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Rigidity dynamic

Routh, E. J. Advanced Rigid Dynamics (Macmillan, London, 1884). [Pg.730]

Rigidity, high T dimensional stability Rigidity, dynamic toughness Impact, temp, resistance Rigidity, chemical resistance, dynamic toughness... [Pg.651]

Impact, high-temperature rigidity Rigidity, dynamic toughness... [Pg.651]

In comparison, statherin is a multi-functional protein, which inhibits the primary and secondary precipitation of hydroxyapatite in saliva, as well as serving as a boundary lubricant [37]. On the basis of the NMR T p measurements of the N-terminal 15-amino acid peptide in statherin, Drobny et al. proposed that the binding region in the N-terminus has rigid dynamics. [Pg.184]

The fuel hose jacket compound is a HVA-2/Tetrone A cured compound for adhesion to the tie layer and fabric. It is a less expensive formulation as it does not have to meet the rigid dynamic properties of a power steering hose and is exposed to only occasional oil spills. [Pg.337]

In Dynamic Spatial Reconstructor at the expense of use 2D matrix of detectors there was the opportunity to use a divergent cone beam of source emission. This system had a number of lacks. In particular the number of projections is rigidly limited by the number of x-ray sources. The dispersion of source emission results in errors of data collected.. However the system confirmed basic advantages of application of conic beams and 2D matrices of detectors for collecting information about 3D object. [Pg.217]

The paper discusses the application of dynamic indentation method and apparatus for the evaluation of viscoelastic properties of polymeric materials. The three-element model of viscoelastic material has been used to calculate the rigidity and the viscosity. Using a measurements of the indentation as a function of a current velocity change on impact with the material under test, the contact force and the displacement diagrams as a function of time are plotted. Experimental results of the testing of polyvinyl chloride cable coating by dynamic indentation method and data of the static tensile test are presented. [Pg.239]

Ciccotti G, Ferrario M and Ryckaert J-P 1982 Molecular dynamics of rigid systems in cartesian coordinates. A general formulation Mol. Phys. 47 1253-64... [Pg.2281]

Ciccotti G and Ryckaert J P 1986 Molecular dynamics simulation of rigid molecules Comput. Phys. Rep. 4 345-92... [Pg.2281]

Figure C3.5.8. Computed frequency-dependent friction (inverseiy proportionai to tire VER iifetime T ) from a ciassicai moiecuiar dynamics simuiation of rigid Hgl moiecuies in etiianoi soiution, from [90]. The Hgl vibrationai... Figure C3.5.8. Computed frequency-dependent friction (inverseiy proportionai to tire VER iifetime T ) from a ciassicai moiecuiar dynamics simuiation of rigid Hgl moiecuies in etiianoi soiution, from [90]. The Hgl vibrationai...
An interesting approach has recently been chosen in the MBO(N)D program ([Moldyn 1997]). Structural elements of different size varying from individual peptide planes up to protein domains can be defined to be rigid. During an atomistic molecular dynamics simulation, all fast motion orthogonal to the lowest normal modes is removed. This allows use of ca. 20 times longer time steps than in standard simulations. [Pg.73]

Hayward et al. 1994] Hayward, S., Kitao, A., Go, N. Harmonic and anharmonic aspects in the dynamics of BPTI A normal mode analysis and principal component analysis. Prot. Sci. 3 (1994) 936-943 [Head-Gordon and Brooks 1991] Head-Gordon, T., Brooks, C.L. Virtual rigid body dynamics. Biopol. 31 (1991) 77-100... [Pg.76]

The key to these more efficient treatments is a natural canonical formulation of the rigid body dynamics in terms of rotation matrices. The orientational term of the Lagrangian in these variables can be written simply as... [Pg.352]

Ihe allure of methods for calculating free energies and their associated thermod)mai values such as equilibrium constants has resulted in considerable interest in free ene calculations. A number of decisions must be made about the way that the calculatior performed. One obvious choice concerns the simulation method. In principle, eit Monte Carlo or molecular dynamics can be used in practice, molecular dynamics almost always used for systems where there is a significant degree of conformatio flexibility, whereas Monte Carlo can give very good results for small molecules which either rigid or have limited conformational freedom. [Pg.593]

Treating the full internal nuclear-motion dynamics of a polyatomic molecule is complicated. It is conventional to examine the rotational movement of a hypothetical "rigid" molecule as well as the vibrational motion of a non-rotating molecule, and to then treat the rotation-vibration couplings using perturbation theory. [Pg.342]

Consider a quantity of some liquid, say, a drop of water, that is composed of N individual molecules. To describe the geometry of this system if we assume the molecules are rigid, each molecule must be described by six numbers three to give its position and three to describe its rotational orientation. This 6N-dimensional space is called phase space. Dynamical calculations must additionally maintain a list of velocities. [Pg.12]

Khludneva E.Yu. (1990b) Contact of a nonelastic plate with a rigid punch. In Dynamics of Continuum Media. Novosibirsk (98), 67-79 (in Russian). [Pg.380]

Microfilaments and Microtubules. There are two important classes of fibers found in the cytoplasm of many plant and animal ceUs that are characterized by nematic-like organization. These are the microfilaments and microtubules which play a central role in the determination of ceU shape, either as the dynamic element in the contractile mechanism or as the basic cytoskeleton. Microfilaments are proteinaceous bundles having diameters of 6—10 nm that are chemically similar to actin and myosin muscle ceUs. Microtubules also are formed from globular elements, but consist of hoUow tubes that are about 30 nm in diameter, uniform, and highly rigid. Both of these assemblages are found beneath the ceU membrane in a linear organization that is similar to the nematic Hquid crystal stmcture. [Pg.202]

Laurion, U.S. Pat. No. 3,847,443, discloses an oma-mental wheel element which is designed to fit between the spokes, inside a wheel. Strazis, U.S. Pat. No. 4,682,821, discloses a semi-rigid, tension attached bicycle wheel cover assembly intended to improve the aero-dynamic efficiency of bicycle wheels. Monte, U.S. Pat. [Pg.28]


See other pages where Rigidity dynamic is mentioned: [Pg.415]    [Pg.575]    [Pg.248]    [Pg.158]    [Pg.80]    [Pg.415]    [Pg.575]    [Pg.248]    [Pg.158]    [Pg.80]    [Pg.240]    [Pg.595]    [Pg.1515]    [Pg.2312]    [Pg.2725]    [Pg.3044]    [Pg.22]    [Pg.24]    [Pg.132]    [Pg.140]    [Pg.246]    [Pg.349]    [Pg.349]    [Pg.352]    [Pg.357]    [Pg.384]    [Pg.390]    [Pg.406]    [Pg.468]    [Pg.680]    [Pg.166]    [Pg.177]    [Pg.328]    [Pg.109]    [Pg.413]    [Pg.465]   
See also in sourсe #XX -- [ Pg.327 , Pg.336 , Pg.344 ]




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