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A relaxations

Ultrasonic absorption is used in the investigation of fast reactions in solution. If a system is at equilibrium and the equilibrium is disturbed in a very short time (of the order of 10"seconds) then it takes a finite time for the system to recover its equilibrium condition. This is called a relaxation process. When a system in solution is caused to relax using ultrasonics, the relaxation lime of the equilibrium can be related to the attenuation of the sound wave. Relaxation times of 10" to 10 seconds have been measured using this method and the rates of formation of many mono-, di-and tripositive metal complexes with a range of anions have been determined. [Pg.411]

It was determined, for example, that the surface tension of water relaxes to its equilibrium value with a relaxation time of 0.6 msec [104]. The oscillating jet method has been useful in studying the surface tension of surfactant solutions. Figure 11-21 illustrates the usual observation that at small times the jet appears to have the surface tension of pure water. The slowness in attaining the equilibrium value may partly be due to the times required for surfactant to diffuse to the surface and partly due to chemical rate processes at the interface. See Ref. 105 for similar studies with heptanoic acid and Ref. 106 for some anomalous effects. [Pg.34]

Since the development of grazing incidence x-ray diffraction, much of the convincing evidence for long-range positional order in layers has come from this technique. Structural relaxations from distorted hexagonal structure toward a relaxed array have been seen in heneicosanol [215]. Rice and co-workers combine grazing incidence x-ray diffraction with molecular dynamics simulations to understand several ordering transitions [178,215-219]. [Pg.135]

In the presence of some fomi of relaxation the equations of motion must be supplemented by a temi involving a relaxation superoperator—superoperator because it maps one operator into another operator. The literature on the correct fomi of such a superoperator is large, contradictory and incomplete. In brief, the extant theories can be divided into two kinds, those without memory relaxation (Markovian) Tp and those with memory... [Pg.233]

Figure Al.7.3. Schematic illustration showing side views of (a) a biilk-tenninated surface, (b) a relaxed surface with oscillatory behaviour, and (c) a reconstructed surface. Figure Al.7.3. Schematic illustration showing side views of (a) a biilk-tenninated surface, (b) a relaxed surface with oscillatory behaviour, and (c) a reconstructed surface.
Simultaneous application of an RF field at a frequency corresponding to the ++)<- +-) (i.e. 2<- l) transition then opens a relaxation path via T, and Pj or, more directly, via W p The extent to which these relaxation... [Pg.1570]

The atomic structure of a surface is usually not a simple tennination of the bulk structure. A classification exists based on the relation of surface to bulk stnicture. A bulk truncated surface has a structure identical to that of the bulk. A relaxed surface has the synnnetry of the bulk stnicture but different interatomic spacings. With respect to the first and second layers, lateral relaxation refers to shifts in layer registry and vertical relaxation refers to shifts in layer spacings. A reconstructed surface has a synnnetry different from that of the bulk synnnetry. The methods of stnictural analysis will be delineated below. [Pg.1813]

Here is a friction coefficient which is allowed to vary in time 2 is a thennal inertia parameter, which may be replaced by v.j., a relaxation rate for thennal fluctuations g 3Ais the number of degrees of freedom. [Pg.2261]

Point defects and complexes exliibit metastability when more than one configuration can be realized in a given charge state. For example, neutral interstitial hydrogen is metastable in many semiconductors one configuration has H at a relaxed bond-centred site, bound to the crystal, and the other has H atomic-like at the tetrahedral interstitial site. [Pg.2885]

However, most impurities and defects are Jalm-Teller unstable at high-symmetry sites or/and react covalently with the host crystal much more strongly than interstitial copper. The latter is obviously the case for substitutional impurities, but also for interstitials such as O (which sits at a relaxed, puckered bond-centred site in Si), H (which bridges a host atom-host atom bond in many semiconductors) or the self-interstitial (which often fonns more exotic stmctures such as the split-(l lO) configuration). Such point defects migrate by breaking and re-fonning bonds with their host, and phonons play an important role in such processes. [Pg.2888]

Figure 11. Perspective view [60] of a relaxed triangular plot [68] for the two DMBE adiabatic potential energy surfaces of H3 using hyperspherical coordinates. Figure 11. Perspective view [60] of a relaxed triangular plot [68] for the two DMBE adiabatic potential energy surfaces of H3 using hyperspherical coordinates.
In other words, the non-adiabatic coupling terms between P and Q states are all assumed to be zero. These requirements will later be reconsidered for a relaxed situation where these coupling terms are assumed to be not necessarily identically zero but small, that is, of the order s in regions of interest. [Pg.641]

Also in this case, Tp corresponds to a relaxation time which determines the coupling of the modulated variable to the external bath. The pressure scaling can be applied isotropically, whidi means that the factor is the same in all three spatial directions. More realistic is an anisotropic pressure scaling, because the box dimensions also change independently during the course of the simulation. [Pg.368]

