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Minimum of Energy

The situation becomes completely different when we ask for the energy to be an extremum at a given length. [Pg.97]

For two coupled springs T,ot (fi, fa) as a function of the energy of the springs under consideration, T is no longer a constant. If the other condition regarding the length remains still the same, the total length will be a constant. Therefore, we have the equations  [Pg.97]

For the first equation we want to find a minimum. The second equation in Eq. (2.51) is a constraint equation. We can easily insert the second equation of Eq. (2.51) in the first equation to obtain [Pg.97]

By substitution, we have now reduced the problem to a function of one variable, fi, find the extremum under the constraint, form the derivative as usual and obtain [Pg.98]

Therefore, the dimensionless elongation is = I2 = fwr/2. Eventually we from the second derivative which is d T,o,/dfi = 4. This indicates that basically only a minimum energy is possible. [Pg.98]


We carried out a second calculation for BeH at an internuclear distance of 2.67 a.u. corresponding to the minimum of energy.The mean magnetic susceptibility x obtained value, which is equal to -0,86.lO erg.G. mol V, agrees more closely to the value calculated by Fowler and Steiner [5], at the same internuclear distance,which is equal to -0.50 10 erg. G. mol F... [Pg.315]

The term H e is the electron correlation operator, the term H p corresponds to phonon-phonon interaction and H l corresponds to electron-phonon interaction. If we analyze the last term H l we see that when using crude approximation this corresponds to such phonons that force constant in eq. (17) is given as a second derivative of electron-nuclei interaction with respect to normal coordinates. Because we used crude adiabatic approximation in which minimum of the energy is at the point Rg, this is also reflected by basis set used. Therefore this approximation does not properly describes the physical vibrations i.e. if we move the nuclei, electrons are distributed according to the minimum of energy at point Rg and they do not feel correspondingly the R dependence. The perturbation term H) which corresponds to electron-phonon interaction is too large... [Pg.387]

Liposomes of different sizes can be prepared by extrusion, and when mixed with one another they remain stable in their given dimension, they do not equilibrate into one another. Why is this so How would you prove if there is one size that corresponds to the minimum of energy ... [Pg.213]

The line search algorithm outlined is parameter dependent. After much numerical experimentation, we choose a = 0.9 and p = 0.03, parameters which constitute a fairly weak line search. In our experience it is more effective to change search directions than to determine a more exact minimum of energy along a given search direction. In practice a is usually equal to unity. When a line search fails, however, the subsequent treatment of a can have a marked affect on the efficiency of the optimization. [Pg.250]

As can be seen in Figure 8 the maximum of energy corresponds to the conformation with the nitrogen atoms eclipsed, whereas the conformation rotated 180°, anti, corresponds to a minimum of energy. [Pg.313]

The least-squares method is a very powerful tool, provided the model is sufficiently close to the true structure. If the initial model is basically correct, the shifts in parameters indicated by the least-squares refinement will drive the energy of the structure to a global minimum. Unfortunately, if the model is not quite correct, the least-squares refinement will produce a structure that is trapped in a local minimum of energy which is not the true structure (see Figure 10.12). This problem manifests itself by monitoring the R value. Often there is a hint of trouble in that the R value is higher than expected and will not decrease to acceptable values. Several crystal structures have been reported with this type of problem, but they are generally corrected in the subsequent literature. [Pg.405]

Direct recycling is combined with a minimum of energy consumption, chemical waste, and lowest production costs. A general comparison of direct and indirect tungsten recycling is presented in Fig. 11.3. [Pg.381]

First, valence bonds of macromolecule break under irradiation effect and radicals are being formed, which further undergo dark elementary reaction. For hemolytic break of the bond it is necessary for photon to possess definite minimum of energy, which depends on the wave length of photon. [Pg.154]

Also, since we are considering infinitesimal vibrational amplitudes, the terms higher than quadratic can be neglected because qt qj qt qj qt-(This approximation will be inadequate when strong anharmonicities are present.) If we choose the minimum of energy, Fo °, as the arbitrary zero of our energy scale, the potential energy, within our approximation is ... [Pg.142]

There exists a universal functional for the energy of the fixed density, p(r). For a given external potential, the minimum of energy is the exact ground state energy that occurs for the exact ground state density, p(r). ... [Pg.120]

Energy calculations have complemented these stereochemical considerations and showed that in the case of bidentate squarate a minimum of energy is obtained if the configuration around the metal ion is close to tetrahedral, a situation that would be unusual for copper(ii). [Pg.367]


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1 energy minimum

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