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Free energy minima

The free energy minimum is found by differentiating equation (A2.5.18) with respect to s at constant Tand setting the derivative equal to zero. In its simplest fonn the resultant equation is... [Pg.632]

For any given protein, the number of possible conformations that it could adopt is astronomical. Yet each protein folds into a unique stmcture totally deterrnined by its sequence. The basic assumption is that the protein is at a free energy minimum however, calometric studies have shown that a native protein is more stable than its unfolded state by only 20—80 kj/mol (5—20 kcal/mol) (5). This small difference can be accounted for by the favorable... [Pg.209]

If the polymer system was able to exist in an equilibrium state only, then a strictly defined correlation between (a, ph) and (a, ph) would exist in particular conditions, according to minimum of free energy of system formation. Consequently, there would occur only one temperature at which process initiation is thermodynamically probable. In rare ca.ses there may occur different correlations between ( ph, a) and ( ph, a ), which display one and the same value of free energy minimum of system formation. [Pg.366]

The thermodynamic analysis of conformational and structural transformations in the melt at high pressures34 showed that the free volume and free energy minimum required for hydrostatic compression is attained as a result of the transition of the molecules in the melt into a more extended conformation (gauche —> trans transitions) since the extended molecules ensure a more compact packing of the chains at compression. Chain uncoiling leads to a decrease in their flexibility parameter f with increasing pressure p ... [Pg.217]

The transition state, on the other hand, is a species that reacts without further activation. It cannot be diverted to an alternative product, nor will it succumb to trapping. An intermediate, at a free-energy minimum, is both preceded and followed by a transition state. Both of the transition states lie at free-energy maxima. [Pg.127]

Let A = yc, , 1 < / < Nc, be conformations generated for C using a computational method. Because the global free energy minimum conformation is expected to statistically dominate the thermodynamic ensemble, the predicted binding activity for C is determined by (C)=min F y. ) = F(yf ). [Pg.336]

A (either a transition state or a free energy minimum) reacts to form B. In hydrogenation, R in C is an alkyl group formed by reaction of H with adsorbed olefin and the mechanism is not Horiuti-Polanyi-like. Rather reaction via both A and C are among the few relatively clear examples of Rideal-Eley processes. [Pg.66]

The above analysis applies to those situations where the pairwise interaction curve is characterised by a free energy minimum (figure 7). If charges are present, then contributions... [Pg.18]

It is now instructive to ask why the achiral calamitic SmC a (or SmC) is not antiferroelectric. Cladis and Brand propose a possible ferroelectric state of such a phase in which the tails on both sides of the core tilt in the same direction, with the cores along the layer normal. Empirically this type of conformational ferroelectric minimum on the free-energy hypersurface does not exist in known calamitic LCs. Another type of ferroelectric structure deriving from the SmCA is indicated in Figure 8.13. Suppose the calamitic molecules in the phase were able to bend in the middle to a collective free-energy minimum structure with C2v symmetry. In this ferroelectric state the polar axis is in the plane of the page. [Pg.479]

An equivalent method was used by Kitaigorodski and Ahmed (11) to predict the equilibrium habit of anthracene. Starting from a nucleus of just one molecule, the growth was simulated by adding one molecule at a time at positions such that the free energy minimum condition was always satisfied. A simple 6-exp two-parameter potential function was used to estimate... [Pg.57]

The critical nucleus corresponds to p = 1 = m, and the global free-energy minimum corresponds to infinitely large dimensions of the cylinder in both length and radius. [Pg.20]

It is this property that was used by Zel dovich [22] to prove the uniqueness of the equilibrium specified as a point of the free energy minimum. [Pg.124]


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See also in sourсe #XX -- [ Pg.144 ]

See also in sourсe #XX -- [ Pg.50 ]

See also in sourсe #XX -- [ Pg.216 ]




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1 energy minimum

Crystal minimum Gibbs free energy

Local free energy minimum

Minimum free energy paths

Minimum free energy principle

Minimum value of the free energy

Minimum, in free energy

Thermodynamic minimum free-energy

Thermodynamic minimum free-energy point

Thermodynamic minimum free-energy state

Thermodynamic minimum free-energy temperature

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