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Stokes-Einstein

This result is often called the Stokes-Einstein formula for the difflision of a Brownian particle, and the Stokes law friction coefficient 6iiq is used for... [Pg.689]

In the Smoluchowski limit, one usually assumes that the Stokes-Einstein relation (Dq//r7)a = C holds, which fonns the basis of taking the solvent viscosity as a measure for the zero-frequency friction coefficient appearing in Kramers expressions. Here C is a constant whose exact value depends on the type of boundary conditions used in deriving Stokes law. It follows that the diffiision coefficient ratio is given by ... [Pg.850]

The relation between the microscopic friction acting on a molecule during its motion in a solvent enviromnent and macroscopic bulk solvent viscosity is a key problem affecting the rates of many reactions in condensed phase. The sequence of steps leading from friction to diflfiision coefficient to viscosity is based on the general validity of the Stokes-Einstein relation and the concept of describing friction by hydrodynamic as opposed to microscopic models involving local solvent structure. In the hydrodynamic limit the effect of solvent friction on, for example, rotational relaxation times of a solute molecule is [ ]... [Pg.853]

Figure 5 relates N j to collection efficiency particle diffusivity from Stokes-Einstein equation assumes Brownian motion same order of magnitude or greater than mean free path of gas molecules (0.1 pm at... [Pg.392]

Supercritical Mixtures Dehenedetti-Reid showed that conven-tionaf correlations based on the Stokes-Einstein relation (for hquid phase) tend to overpredict diffusivities in the supercritical state. Nevertheless, they observed that the Stokes-Einstein group D g l/T was constant. Thus, although no general correlation ap es, only one data point is necessaiy to examine variations of fluid viscosity and/or temperature effects. They explored certain combinations of aromatic solids in SFg and COg. [Pg.595]

StoKes-Einstein and Free-Volume Theories The starting point for many correlations is the Stokes-Einstein equation. This equation is derived from continuum fluid mechanics and classical thermodynamics for the motion of large spherical particles in a liqmd. [Pg.596]

For this case, the need for a molecular theory is cleverly avoided. The Stokes-Einstein equation is (Bird et al.)... [Pg.596]

Wilke-Chang This correlation for D°b is one of the most widely used, and it is an empirical modification of the Stokes-Einstein equation. It is not very accurate, however, for water as the solute. Otherwise, it apphes to diffusion of very dilute A in B. The average absolute error for 251 different systems is about 10 percent. ( )b is an association factor of solvent B that accounts for hydrogen bonding. [Pg.596]

The Stokes-Einstein equation has already been presented. It was noted that its vahdity was restricted to large solutes, such as spherical macromolecules and particles in a continuum solvent. The equation has also been found to predict accurately the diffusion coefficient of spherical latex particles and globular proteins. Corrections to Stokes-Einstein for molecules approximating spheroids is given by Tanford. Since solute-solute interactions are ignored in this theory, it applies in the dilute range only. [Pg.598]

In connection with the earlier consideration of diffusion in liquids using tire Stokes-Einstein equation, it can be concluded that the temperature dependence of the diffusion coefficient on the temperature should be T(exp(—Qvis/RT)) according to this equation, if the activation energy for viscous flow is included. [Pg.295]

Using the Stokes-Einstein equation for the viscosity, which is unexpectedly useful for a range of liquids as an approximate relation between diffusion and viscosity, explains a resulting empirical expression for the rate of formation of nuclei of the critical size for metals... [Pg.300]

By equating Fiek s seeond law and the Stokes-Einstein equation for diffusivity, Smoluehowski (1916,1917) showed that the eollision frequeney faetor takes the form... [Pg.170]

Very commonly Eq. (4-5) is combined with Eq. (4-6), the Stokes-Einstein equation relating the diffusion coefficient to the viscosity -q. [Pg.135]

Equations (4-5) and (4-7) are alternative expressions for the estimation of the diffusion-limited rate constant, but these equations are not equivalent, because Eq. (4-7) includes the assumption that the Stokes-Einstein equation is applicable. Olea and Thomas" measured the kinetics of quenching of pyrene fluorescence in several solvents and also measured diffusion coefficients. The diffusion coefficients did not vary as t) [as predicted by Eq. (4-6)], but roughly as Tf. Thus Eq. (4-7) is not valid, in this system, whereas Eq. (4-5), used with the experimentally measured diffusion coefficients, gave reasonable agreement with measured rate constants. [Pg.136]

Following the general trend of looldng for a molecular description of the properties of matter, self-diffusion in liquids has become a key quantity for interpretation and modeling of transport in liquids [5]. Self-diffusion coefficients can be combined with other data, such as viscosities, electrical conductivities, densities, etc., in order to evaluate and improve solvodynamic models such as the Stokes-Einstein type [6-9]. From temperature-dependent measurements, activation energies can be calculated by the Arrhenius or the Vogel-Tamman-Fulcher equation (VTF), in order to evaluate models that treat the diffusion process similarly to diffusion in the solid state with jump or hole models [1, 2, 7]. [Pg.164]

T0 is a reference temperature which can be identified with T, and although the constant B is not related to any simple activation process, it has dimensions of energy. This form of the equation is derived by assuming an electrolyte to be fully dissociated in the solvent, so it can be related to the diffusion coefficient through the Stokes-Einstein equation. It suggests that thermal motion above T0 contributes to relaxation and transport processes and that... [Pg.507]

The same equation applies to other solvents. It is often easier to incorporate an expression for the diffusion coefficient than a numerical value, which may not be available. According to the Stokes-Einstein equation,6 diffusion coefficients can be estimated from the solvent viscosity by... [Pg.200]

