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Statistical Mechanics Approach

The language of Statistical Mechanics evolved over a considerable period of time. For example, the term ensemble is used to denote a statistical population of molecules partition function is the integral, over phase-space of a system, of the exponential of -E/kT [where E is the energy of the system, k is Boltzmann s eonstant, and T is the temperature in °K]. From this function , all of the thermodynamic functions can be derived. The definitions that we shall need are given as follows in 2.5.1. on the next page. [Pg.65]

Using these, we can derive the following equation for the total energy of any given system  [Pg.66]

In these equations, r is a so-called partition coefficient , co is a degeneracy, k is Boltzsmann s constant, and T is in degrees Kelvin. The first equation in 2.5.3. is a statistical mechanical definition of work, whereas the last two describe total energy states. Having these definitions and equations allows us to define point defects firom a Statistical Mechanical viewpoint. [Pg.66]

Consider a plane net having N sites, of which Nl are lattice sites, Nv are vacancies, andNi are Interstitials. (Note that we do not consider charge at the sites for the moment). Using these, we have the following two equations  [Pg.66]

E)quation 2.5.4. holds if some fraction of Ni is associated with Nl, the number of lattice sites, i.e.- Frenkel defects. According to the Binomial Theorem, we can combine pairs of these sites as  [Pg.67]


Another statistical mechanical approach makes use of the radial distribution function g(r), which gives the probability of finding a molecule at a distance r from a given one. This function may be obtained experimentally from x-ray or neutron scattering on a liquid or from computer simulation or statistical mechanical theories for model potential energies [56]. Kirkwood and Buff [38] showed that for a given potential function, U(r)... [Pg.62]

The statistical mechanical approach, density functional theory, allows description of the solid-liquid interface based on knowledge of the liquid properties [60, 61], This approach has been applied to the solid-liquid interface for hard spheres where experimental data on colloidal suspensions and theory [62] both indicate 0.6 this... [Pg.62]

The non-consen>ed variable (.t,0 is a broken symmetry variable, it is the instantaneous position of the Gibbs surface, and it is the translational synnnetry in z direction that is broken by the inlioinogeneity due to the liquid-vapour interface. In a more microscopic statistical mechanical approach 121, it is related to the number density fluctuation 3p(x,z,t) as... [Pg.727]

It will be noted that these various limitations cannot be removed merely by adopting a statistical-mechanical approach rather than the original BET treatment. [Pg.49]

Peng XF, Tien Y, Lee DJ (2001) Bubble nucleation in micro-channels statistical mechanics approach. Int J Multiphase Flow 44 2953-2964... [Pg.463]

Ab initio molecular orbital calculations are being used to study the reactions of anionic nucleophiles with carbonyl compounds in the gas phase. A rich variety of energy surfaces is found as shown here for reactions of hydroxide ion with methyl formate and formaldehyde, chloride ion with formyl and acetyl chloride, and fluoride ion with formyl fluoride. Extension of these investigations to determine the influence of solvation on the energy profiles is also underway the statistical mechanics approach is outlined and illustrated by results from Monte Carlo simulations for the addition of hydroxide ion to formaldehyde in water. [Pg.200]

Note that we can use the same statistical mechanical approach to calculate SchottslQi" pairs, Frenkel pairs, divancies (which are associated vacancies), impurity-vacancy complexes, and line dislocation-point defect complexes. [Pg.127]

Michael W. Deem, A Statistical Mechanical Approach to Combinatorial Chemistry Venkat Ganesan and Glenn H. Fredrickson, Fluctuation Effects in Microemulsion Reaction Media... [Pg.233]

We have introduced a statistical mechanical approach, illustrating how the material properties and rheology play a role at the microscopic level. Our main reason for doing this is to determine the microstructure and calculate the macroscopic rheological properties. We can now evaluate the coordination number z from Equation (5.30) for our colloid pair potential in Figure 5.9. The variation of z with volume fraction is shown in Figure 5.10. [Pg.164]

