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Perfect equilibrium

Taking the balance, around both phases, effectively disregards the rate of solute transfer from liquid to solid and, instead, the assumption of a perfect equilibrium stage is employed to provide a relation between the resulting liquid and solid phase concentrations. For the special case of a linear equilibrium... [Pg.487]

Ratio QIK is adimensional if it is higher than 1 (i.e., log QIK> 0), the aqueous solution is oversaturated with respect to the solid phase if it is zero, we have perfect equilibrium and if it is lower than 1 (i.e., log QIK < 0), the aqueous phase is undersaturated with respect to the solid phase. [Pg.579]

In complete equilibrium, the ratio of the population of an atomic or molecular species in an excited electronic state to the population in the groun d state is given by Boltzmann factor e — and the statistical weight term. Under these equilibrium conditions the process of electronic excitation by absorption of radiation will be in balance with electronic deactivation by emission of radiation, and collision activation will be balanced by collision deactivation excitation by chemical reaction will be balanced by the reverse reaction in which the electronically excited species supplies the excitation energy. However, this perfect equilibrium is attained only in a constant-temperature inclosure such as the ideal black-body furnace, and the radiation must then give -a continuous spectrum with unit emissivity. In practice we are more familiar with hot gases emitting dis-... [Pg.527]

The term "perfect" is a play on the standard game-theoretic notion of perfect equilibrium and here reflects that people believe that their future behavior will be rational. The term "perception" allows for people to have correct or incorrect beliefs about their own future behavior. [Pg.202]

The concept of plate theory was originally proposed for the performance of distillation columns (12). However, Martin and Synge (13) first applied the plate theory to partition chromatography. The theory assumes that the column is divided into a number of zones called theoretical plates. One determines the zone thickness or height equivalent to a theoretical plate (HETP) by assuming that there is perfect equilibrium between the gas and liquid phases within each plate. The resulting behavior of the plate column is calculated on the assumption that the distribution coefficient remains unaffected by the presence of other... [Pg.62]

Many human activities interfere with the normal conditions of the upper crust, the hydrosphere and the atmosphere. Geochemistry can monitor and possibly direct the development of more environment-conscious attitudes. For decades geochemists have been busy collecting data on sediment cover, soil, and the hydrosphere, atmosphere and biosphere of our planet. Early observations demonstrated an almost perfect equilibrium system today atmosphere, hydrosphere, and soil in many places are far out of balance (cf. Banar, Forstner and Muller, 1972 a, b, a report on river waters and sediments in Germany with a good reference list). All biological activity is seriously affected (cf. Muller and Forstner, 1973), not only in freshwater systems but also in parts of the oceans, where disequilibrium conditions have been observed locally. The German Science... [Pg.165]

Let us first consider the case of a discontinuous, point-by-point procedure. An absolute or perfect equilibrium can of course never be attained, since it is limited by the fluctuations of (a) the adsorbent temperature, (b) the residual gas temperature, and (c) the baseline of the pressure transducer. As a consequence, after a certain time, the system is as close as it will ever get to true equilibrium. Nevertheless, this time may be relatively long (e.g. it may take hours to determine each point). The experimenter may then decide to be less demanding in order to save time. A convenient way to operate, which lends itself to automation, is the following ... [Pg.86]

Martin and Synge provided the first theoretical treatment of LLPC by adapting the concept of theoretical plates which had been developed, mainly, for distillation and countercurrent extraction. According to the theory, a chromatographic column is considered to consist of a number of theoretical plates, within each of which perfect equilibrium occurs between the mobile and the stationary phases. Unlike in RPC employing hydrocarbonaceous bonded stationary phases where the retention mechanism is still the subject of contro-... [Pg.960]

Nernst, Walther. (1864-1941). A German chemist who won the Nobel Prize in 1920. He was educated atZurich and Berlin and received his Ph.D. at Wurzburg. He wrote many works concerning theory of electric potential and conduction of electrolytic solutions. He developed the third law of thermodynamics, which states that at absolute zero the entropy of every material in perfect equilibrium is zero, and therefore volume, pressure, and surface tension all become independent of temperature. He also invented Nernst s lamp, which required no vacuum and little current. [Pg.882]

In a real radiation source this perfect equilibrium cannot exist and there are losses of energy as a result of the emission and absorption of radiation, which also have to be considered. However, as long as both only slightly affect the energy balance, the system is in so-called local thermal equilibrium and ... [Pg.10]

Theoretically an infinite incubation period would be needed to reach perfect equilibrium in the first step (incubation with H). However, in practice, conditions are chosen so as to shorten this period to reach near-perfect equilibrium. The association and dissociation constants (fca., and /c,) are usually not known, but according to the law of mass action the higher the Ab and H concentrations, the faster Ab-H is formed. The concentration of H, however, should not exceed that of Ab. In the commercial kits (Section 14.3), the concentrations are sometimes so high that the few seconds between... [Pg.142]

As mentioned earher, the plate theory has played a role in the development of chromatography. The concept of "plate" was originally proposed as a measmement of the performance of distillation processes. It is based upon the assumption that the column is divided into a number of zones called theoretical plates, that are treated as if there exists a perfect equilibrium between the gas and the Hquid phases within each plate. This assumption imphes that the distribution coefficient remains the same fi-om one plate to another plate, and is not affected by other sample components, and that the distribution isotherm is hnear. However, experimental evidences show that this is not true. Plate theory disregards that chromatography is a dynamic process of mass transfer, and it reveals httle about the factors affecting the values of the theoretical plate number. In principle, once a sample has been introduced, it enters the GC column as a narrow-width "band" or "zone" of its composite molecules. On the column, the band is further broadened by interaction of components with the stationary phase which retains some components more than others. Increasing... [Pg.70]

