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Gases standard pressure

Rare-gas clusters can be produced easily using supersonic expansion. They are attractive to study theoretically because the interaction potentials are relatively simple and dominated by the van der Waals interactions. The Lennard-Jones pair potential describes the stmctures of the rare-gas clusters well and predicts magic clusters with icosahedral stmctures [139, 140]. The first five icosahedral clusters occur at 13, 55, 147, 309 and 561 atoms and are observed in experiments of Ar, Kr and Xe clusters [1411. Small helium clusters are difficult to produce because of the extremely weak interactions between helium atoms. Due to the large zero-point energy, bulk helium is a quantum fluid and does not solidify under standard pressure. Large helium clusters, which are liquid-like, have been produced and studied by Toennies and coworkers [142]. Recent experiments have provided evidence of... [Pg.2400]

For species present as gases ia the actual reactive system, the standard state is the pure ideal gas at pressure F°. For Hquids and soHds, it is usually the state of pure real Hquid or soHd at F°. The standard-state pressure F° is fixed at 100 kPa. Note that the standard states may represent different physical states for different species any or all of the species may be gases, Hquids, or soHds. [Pg.500]

Flow Low mass flow indicated. Mass flow error. Transmitter zero shift. Measurement is high. Measurement error. Liquid droplets in gas. Static pressure change in gas. Free water in fluid. Pulsation in flow. Non-standard pipe runs. Install demister upstream heat gas upstream of sensor. Add pressure recording pen. Mount transmitter above taps. Add process pulsation damper. Estimate limits of error. [Pg.325]

All the above deals with gases and gas phase processes. We now turn to non-gaseous components of the system. There are many ways of expressing this. Probably the simplest is to consider an ideal solution of a solute in a solvent. If the solution is ideal, the vapour pressure of the solute is proportional to its concentration, and we may write p = kc, where c is the concentration and k is the proportionality constant. Similarly, = Arc , which expresses the fact that the standard pressure is related to a standard concentration. Thus we may write from equation 20.198 for a particular component... [Pg.1234]

FIGURE 8.4 The variation of the molar Gibbs free energy of an ideal gas with pressure. The Gibbs free energy has its standard value when the pressure of the gas is 1 bar. The value of the Gibbs free energy approaches minus infinity as the pressure falls to zero. [Pg.433]

The gas stored in the tank is not at standard pressure, so apply Equation to calculate its molar entropy. As the gas leaves the tank, it expands and its entropy increases. The final pressure is not standard pressure, so again use Equation to calculate its molar entropy at the final pressure. Then calculate the entropy change for the expansion, taking the difference in molar entropies between initial and final conditions and multiplying by the number of moles undergoing the expansion. [Pg.999]

Equation (3.1.50) can be developed further. Consider once again cell (3.1.40), together with Eq. (3.1.49). We shall assume that hydrogen gas is under standard pressure in addition, metallic silver, solid silver chloride and gaseous hydrogen at standard pressure are selected as standards, that is... [Pg.174]

Values for free energy are usually referred to the standard free energy G°. The standard state is arbitrary and designates the datum level. A gas is considered here to be at a standard state if it is at a pressure of 1 atm or 1 bar for the designated temperature of an isothermal process. Thus, integrating Equation 6.9 from standard pressure P< > to pressure P gives ... [Pg.97]

According to the combined gas law, the volume of a given mass of gas can have any value, depending on its temperature and pressure. To compare the quantities of gas present in two different samples, it is useful to adopt a set of standard conditions of temperature and pressure. By universal agreement, the standard temperature is chosen as 273 K (0°C) and the standard pressure is chosen as exactly 1 atm (760torr). Together, these conditions are referred to as standard conditions or as standard temperature and pressure (STP). While there is nothing special about STP, some authors and some instructors find it convenient to use this short notation for this particular temperature and pressure. [Pg.189]

The thermodynamic standard state of a substance is its most stable state under standard pressure (1 atm) and at some specific temperature (usually 25°C). Thermodynamic refers to the observation, measurement and prediction of energy changes that accompany physical changes or chemical reaction. Standard refers to the set conditions of 1 atm pressure and 25°C. The state of a substance is its phase gas, liquid or solid. Substance is any kind of matter all specimens of which have the same chemical composition and physical properties. [Pg.239]