Various treatments of these effects have been developed over a period of years. The conductance equations of Fuoss and Onsager l, based on a model of a sphere moving through a continuum, are widely used to interpret conductance data. Similar treatments n 3, as well as more rigorous statistical mechanical approaches 38>, will not be discussed here. For a comparison of these treatments see Ref. 11-38) and 39>. The Fuoss-Onsager equations are derived in Ref.36), and subsequently modified slightly by Fuoss, Onsager and Skinner in Ref. °). The forms in which these equations are commonly expressed are... [Pg.12]

Transition state theory, a quasi-thermodynamic/statistical mechanical approach to the theory of reaction rates was developed in the early 1930s by a number of workers including H. Eyring, E. R Wigner, and J. C. Polanyi and was very quickly applied to the consideration of isotope effects on rates of simple molecular reactions. [Pg.33]

Parallel with the phenomenological development, an alternative point of view has developed toward thermodynamics, a statistical-mechanical approach. Its philosophy is more axiomatic and deductive than phenomenological. The kinetic theory of gases naturally led to attempts to derive equations describing the behavior of matter in bulk from the laws of mechanics (first classic, then quanmm) applied to molecular particles. As the number of molecules is so great, a detailed treatment of the mechanical problem presents insurmountable mathematical difficulties, and statistical methods are used to derive average properties of the assembly of molecules and of the system as a whole. [Pg.528]

The situation is entirely different when a molecular or a statistical mechanical approach is adopted. In molecular terms the three intrinsic binding constants are... [Pg.332]

In 1985 I was glad to see T. L. Hill s volume entitled Cooperativity Theory in Biochemistry, Steady State and Equilibrium Systems. This was the first book to systematically develop the molecular or statistical mechanical approach to binding systems. Hill demonstrated how and why the molecular approach is so advantageous relative to the prevalent phenomenological approach of that time. On page 58 he wrote the following (my italics) ... [Pg.358]

The statistical mechanical approach starts from more fundamental ingredients, namely, the molecular properties of all the molecules involved in the binding process. The central quantity of this approach is the partition function (PF) for the entire macroscopic system. In particular, for binding systems in which the adsorbent molecules are independent, the partition function may be expressed as a product of partition functions, each pertaining to a single adsorbent molecule. The latter function has the general form... [Pg.359]

Thermodynamics cannot provide the extension to the BP for nonideal systems (with respect to either the ligands or the adsorbent molecules). The statistical mechanical approach can, in principle, provide corrections for the nonideality of the system. An example is worked out in Appendix D. [Pg.359]

In general, the statistical mechanical approach may also be appUed to systems where the adsorbent molecules are not necessarily independent. However, in this book we shall always assume independence of the adsorbent molecules. [Pg.359]

While there are several books that deal with the subject matter of this volume, the only one that develops the statistical mechanical approach is T. L. Hill s monograph (1985), which includes equilibrium as well as nonequilibrium aspects of cooperativity. Its style is quite condensed, formal, and not always easy to read. The emphasis is on the effect of cooperativity on the form of the PF and on the derived binding isotherm (BI). Less attention is paid to the sources of cooperativity and to the mechanism of communication between ligands, which is the main subject of the present volume. [Pg.361]

Michael W. Deem, A Statistical Mechanical Approach to Combinatorial Chemistry... [Pg.186]

An alternate form of the rate constant predicted by transition state theory using a statistical mechanical approach for the equilibrium constant K is Eq. (R) ... [Pg.140]

Recent developments in the theory of polymer solutions have been reviewed by Berry and Casassa (32), and by Casassa (71). Casassa, who has contributed very largely to these developments, has adopted a statistical mechanical approach using molecular distribution functions, as first outlined by Zimm (72), rather than using a lattice model like that used by Flory, Huggins, and many later workers. [Pg.19]

Relation of Electrostatic and Statistical-Mechanical Approaches to Interionic Theory. We believe that the ionic cloud concept is appropriate for the... [Pg.219]

Attempts to interpret the mechanism of ethylene hydrogenation over nickel [96—99] and over platinum catalysts [100,101] in terms of a statistical mechanical approach have not met with any substantial success, partly due to the limitations of the model which must be assumed in order to perform the calculations and partly due to the complexity of the calculations themselves. [Pg.27]

