Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Ideality, deviations

Plug flow is an idealization. Deviations arise with viscous or non-Newtonian fluids. A mathematically simple deviation from the plug flow pattern is that of power law fluids whose velocity in a tube depends on the radial position, /3 = r/R, according to the equation,... [Pg.265]

B + B A4-A N + N A + N B + N Quasi-ideal, + deviation if any No H bonds involved Acetone + -hexane (min), benzene + methyl-cyclopentane (min), propyl ether + triethyl-amine (min), methyl mercaptan + butane (min), 2-butanone + benzene (min)... [Pg.40]

Drivers of liking 1 + 1 1 Deviation from ideal Deviation from ideal Drivers of liking ... [Pg.329]

The stability of the laser wavelength can, of course, never exceed that of the reference wavelength. Generally it is worse because the control system is not ideal. Deviations AX(t) = -A.l(0 r cannot be compensated immediately because the system has a finite frequency response and the inherent time constants always cause a phase lag between deviation and response. [Pg.280]

Figures 3 and 4 show fugacity coefficients for two binary systems calculated with Equation (10b). Although the pressure is not large, deviations from ideality and from the Lewis rule are not negligible. Figures 3 and 4 show fugacity coefficients for two binary systems calculated with Equation (10b). Although the pressure is not large, deviations from ideality and from the Lewis rule are not negligible.
The virial equation is appropriate for describing deviations from ideality in those systems where moderate attractive forces yield fugacity coefficients not far removed from unity. The systems shown in Figures 2, 3, and 4 are of this type. However, in systems containing carboxylic acids, there prevails an entirely different physical situation since two acid molecules tend to form a pair of stable hydrogen bonds, large negative... [Pg.31]

Figure 4-9. Vapor-liquid equilibria for a binary system where one component dimerizes in the vapor phase. Activity coefficients show only small deviations from liquid-phase ideality. Figure 4-9. Vapor-liquid equilibria for a binary system where one component dimerizes in the vapor phase. Activity coefficients show only small deviations from liquid-phase ideality.
Moderate errors in the total pressure calculations occur for the systems chloroform-ethanol-n-heptane and chloroform-acetone-methanol. Here strong hydrogen bonding between chloroform and alcohol creates unusual deviations from ideality for both alcohol-chloroform systems, the activity coefficients show... [Pg.53]

The results shown in Table 2 indicate that UNIQUAC can be used with confidence for multicomponent vapor-liquid equilibria including those that exhibit large deviations from ideality. [Pg.55]

For a real vapor mixture, there is a deviation from the ideal enthalpy that can be calculated from an equation of state. The enthalpy of the real vapor is given by... [Pg.84]

Figure 3 presents results for acetic acid(1)-water(2) at 1 atm. In this case deviations from ideality are important for the vapor phase as well as the liquid phase. For the vapor phase, calculations are based on the chemical theory of vapor-phase imperfections, as discussed in Chapter 3. Calculated results are in good agreement with similar calculations reported by Lemlich et al. (1957). ... [Pg.91]

By contrast with ideal models, practical reactors must consider many factors other than variations in temperature, concentration, and residence time. Practical reactors deviate from the three idealized models but can be classified into a number of common types. [Pg.52]

The above equation is valid at low pressures where the assumptions hold. However, at typical reservoir temperatures and pressures, the assumptions are no longer valid, and the behaviour of hydrocarbon reservoir gases deviate from the ideal gas law. In practice, it is convenient to represent the behaviour of these real gases by introducing a correction factor known as the gas deviation factor, (also called the dimensionless compressibility factor, or z-factor) into the ideal gas law ... [Pg.106]

It was found that that in the case of soft beta and X-ray radiation the IPs behave as an ideal gas counter with the 100% absorption efficiency if they are exposed in the middle of exposure range ( 10 to 10 photons/ pixel area) and that the relative uncertainty in measured intensity is determined primarily by the quantum fluctuations of the incident radiation (1). The thermal neutron absorption efficiency of the present available Gd doped IP-Neutron Detectors (IP-NDs) was found to be 53% and 69%, depending on the thicknes of the doped phosphor layer ( 85pm and 135 pm respectively). No substantial deviation in the IP response with the spatial variation over the surface of the IP was found, when irradiated by the homogeneous field of X-rays or neutrons and deviations were dominated by the incident radiation statistics (1). [Pg.507]

At each step, the computer reeords the amplitude of R.F. signal sent by the generator, witli tile eventual eorreetion made by the operator. At the end of the measurement, the software calculates the maximum deviation of linearity versus the ideal curve. [Pg.704]

The deviation of Gibbs monolayers from the ideal two-dimensional gas law may be treated by plotting xA// 7 versus x, as shown in Fig. III-15c. Here, for a series of straight-chain alcohols, one finds deviations from ideality increasing with increasing film pressure at low x values, however, the limiting value of unity for irAfRT is approached. [Pg.83]