To = temperature of the solvent at which tan A goes through a maximum. These values are presented in Table II. VSE (the Stokes-Eeinstein volume) is calculated for a spherical molecule if the molecule is aspherical this calculation (VSE) is called Vapparent The Vapparent can be smaller or larger than the Stokes-Einstein volume and varies from the equivalent sphere volume obtained by solution of equations 3,4 and 5. [Pg.191]

Table II. Comparison of Stokes-Einstein (Vapparent) Volume to the Perrin Volume... Table II. Comparison of Stokes-Einstein (Vapparent) Volume to the Perrin Volume...
Using the Stokes-Einstein equation of diffusion coefficient ... [Pg.98]

According to Stokes-Einstein equation, the diffusion coefficient is inversely proportional to the solution viscosity which increases with temperature. Hence, a lower diffusion coefficient corresponds to a lower size molecule. [Pg.109]

The Stokes-Einstein equation can be successfully used to explain diffusion under the following conditions [401], where (a) the diffusing molecule is large with respect to the molecules defining the medium, (b) the medium has a very low viscosity, and (c) no solute-solvent interactions occur. [Pg.580]

Thus, the Stokes-Einstein equation is expected to be valid for colloidal particles and suspensions of large spherical particles. Experimental evidence supports these assumptions [101], and this equation has occasionally been used for much smaller species. [Pg.580]

The Stokes-Einstein equation predicts that DfxITa is independent of the solvent however, for real solutions, it has long been known that the product of limiting interdiffusion coefficient for solutes and the solvent viscosity decreases with increasing solute molar volume [401]. Based upon a large number of experimental results, Wilke and Chang [437] proposed a semiempirical equation,... [Pg.580]

Perrin model and the Johansson and Elvingston model fall above the experimental data. Also shown in this figure is the prediction from the Stokes-Einstein-Smoluchowski expression, whereby the Stokes-Einstein expression is modified with the inclusion of the Ein-stein-Smoluchowski expression for the effect of solute on viscosity. Penke et al. [290] found that the Mackie-Meares equation fit the water diffusion data however, upon consideration of water interactions with the polymer gel, through measurements of longitudinal relaxation, adsorption interactions incorporated within the volume averaging theory also well described the experimental results. The volume averaging theory had the advantage that it could describe the effect of Bis on the relaxation within the same framework as the description of the diffusion coefficient. [Pg.584]

Dunning, JW Angus, JC, Particle-Size Measurement by Doppler-Shifted Laser Light, a Test of the Stokes-Einstein Relation, Journal of Applied Physics 39, 2479, 1968. [Pg.611]

Since thermal agitation is the common origin of transport properties, it gives rise to several relationships among them, for example, the Nemst-Einstein relation between diffusion and conductivity, or the Stokes-Einstein relation between diffusion and viscosity. Although transport... [Pg.120]


See other pages where Stokes-Einstein is mentioned: [Pg.511]    [Pg.932]    [Pg.133]    [Pg.31]    [Pg.548]    [Pg.598]    [Pg.1511]    [Pg.294]    [Pg.294]    [Pg.892]    [Pg.238]    [Pg.617]    [Pg.56]    [Pg.191]    [Pg.191]    [Pg.208]    [Pg.580]   
See also in sourсe #XX -- [ Pg.73 , Pg.79 , Pg.112 , Pg.170 , Pg.175 , Pg.346 , Pg.347 ]

See also in sourсe #XX -- [ Pg.73 , Pg.79 , Pg.112 , Pg.170 , Pg.175 , Pg.346 , Pg.347 ]

See also in sourсe #XX -- [ Pg.141 ]

See also in sourсe #XX -- [ Pg.147 ]




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Breakdown of Stokes-Einstein

Brownian dynamics Stokes-Einstein relation

Brownian motion Stokes-Einstein theory

Coefficients) Stokes-Einstein

Debye-Stokes Einstein relationship

Diffusion Stokes-Einstein

Diffusion Stokes-Einstein equation

Diffusion Stokes-Einstein relation

Diffusion coefficients Stokes-Einstein equation

Diffusion coefficients Stokes-Einstein expression

Diffusivity liquids, Stokes-Einstein

Einstein-Stokes relationship

Equation Stokes-Einstein

Ionic liquids Stokes-Einstein equation

Ionic liquids Stokes-Einstein relation

Mean-square displacement Stokes-Einstein relation

Smoluchowski/Stokes-Einstein expression

Stokes-Einstein Equation for Dilute Solutions

Stokes-Einstein and Free-Volume Theories

Stokes-Einstein behavior

Stokes-Einstein coefficient diffusion

Stokes-Einstein equation Brownian diffusion coefficient

Stokes-Einstein equation correlation

Stokes-Einstein equation dynamics

Stokes-Einstein equation for diffusion

Stokes-Einstein equation generalized

Stokes-Einstein equation ionicity

Stokes-Einstein equation modifications

Stokes-Einstein equation particle

Stokes-Einstein equation relations

Stokes-Einstein equation size-dependent diffusion

Stokes-Einstein equation translational

Stokes-Einstein equation variables

Stokes-Einstein formula

Stokes-Einstein friction

Stokes-Einstein hydrodynamic radius

Stokes-Einstein model

Stokes-Einstein product

Stokes-Einstein radius, effect

Stokes-Einstein relation

Stokes-Einstein relation breakdown

Stokes-Einstein relation effects

Stokes-Einstein relation formula

Stokes-Einstein relation tested

Stokes-Einstein relationship hydrodynamic radius

Stokes-Einstein volume

Stokes-Einstein-Debye equation

Stokes-Einstein-Debye model

Stokes—Einstein correlation, ionic liquids

Stokes—Einstein law

Stokes—Einstein theory

The Stokes-Einstein Relation

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