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Constant Temperature and Pressure

However, it is common practice to sample an isothermal isobaric ensemble NPT, constant pressure and constant temperature), which normally reflects standard laboratory conditions well. Similarly to temperature control, the system is coupled to an external bath with the desired target pressure Pq. By rescaling the dimensions of the periodic box and the atomic coordinates by the factor // at each integration step At according to Eq. (46), the volume of the box and the forces of the solvent molecules acting on the box walls are adjusted. [Pg.368]

Although constrained dynamics is usually discussed in the context of the geometrically constrained system described above, the same techniques can have many other applications. For instance, constant-pressure and constant-temperature dynamics can be imposed by using constraint methods [33,34]. Car and Parrinello [35] describe the use of the extended Lagrangian to maintain constraints in the context of their ab initio MD method. (For more details on the Car-Parrinello method, refer to the excellent review by Gain and Pasquarrello [36].)... [Pg.63]

Compare the product of pressure and volume at different pressures and constant temperature. [Pg.109]

The relationship obtained finally as above implies that when precipitation is implemented at a constant H2 pressure and constant temperature, then log [Cu2+] and the pH of the solution bear linear functional relationship at the point of equilibrium, and the slope of this straight line corresponds to 2. [Pg.542]

Berger, O., Edholm, O. and Jahnig F. (1997). Molecular dynamics simulations of a fluid bilayer of dipalmitoylphosphatidylcholine at full hydration, constant pressure and constant temperature, Biophys. J., 72, 2002-2013. [Pg.105]

From the ideal gas law, the molar mass of the gas is proportional to the volume of the gas under constant pressure and constant temperature, therefore, by use of Equation 13.6,... [Pg.292]

At constant total pressure and constant temperature, uB and ulb, should also be constant, since they depend only on the structure and state of the solid, unlike //A which depends on environment. [Pg.95]

Gibbs free energy Energy liberated or absorbed in a reversible process at constant pressure and constant temperature. [Pg.118]

Show that equations (19.25) and (19.26) for the entropy change of ala ideal monatomic gas at constant pressure and constant temperature, respectively, follow from the Sackur-Tetrode equation (24.13) or (24.14). [Pg.200]

Ruff and Bergdahl (1919) and Fischer et al. (1932) recorded the change in the mass of the cell at increasing temperature and at constant inert gas pressure. They observed that the dependence of mass of the cell on time or temperature did not show a sharp break at the equilibrium vapor pressure. The results were not substantially improved by plotting the derivative of mass with respect to time (i.e. the rate of mass loss). Fischer et al. (1932) used the variant of recording the changes of mass at a stepwise decreasing pressure and constant temperature. Flowever, even in this variant, a sharp break of the rate of mass loss versus pressure was not observed. [Pg.321]

Massobrio et al. (1989, 1990) studied defect-induced amorphization in NiZr2 using a constant number of particles, constant pressure and constant temperature (NPT) MD and tight-binding potentials, by randomly exchanging a number of Ni and Zr atoms. They observed a volume increase in the system. The change in volume is more pronounced as the degree of chemical disorder introduced increases. The amorphous structure is similar to a structure obtained from a quenched liquid. [Pg.328]

The energy liberated or absorbed in a reversible process at constant pressure and constant temperature. The change in free energy, AG, in a chemical reaction is given by AG=AH — TAS, where AH is the change in enthalpy, AS is the change in entropy and T is the temperature. This is known as the Gibbs equation. See Enthalpy, Entropy. [Pg.331]

For closed systems at constant pressure and constant temperature, the criterion for equUibxium is that the total free energy of the system Gj) is a minimum. For example, consider the reversible reaction previously examined in Eq. 3-1,... [Pg.61]

However, the most important case is that a system is in contact with a reservoir of constant pressure and constant temperature, and compression energy and thermal energy can be freely exchanged. Here the function Gsys = Usys - Tsys Ssys+Psys Vsys is appropriate and dGsys = 0 is the condition for equilibrium. [Pg.214]

Figure 3.5 A general reaction at constant external pressure and constant temperature. Figure 3.5 A general reaction at constant external pressure and constant temperature.
In a chemical reaction, the substances involved produce new ones with changed entropy demands. Here, we are interested in the amount of entropy AS which is added or removed for compensation when a reaction takes place at constant pressure and constant temperature. Let us consider the reaction of 0.1 mol of iron and 0.1 mol of sulfur forming 0.1 mol of iron sulfide, at room conditions ... [Pg.231]