Quantities with small relaxation times can thus be determined with greater statistical pre sion, as it will be possible to include a greater number of data sets from a given simulatii Moreover, no quantity with a relaxation time greater than the length of the simulation can determined accurately. [Pg.393]

CHAIN a relaxation method for obtaining reaction paths from semiempirical calculations... [Pg.361]

The tube is a construct which we might continue to sketch around an emerging chain as it diffuses out of the original sleeve. Instead, it is convenient to start with the tube initially in place and consider how long it takes for the molecule to escape. The initial entanglements which determine the contours of the tube comprise a set of constraints from which the molecule is relaxing, even if only to diffuse into another similar set. Accordingly, we identify this reptation time as a relaxation time r for the molecule. [Pg.120]

It is interesting to note that the Voigt model is useless to describe a relaxation experiment. In the latter a constant strain was introduced instantaneously. Only an infinite force could deform the viscous component of the Voigt model instantaneously. By constrast, the Maxwell model can be used to describe a creep experiment. Equation (3.56) is the fundamental differential equation of the Maxwell model. Applied to a creep experiment, da/dt = 0 and the equation becomes... [Pg.170]

The purpose of this problem is to consider numerically the effect of including more than two Maxwell elements in the model for a relaxation experiment. Prepare a table analogous to Table 3.2 for a set of four Maxwell elements having the following properties ... [Pg.194]

The relaxatioa temperature appears to iacrease with increa sing HFP coateat. Relaxatioa iavolves 5—13 of the chaia carboa atoms. Besides a and y relaxations, one other dielectric relaxation was observed below —150° C, which did not vary ia temperature or ia magnitude with comonomer content or copolymer density (55). The a relaxation (also called Glass 1) is a high temperature transition (157°C) andy relaxation (Glass 11) (internal friction maxima) occurs between —5 and 29°C. [Pg.359]

Fig. 4. Laboratory tubing model for supercoiling in closed-circular DNA (a) relaxed DNA, ALK = 0 (b) ALK = ATw -... Fig. 4. Laboratory tubing model for supercoiling in closed-circular DNA (a) relaxed DNA, ALK = 0 (b) ALK = ATw -...
The standard conventional finishing process has been modified to suit the purposes for different fabrics and garments. Eor example, tubular knits are frequently handled using specialized equipment to control tension and to get adequate padding. Some tubular knits are subjected to wet-on-wet padding, dried and cured in large dmm dryers, and steam-treated to achieve a relaxed and nondistorted knit. [Pg.442]

A finite time is required to reestabUsh the ion atmosphere at any new location. Thus the ion atmosphere produces a drag on the ions in motion and restricts their freedom of movement. This is termed a relaxation effect. When a negative ion moves under the influence of an electric field, it travels against the flow of positive ions and solvent moving in the opposite direction. This is termed an electrophoretic effect. The Debye-Huckel theory combines both effects to calculate the behavior of electrolytes. The theory predicts the behavior of dilute (<0.05 molal) solutions but does not portray accurately the behavior of concentrated solutions found in practical batteries. [Pg.509]

The precise mechanism of nitrate action is not cleady understood and may be a combination of many factors. The basic pharmacologic action of nitrates is a relaxation of most vascular smooth muscle, eg, vascular, bronchial, gastrointestinal, uretal, uterine, etc. Vascular smooth muscle relaxation is a... [Pg.122]

In this expression. Ait is the size of the integration time step, Xj is a characteristic relaxation time, and T is the instantaneous temperature. In the simulation of water, they found a relaxation time of Xj = 0.4 ps to be appropriate. However, this method does not correspond exactly to the canonical ensemble. [Pg.58]

At short times, there is a relaxation of the reactant and product state populations to their equilibrium values. For example, the deviation from the equilibrium concentration of products is given by... [Pg.201]


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Misfit strain relaxation due to a viscous underlayer

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Relaxation a and

Relaxation as a function of frequency

Relaxation of a Single Conserved Variable

Relaxation of a localized vibrational mode

Relaxation of a prepared state

Relaxation of a quantum harmonic oscillator

Relaxation of magnetization after a pulse

Resonant excitation of a two-level system free from relaxation

Resonant excitation of a two-level system with relaxations

Segmental a-relaxation process

Spin Relaxation and Local Motion in a Dissolved Aromatic Polyformal

Spin-Lattice Relaxation of a Rouse Chain

Stress relaxation after a step strain

Stress relaxation as a measure of chemical degradation

Stress relaxation as thermally activated process

Structural a-Relaxation Dynamic Structure Factor

Temperature of the a relaxation

The a-relaxation

The influence of a constant and thermally activated relaxation rate

Thermally activated reorientations and tunnel relaxation of orientational states in a phonon field

Use of Botulinum Toxin as a Muscle Relaxant

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