The sequence of condensation of solids from a solar composition at a nebular pressure of 10 Pa (about 10 atm) is shown in Fig. 2-4. This sequence is calculated for what solids could exist in equilibrium with the solar nebula at various temperatures. Attainment of true equilibrium requires the lack of nucleation barriers, and efficient diffusion within solids so that grain interiors can maintain equilibrium with the gas phase. While strict equilibrium condensation may have occurred at higher temperatures, perfect equilibrium probably did not occur with grains larger than a few micrometers in size or... [Pg.15]

The glyph of Libra (see Figure 6-2) represents a simple balance or the scales of justice. It also suggests the setting Sun, which reflects the fact that the first day of Libra is the fall equinox, when day and night reach a point of perfect equilibrium. [Pg.69]

The theory developed in Section 12.6 assumed that the plate acts as a perfect equilibrium stage for separation. However, in practice it is found that this is only an approximation. While the temperature of the vapour leaving the plate is likely to be the same as that of the liquid leaving the plate, the difference in compositions of the vapour and the liquid is often not as great as implied by equation (12.63), and the plate has therefore not been such an efficient separation stage. The deviation from equilibrium is accounted for partly by gross physical phenomena such as carryover of liquid droplets in the vapour leaving the plate, but a more fundamental reason is the restricted rate of mass transfer between the vapour and liquid phases. A column efficiency, r/r, may be defined as the ratio of the number of plates needed in theory. Nr, to the number needed in practice, Np, to achieve the desired separation ... [Pg.132]

The material-balance equation for each component in the upper section of the column [Eq. (18.14)] can be written with yJK in place of x , which assumes perfect equilibrium between vapor and liquid ... [Pg.600]

Under the presumed condition of having reached a perfect equilibrium, and as the liquid is a pure substance, the partial pressure appears to equal the vapor pressure p (T = r ). For temperatures near the boiling point of water, the simplified equation, (4.2-29) is no longer applicable and rather the following holds ... [Pg.186]

State of perfect (or nearly perfect) equilibrium. Moreover the separation or crystallisation gives rise to an establishment of mutual equilibrium between the two liquid layers, or between the crystals and saturated solution. [Pg.7]

However, we observed a long time dependence of x in the temperature range of 44-55 K over several hours upon cooling from liquid O2. Figure 3 shows the y-T relation at equilibrium. Here the % value at 44K after 2.2 x lO s is used in Fig. 3, which should be smaller than the perfect equilibrium % value. The equilibrium x values are smaller than nonequilibrium ones by one or two orders of magnitude (see Fig. 2). An obscure jump near 24 K and a very steep jump at 44 K are shown. The latter jump should become more pronounced if we measure it after a much longer time. The shape of x relation near 44K is close to a type [44]. Consequently, the well-known x relation in Fig. 2 is obtained at nonequilibrium conditions. [Pg.494]

It is presumed that both the a and (3 phases should form a single phase at perfect equilibrium. The obscure a—p transition at 24K should stem from residual crystallites of the p phase due to a finite cooling rate from liquid O2. Marked time dependence is one of the characteristics of random magnetism, and therefore the higher temperature solid phase (> 24 K) should show random magnetism. As the X value of the lower temperature phase (<24K) decreases with the decrease of temperature, it should be antiferromagnetic. [Pg.494]

In thermodynamic systems, that is, in our models, equilibrium is defined in terms of chemical potentials, which we will get to in a later chapter. This state, as you might imagine, is one of perfect equilibrium, perfect rest, with absolutely no gradients or inhomogeneities of any kind. Real systems often approach this state more or less closely, but probably never attain it. When real systems do approach equilibrium, thermodynamics can be applied to them. Obviously, we need to have some way of telling whether real systems are at equilibrium, or have closely approached equilibrium. [Pg.12]

Maintaining perfect equilibrium while cooling is one end of a complete spectrum of possibilities. The other end of the spectrum is that crystals form, but always completely out of equilibrium. This end of the spectrum involves an infinite number of cases and so is rather difficult to discuss in a finite number of words. A subset of these possibilities is the case where crystallization produces crystals in equilibrium with the liquid, as required by the diagram, but after forming, they do not react with the liquid in any way. This is called surface equilibrium (because the liquid is at all times in equilibrium with the surface of the crystals) or fractional crystallization, and is a model process just as much as is equilibrium crystallization. It is also used in connection with liquid-vapor processes (fractional distillation fractional condensation), as well as isotope fractionation processes. [Pg.519]

Mb Ms) The maximum share the buyer (the supplier) could receive in a subgame perfect equilibrium for any subgame initiated with the buyer s (the supplier s) offer. [Pg.82]


See other pages where Perfect equilibrium is mentioned: [Pg.42]    [Pg.20]    [Pg.521]    [Pg.28]    [Pg.545]    [Pg.16]    [Pg.24]    [Pg.25]    [Pg.114]    [Pg.3081]    [Pg.168]    [Pg.42]    [Pg.620]    [Pg.133]    [Pg.38]    [Pg.66]    [Pg.35]    [Pg.3]    [Pg.103]    [Pg.122]    [Pg.519]    [Pg.20]    [Pg.42]    [Pg.43]    [Pg.82]    [Pg.82]   
See also in sourсe #XX -- [ Pg.24 , Pg.25 ]




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Equilibrium thermodynamics of the perfect solid

Introduction and Perfect Gas Equilibria

Other forms of equilibrium constant for perfect gas mixtures

Perfect equilibrium crystallization

Perfecting

Perfection

Perfectly

Perfectly mobile equilibria the mean diffusion coefficient

Subgame perfect equilibrium

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