface, for much longer times Exact time reversibility is highly desirable (since the original equations... [Pg.2250]

Mbiler-Krumbhaar H and Binder K 1973 Dynamic properties of the Monte-Carlo method in statistical mechanics J. Stat. Phys. 8 1-24... [Pg.2279]

The complexity of polymeric systems make tire development of an analytical model to predict tlieir stmctural and dynamical properties difficult. Therefore, numerical computer simulations of polymers are widely used to bridge tire gap between tire tlieoretical concepts and the experimental results. Computer simulations can also help tire prediction of material properties and provide detailed insights into tire behaviour of polymer systems. A simulation is based on two elements a more or less detailed model of tire polymer and a related force field which allows tire calculation of tire energy and tire motion of tire system using molecular mechanisms, molecular dynamics, or Monte Carlo teclmiques 1631. [Pg.2537]

For the mechanistic studies made, this protocol is able to give information about how dynamical properties affect the evolution of a photochemical reaction, but is not accurate enough for quantitative results. The information obtained relates to aspects of the surface such as the relative steepness of regions on the lower slopes of the conical intersection, and the relative width of alternative channels. [Pg.302]

Teleman, O. An efficient way to conserve the total energy in molecular dynamics simulations boundary effects on energy conservation and dynamic properties. Mol. Simul. 1 (1988) 345-355. [Pg.31]

Cao, J., Voth, G.A. The formulation of quantum statistical mechanics based on the Feynman path centroid density. I. Equilibrium properties. J. Chem. Phys. 100 (1994) 5093-5105 II Dynamical properties. J. Chem. Phys. 100 (1994) 5106-5117 III. Phase space formalism and nalysis of centroid molecular dynamics. J. Chem. Phys. 101 (1994) 6157-6167 IV. Algorithms for centroid molecular dynamics. J. Chem. Phys. 101 (1994) 6168-6183 V. Quantum instantaneous normal mode theory of liquids. J. Chem. Phys. 101 (1994) 6184 6192. [Pg.34]

Among the main theoretical methods of investigation of the dynamic properties of macromolecules are molecular dynamics (MD) simulations and harmonic analysis. MD simulation is a technique in which the classical equation of motion for all atoms of a molecule is integrated over a finite period of time. Harmonic analysis is a direct way of analyzing vibrational motions. Harmonicity of the potential function is a basic assumption in the normal mode approximation used in harmonic analysis. This is known to be inadequate in the case of biological macromolecules, such as proteins, because anharmonic effects, which MD has shown to be important in protein motion, are neglected [1, 2, 3]. [Pg.332]

There are many algorithms for integrating the equations of motion using finite difference methods, several of which are commonly used in molecular dynamics calculations. All algorithms assume that the positions and dynamic properties (velocities, accelerations, etc.) can be approximated as Taylor series expansions ... [Pg.369]

Focuses on force field calculations for understanding the dynamic properties of proteins and nucleic acids. Provides a useful introduction to several computational techniques, including molecular mechanics minimization and molecular dynamics. Includes discussions of research involving structural changes and short time scale dynamics of these biomolecules, and the influence of solvent in these processes. [Pg.4]

If the Bath relaxation constant, t, is greater than O.I ps, you should be able to calculate dynamic properties, like time correlation functions and diffusion constants, from data in the SNP and/or CSV files (see Collecting Averages from Simulations on page 85). [Pg.72]

The temperature of a simulation depends on your objectives. You might use high temperatures to search for additional conformations of a molecule (see Quenched Dynamics on page 78). Room temperature simulations generally provide dynamic properties of molecules such as proteins, peptides, and small drug molecules. Low temperatures (<250 K) often promote a molecule to a lower energy conformation than you could obtain by geometry optimization alone. [Pg.90]

D. R. Cmise, Theoretical Computation of Equilibrium Composition, Thermal Dynamic Properties, and Peformance Characteristics of Propellants Systems, NWC... [Pg.53]

A. T. Chen, and co-workers, "Comparison of the Dynamic Properties of Polyurethane Elastomers Based on Low Unsaturation Polyoxypropylene Glycols and Poly(tetramethylene oxide) Glycols," Polyurethanes World Congress 1993, Vancouver, B.C., Canada, Oct. 10—13,1993. [Pg.356]

Chloroprene Elastomers. Polychloroprene is a polymer of 2-chloro-l,3-butadiene. The elastomer is largely composed of the trans isomer. There are two basic polymer types the W-type and the G-type. G-types are made by using a sulfur-modified process W-types use no sulfur modification. As a result, G-types possess excellent processing and dynamic properties, and tend to be used in V-belts. However, they have poorer aging properties than W-types. The W-types tend to be used in appHcations requiring better aging, such as roUs and mechanical goods (see Elastomers, SYNTHETIC-POLYCm.OROPRENE). [Pg.233]

Dynamic properties are measured by continuous cycles of varying deformation (strain) and/or stress (force required to secure a given strain), at varying frequencies which can be set close to those a component would experience in a tire. These properties are more correlative to many tire performance parameters. [Pg.251]

In general, however, the vulcanizates suffer from poor low temperature crystallization performance compared to a conventional sulfur cure, and also have inferior tensile and tear properties. Urethane cross-linking systems (37), eg, Novor 950 (see Table 3) are also extremely heat resistant, but exhibit inferior tensile and dynamic properties compared to conventional sulfur-cured vulcanizates. One added virtue is that they can be used in conjunction with sulfur systems to produce an exceUent compromise according to the ratios used (38). [Pg.269]

Mamzen Oil Co. has developed various Ziegler-Natta catalysts that can produce poly(butadiene-i //-prop5iene) (PBR) (78). PBR shows tack (self-adhesion) and green (unvulcanized) dynamic properties superior to those of BR and EPDM. Carbon black-loaded vulcanizates can be compounded to give high strength and elongation at break (79,80). PBR can also be covulcanized with SBR, BR, and EPDM. [Pg.185]

A. E. Hirsch and R. J. Boyce, Dynamic Properties of EthjlenefMcrylic Elastomers M New Heat Resistant Rubber Bulletin EA-530.604, Du Pont Polymers, Stow, Ohio, May 1977. [Pg.501]

Two elastomers have been commercialized with unique property profiles. One has fluoroalkoxy substituents that provide resistance to many fluids, especially to hydrocarbons. This material also has a broad use temperature range and useful dynamic properties. Aryloxy substituents provide flame retardant materials without halogens. [Pg.525]


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