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Constant temperature/energy

A very important thermodynamic relationship is that giving the effect of surface curvature on the molar free energy of a substance. This is perhaps best understood in terms of the pressure drop AP across an interface, as given by Young and Laplace in Eq. II-7. From thermodynamics, the effect of a change in mechanical pressure at constant temperature on the molar h ee energy of a substance is... [Pg.53]

At constant temperature and pressure a small change in the surface free energy of the system shown in Fig. IV-1 is given by the total differential... [Pg.104]

For an ideal gas and a diathemiic piston, the condition of constant energy means constant temperature. The reverse change can then be carried out simply by relaxing the adiabatic constraint on the external walls and innnersing the system in a themiostatic bath. More generally tlie initial state and the final state may be at different temperatures so that one may have to have a series of temperature baths to ensure that the entire series of steps is reversible. [Pg.338]

Thus, for spontaneous processes at constant temperature and volume a new quantity, the Helmholtz free energy A, decreases. At equilibrium under such restrictions cL4 = 0. [Pg.346]

For spontaneous processes at constant temperature and pressure it is the Gibbs free energy G that decreases, while at equilibrium under such conditions dG = 0. [Pg.347]

In many experiments the sample is in thennodynamic equilibrium, held at constant temperature and pressure, and various properties are measured. For such experiments, the T-P ensemble is the appropriate description. In this case the system has fixed and shares energy and volume with the reservoir E = E + E" and V=V + V", i.e. the system... [Pg.417]

Figure A2.5.7. Constant temperature isothenns of reduced Helmlioltz free energy A versus reduced volume V. The two-phase region is defined by the line simultaneously tangent to two points on the curve. The dashed parts of the smooth curve are metastable one-phase extensions while the dotted curves are unstable regions. (The isothenns are calculated for an unphysical r = 0.1, the only effect of which is to separate the isothenns... Figure A2.5.7. Constant temperature isothenns of reduced Helmlioltz free energy A versus reduced volume V. The two-phase region is defined by the line simultaneously tangent to two points on the curve. The dashed parts of the smooth curve are metastable one-phase extensions while the dotted curves are unstable regions. (The isothenns are calculated for an unphysical r = 0.1, the only effect of which is to separate the isothenns...
This type of calorimeter is nomrally enclosed in a themiostatted-jacket having a constant temperature T(s). and the calorimeter (vessel) temperature T(c) changes tln-ough the energy released as the process under study proceeds. The themial conductivity of the intemiediate space must be as small as possible. Most combustion calorimeters fall into this group. [Pg.1903]

There are tln-ee general approaches to conducting MD at constant temperature rather than constant energy. [Pg.2261]

The equilibrium constant at constant temperature is directly related to the maximum energy, called the free energy AG. which is obtainable from a reaction, the relationship being... [Pg.66]

For free dynam ics wdierc the constant temperature check box in the Molecular Dynam ics dialog box is not checked, the total energy K l OT should remain constant,, A fhictuation of the total... [Pg.320]

The canonical ensemble is the name given to an ensemble for constant temperature, number of particles and volume. For our purposes Jf can be considered the same as the total energy, (p r ), which equals the sum of the kinetic energy (jT(p )) of the system, which depends upon the momenta of the particles, and the potential energy (T (r )), which depends upon tlie positions. The factor N arises from the indistinguishability of the particles and the factor is required to ensure that the partition function is equal to the quantum mechanical result for a particle in a box. A short discussion of some of the key results of statistical mechanics is provided in Appendix 6.1 and further details can be found in standard textbooks. [Pg.319]

Just as one may wish to specify the temperature in a molecular dynamics simulation, so may be desired to maintain the system at a constant pressure. This enables the behavior of the system to be explored as a function of the pressure, enabling one to study phenomer such as the onset of pressure-induced phase transitions. Many experimental measuremen are made under conditions of constant temperature and pressure, and so simulations in tl isothermal-isobaric ensemble are most directly relevant to experimental data. Certai structural rearrangements may be achieved more easily in an isobaric simulation than i a simulation at constant volume. Constant pressure conditions may also be importai when the number of particles in the system changes (as in some of the test particle methoc for calculating free energies and chemical potentials see Section 8.9). [Pg.401]

Alternatively, authors have repeatedly invoked the internal pressure of water as an explanation of the rate enhancements of Diels-Alder reactions in this solvent ". They were probably inspired by the well known large effects of the external pressure " on rates of cycloadditions. However, the internal pressure of water is very low and offers no valid explanation for its effect on the Diels-Alder reaction. The internal pressure is defined as the energy required to bring about an infinitesimal change in the volume of the solvents at constant temperature pi = (r)E / Due to the open and... [Pg.20]

These calculations can incorporate various types of constraints. It is most common to run simulations with a hxed number of atoms and a hxed volume. In this case, the temperature can be computed from the average kinetic energy of the atoms. It is also possible to adjust the volume to maintain a constant pressure or to scale the velocities to maintain a constant temperature. [Pg.304]

If there is no external temperature control (using a simulated constant temperature bath), molecular dynamics simulations are constant energy. [Pg.77]

To some extent you can monitor constant temperature simulations by the temperature (TEMP) and its deviation (D TEMP) or by kinetic energy (EKIN) and its deviation (D EKIN). Plot these values using the HyperChem Molecular Averages dialog box. [Pg.87]

For constant temperature dynamics where the constant temperature check box in the Molecular Dynamics Options dialog box is checked, the energy will not remain constant but will fluctuate as energy is exchanged with the bath. The temperature, depending on the value set for the relaxation constant, will approach con-stan cy. [Pg.321]

In considering the differential energy of adsorption, it is useful to picture an experimental procedure which allows the adsorption to proceed at constant temperature and in infinitely small stages. Then... [Pg.14]

Thus by measuring the small amount of heat 5Q which is evolved when the adsorption increases by the small amount 6n mole at constant temperature, the differential molar energy of adsorption can be evaluated calorimetri-... [Pg.15]

Chemical systems spontaneously react in a fashion that lowers their overall free energy. At a constant temperature and pressure, typical of many bench-top chemical reactions, the free energy of a chemical reaction is given by the Gibb s free energy function... [Pg.137]


See other pages where Constant temperature/energy is mentioned: [Pg.111]    [Pg.111]    [Pg.111]    [Pg.111]    [Pg.90]    [Pg.93]    [Pg.618]    [Pg.813]    [Pg.2241]    [Pg.367]    [Pg.75]    [Pg.77]    [Pg.94]    [Pg.161]    [Pg.400]    [Pg.469]    [Pg.579]    [Pg.61]    [Pg.75]    [Pg.77]    [Pg.94]    [Pg.94]    [Pg.161]    [Pg.316]    [Pg.317]    [Pg.330]   
See also in sourсe #XX -- [ Pg.77 ]




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