Industrial use of fluorine gas treatment started at the end of the 1980s. Surface modifications with fluorine offer improved reactivity for subsequent demands. One of the major advantages of fluorine gas treatment is the fact that modifications can be carried out under standard pressure and temperature (Figure 17.1), so that it can be used for on-line processes at low cost. Areas of application include, plastic fuel containers, gluing, dyeing or printing preparations on plastics.1-3... [Pg.261]

The discovery of supercritical fluids occurred in 1879, when Thomas Andrews actually described the supercritical state and used the term critical point. A supercritical fluid is a material above its critical point. It is not a gas, or a liquid, although it is sometimes referred to as a dense gas. It is a separate state of matter defined as all matter by both its temperature and pressure. Designation of common states in liquids, solids and gases, assume standard pressure and temperature conditions, or STP, which is atmospheric pressure and 0°C. Supercritical fluids generally exist at conditions above atmospheric pressure and at an elevated temperature. Figure 16.1 shows the typical phase diagram for carbon dioxide, the most commonly used supercritical fluid [1]. [Pg.564]

Is the answer reasonable You have almost 10 mol of gas. It would occupy about 224 L at STP (10 mol x 22.4 L/mol) by Avogadro s relationship. The pressure is slightly less than standard pressure of 1 atm, which would tend to increase the volume (Boyle s law), and temperature is greater than standard temperature of 0°C, which would also increase the volume (Charles s law). So you might expect a volume greater than 224 L, and that is exactly what you found. [Pg.109]

Equation 2.63 is valid for any homogeneous or heterogeneous reaction. The only difference is in the definition of activities. For a species in a perfect gas-phase mixture a = pi/p°, where pi is the partial pressure of species i andp° is the standard pressure (1 bar). For a real gas-phase mixture a =f/p°, where is the fugacity of i. The fugacity concept was developed for the same reason as the activity to extend to real gases the formalism used to describe perfect gas mixtures. In the low total pressure limit (p -> 0), fi = pi. [Pg.34]

Here G°(T) refers to an n mole ideal gas system at a standard pressure designated as P° (usually 1 bar). The chemical potential of a one component i ideal gas system is then... [Pg.85]

Here fif (T) is the Gibbs free energy per mole of an ideal gas at temperature T and standard pressure P°. Thus the condition of equilibrium for a gas phase system subject to a chemical reaction (Equation 4.36), whether at constant T and P or constant T and V, is given by... [Pg.85]

Here /i j3 is the chemical potential of the ideal gas at the standard pressure. It will be seen subsequently that qi for an ideal gas depends linearly on the volume V, so fif is a function only of the temperature. It does of course depend on the distribution of energy levels of the ideal gas molecules. The form of Equation 4.59 for the chemical potential of an ideal gas component is the same as that previously derived from thermodynamics (Equation 4.47). The present approach shows how to calculate m through the evaluation of the molecular partition function. Furthermore, the... [Pg.87]

The SHE. The H" " H2 couple is the basis of the primary standard around which the whole edifice of electrode potentials rests. We call the H H2 couple, under standard conditions, the standard hydrogen electrode (SHE). More precisely, we say that hydrogen gas at standard pressure, in equilibrium with an aqueous solution of the proton at unity activity at 298 K has a defined value of of 0 at all temperatures. Note that all other standard electrode potentials are temperature-dependent. The SHE is shown schematically in Figure 3.3, while values of Eq r are tabulated in Appendix 3. [Pg.32]

Standard state of gas Zero pressure" and the specified temperature... [Pg.48]

Integration of this equation from the vapor pressure of the liquid p to the standard state for an ideal gas, a pressure of 0.1 MPa, P°,... [Pg.198]

In addition to the correction for the new standard state, it is necessary to correct for the transformation from the real gas at standard pressure to the ideal gas at standard pressure, which is defined as the standard state. ... [Pg.269]

If the pressure of hydrogen gas is maintained at the standard pressure of 1 bar, a pressure that is essentially equal to the fugacity, then the hydrogen can be considered to be in its standard state, with an activity equal to 1. As pure solid Ag and pure solid AgCl are in their standard states, their activities also are equal to 1. Thus, Equation (19.30) can be written as... [Pg.450]


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