The Marcus treatment uses a classical statistical mechanical approach to calculate the activation energy required to surmount the barrier. It assumes a weakly adiabatic electron transfer process and non-equilibrium dielectric polarization of the solvent (continuum) as the source of activation. This model also considers the vibrational contributions of the inner solvation sphere. The Hush treatment considers ion-dipole and ligand field concepts in the treatment of inner coordination sphere contributions to the energy of activation [55, 56]. [Pg.54]

Eyring s theory is well explained in textbooks on kinetics. It is analogous to the statistical mechanics approach that gives the probability of a particle with total energy H = p2/2mA + 0( ,) to be found in the interval to ( +d ) and p to ip + dp), that is,... [Pg.102]

Many authors7-21 have theoretically investigated the conformation of an isolated adsorbed polymer as a function of adsorption energy, using statistical mechanical approaches. Some important conclusions are as follows ... [Pg.5]

In order to improve MD simulations, a number of specific areas should be addressed in the area of basic molecular dynamics theory. These include (1) development of full quantum mechanical calculations on complex molecules and more robust ways to incorporate quantum mechanical calculations within larger-scale classical mechanics or statistical mechanics approaches (2) development and refinement of transferable force fields between arbitrary atoms and molecules, which are necessary building blocks for MD simulations of general systems and (3) development of multiscale theories and techniques for understanding systems. Moreover, the community must develop toolkits that allow general users to perform such simulations. [Pg.204]

Gelman, N. and Machin, J. (1994). Diffusion through the water barrier of arthropod cuticles A statistical mechanical approach to the analysis of temperature effects. [Pg.116]

Fig.12. Computation by Monte Carlo methods of the first four order parameters of an ensemble of 1000 chromophores (of dipole moment 13 Debye) existing in a medium of uniform dielectric constant. At the beginning of the calculation, the chromophores are randomly ordered thus, ==O. During the first 400 Monte Carlo steps, an electric poling field (600 V/micron) is on but the chromophore number density (=10 7 molecules/cc) is so small that intermolecular electrostatic interactions are unimportant. The order parameters quickly evolve to well-known equilibrium values obtained analytically from statistical mechanics (black dots in figure also see text). During steps 400-800 the chromophore number density is increased to 5xl020 and intermolecular electrostatic interactions act to decrease order parameters consistent with the results of equilibrium statistical mechanical calculations discussed in the text. Although Monte Carlo and equilibrium statistical mechanical approaches described in the text are based on different approximations and mathematical methods, they lead to the same result (i.e., are in quantitative agreement)... Fig.12. Computation by Monte Carlo methods of the first four order parameters of an ensemble of 1000 chromophores (of dipole moment 13 Debye) existing in a medium of uniform dielectric constant. At the beginning of the calculation, the chromophores are randomly ordered thus, <cos9>=<cos30>=O. During the first 400 Monte Carlo steps, an electric poling field (600 V/micron) is on but the chromophore number density (=10 7 molecules/cc) is so small that intermolecular electrostatic interactions are unimportant. The order parameters quickly evolve to well-known equilibrium values obtained analytically from statistical mechanics (black dots in figure also see text). During steps 400-800 the chromophore number density is increased to 5xl020 and intermolecular electrostatic interactions act to decrease order parameters consistent with the results of equilibrium statistical mechanical calculations discussed in the text. Although Monte Carlo and equilibrium statistical mechanical approaches described in the text are based on different approximations and mathematical methods, they lead to the same result (i.e., are in quantitative agreement)...
The statistical mechanics approaches to genetic algorithm dynamics can be applied to the newly developed technique of sexual PCR, in which nucleotide sequences can be recombined at multiple sites [153,154],... [Pg.148]


See other pages where Statistical Mechanics Approach is mentioned: [Pg.660]    [Pg.2815]    [Pg.411]    [Pg.139]    [Pg.301]    [Pg.414]    [Pg.265]    [Pg.265]    [Pg.279]    [Pg.158]    [Pg.221]    [Pg.587]    [Pg.411]    [Pg.38]    [Pg.75]    [Pg.234]    [Pg.241]    [Pg.142]    [Pg.86]   


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