Partial molar properties are defined for any property that has an extensive form for example, volume, enthalpy, etc. They are intensive properties and as such, they are functions of pressure, temperature, and mol fractions. To see how partial molar properties can be useful, consider the following thought experiment a vessels that contains a mixture (for example, a solution of several components) is poured into another vessel B. We will calculate the enthalpy in vessel B as it builds up during this process. The differential of is given bveq. fo.Sl the process obviously takes place under constant pressure and constant temperature, therefore, dT=o and dP = o. This simplifies the differential to the form. [Pg.343]

For the important conditions of constant pressure and constant temperature (such as reactions carried out in an open beaker on the laboratory bench), a sum known as the Gibbs free energy G totals these entropy changes. And as every good chemistry student knows, reactions proceed spontaneously only when G for the initial state is greater than G for the final, and at equilibrium the change in G is zero. [Pg.228]

Thus, for a chemical, thermodynamic process at both constant pressure and constant temperature ... [Pg.57]

St-Pierre (2009) developed a zero-dimensional model that considers competitive adsorption for a contaminant with O2 or H2 at the cathode or anode side, respectively. This model assumes that contaminant transport through the gas flow channels, GDLs and ionomer in the catalyst layers is much faster compared to surface kinetics. The rate determining step is considered to be due to contaminant reaction or desorption of reaction product from the platinum surface. Other model assumptions include the absence of lateral interaction between adsorbates, first-order reaction kinetics, constant pressure, and constant temperature at the cathode/anode sides. Using a set of parameters, St-Pierre (2009) successfully used his model in order to describe experimental transient data obtained in the presence of SOj, NOj, and HjS in the cathode airstreams. [Pg.216]

This means that when 1 mole of liquid benzene reacts with 7 moles of oxygen, forming 3 moles of liquid water and 6 moles of carbon dioxide at constant pressure and constant temperature, 781 kcal are evolved therefore, the enthalpy of the 3 moles of HjOfl) and 6 moles of C02less than the enthalpy of 1 mole of CsHe(0 and 74 moles of 02(g). Since AH = HpmductB Hreactants. AH is negative for the combustion of C6Hg(i). For the decomposition of nickel oxide at 25.0 C,... [Pg.63]

It should be noticed that in the above statements the free energy change is that for the system, and the role of the surroundings need not be included. Since most reactions of chemical and metallurgical interest are performed under constant pressure and constant temperature conditions, the subsequent discussions will be concerned only with the Gibbs free energy, G, and will be described simply as free energy. [Pg.44]

Complete graphical representation of the equilibria requires a three-dimensional diagram [29, 47], as in Fig. 9.1. The curve marked is the vapor-pressure curve of A, lying entirely in the nearest composition plane at x = 1.0. The curve extends from its critical point to its triple point 7 a. but the complications of the solid phase which do not enter into distillation operations will not be considered. Similarly curve is the vapor pressure of pure B, in the far plane at X = 0. The liquid and vapor regions at compositions between x = 0 and 1,0 are separated by a double surface which extends smoothly from p to pg. The shape of this double surface is most readily studied by considering sections at constant pressure and constant temperature, examples of which are shown in the figure. [Pg.344]

Operating conditions of most interest for electrochemical cells are constant pressure and constant temperature. Constant composition is approached in the limit of negligible current flow. Under these conditions. [Pg.153]

With regard to the results obtained due to the variations in pressure, it can be said that an increase in pressure increases solvent permeability thus increasing the contact siuface area between the extractable compounds and the extraction solvent. Therefore, it can be assumed that increases in pressure and constant temperatures can increase the density of the fluid and its solubility power (Santos, 2012 Freitas et al., 2008). [Pg.35]


See other pages where Constant Temperature and Pressure is mentioned: [Pg.62]    [Pg.662]    [Pg.138]    [Pg.80]    [Pg.70]    [Pg.55]    [Pg.111]    [Pg.298]    [Pg.105]    [Pg.12]    [Pg.508]    [Pg.41]    [Pg.44]    [Pg.334]    [Pg.63]    [Pg.187]    [Pg.929]    [Pg.22]    [Pg.532]    [Pg.464]   


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