In 1873, van der Waals [2] first used these ideas to account for the deviation of real gases from the ideal gas law P V= RT in which P, Tand T are the pressure, molar volume and temperature of the gas and R is the gas constant. Fie argried that the incompressible molecules occupied a volume b leaving only the volume V- b free for the molecules to move in. Fie further argried that the attractive forces between the molecules reduced the pressure they exerted on the container by a/V thus the pressure appropriate for the gas law isP + a/V rather than P. These ideas led him to the van der Waals equation of state ... [Pg.184]

It is detemrined experimentally an early study was the work of Andrews on carbon dioxide [1], The exact fonn of the equation of state is unknown for most substances except in rather simple cases, e.g. a ID gas of hard rods. However, the ideal gas law P = pkT, where /r is Boltzmaim s constant, is obeyed even by real fluids at high temperature and low densities, and systematic deviations from this are expressed in tenns of the virial series ... [Pg.441]

The McMillan-Mayer theory offers the most usefiil starting point for an elementary theory of ionic interactions, since at high dilution we can incorporate all ion-solvent interactions into a limitmg chemical potential, and deviations from solution ideality can then be explicitly coimected with ion-ion interactions only. Furthemiore, we may assume that, at high dilution, the interaction energy between two ions (assuming only two are present in the solution) will be of the fomi... [Pg.575]

From these results, the thennodynamic properties of the solutions may be obtamed within the McMillan-Mayer approximation i.e. treating the dilute solution as a quasi-ideal gas, and looking at deviations from this model solely in temis of ion-ion interactions, we have... [Pg.577]

Figure A2.5.5. Phase diagrams for two-eomponent systems with deviations from ideal behaviour (temperature T versus mole fraetion v at eonstant pressure). Liquid-gas phase diagrams with maximum (a) and minimum (b) boiling mixtures (azeotropes), (e) Liquid-liquid phase separation, with a eoexistenee eurve and a eritieal point. Figure A2.5.5. Phase diagrams for two-eomponent systems with deviations from ideal behaviour (temperature T versus mole fraetion v at eonstant pressure). Liquid-gas phase diagrams with maximum (a) and minimum (b) boiling mixtures (azeotropes), (e) Liquid-liquid phase separation, with a eoexistenee eurve and a eritieal point.
In the case of bunolecular gas-phase reactions, encounters are simply collisions between two molecules in the framework of the general collision theory of gas-phase reactions (section A3,4,5,2 ). For a random thennal distribution of positions and momenta in an ideal gas reaction, the probabilistic reasoning has an exact foundation. Flowever, as noted in the case of unimolecular reactions, in principle one must allow for deviations from this ideal behaviour and, thus, from the simple rate law, although in practice such deviations are rarely taken into account theoretically or established empirically. [Pg.769]

In tenns of an electrochemical treatment, passivation of a surface represents a significant deviation from ideal electrode behaviour. As mentioned above, for a metal immersed in an electrolyte, the conditions can be such as predicted by the Pourbaix diagram that fonnation of a second-phase film—usually an insoluble surface oxide film—is favoured compared with dissolution (solvation) of the oxidized anion. Depending on the quality of the oxide film, the fonnation of a surface layer can retard further dissolution and virtually stop it after some time. Such surface layers are called passive films. This type of film provides the comparably high chemical stability of many important constmction materials such as aluminium or stainless steels. [Pg.2722]

The raie gas atoms reveal through their deviation from ideal gas behavior that electrostatics alone cannot account for all non-bonded interactions, because all multipole moments are zero. Therefore, no dipole-dipole or dipole-induced dipole interactions are possible. Van der Waals first described the forces that give rise to such deviations from the expected behavior. This type of interaction between two atoms can be formulated by a Lennaid-Jones [12-6] function Eq. (27)). [Pg.346]


See other pages where Ideality, deviations is mentioned: [Pg.232]    [Pg.207]    [Pg.232]    [Pg.207]    [Pg.31]    [Pg.34]    [Pg.35]    [Pg.51]    [Pg.14]    [Pg.202]    [Pg.205]    [Pg.271]    [Pg.639]    [Pg.483]    [Pg.490]    [Pg.615]    [Pg.160]    [Pg.222]    [Pg.252]   
See also in sourсe #XX -- [ Pg.181 , Pg.182 ]




SEARCH



Bulk, Ideal, measuring deviations

Compressibility Factor and Ideal Gas Deviations

Counterion deviation from ideality

DEVIATIONS FROM IDEAL REACTOR PERFORMANCE

Deviation from Ideal Bond Angles

Deviation from ideal flow,”244------Difference equations

Deviation from ideal gas

Deviation from ideal gas behaviour

Deviation from ideal solution

Deviations from Ideal Gases Difference Measures

Deviations from Ideal Gases Ratio Measures

Deviations from Ideal Kinetics

Deviations from Ideal Solutions Difference Measures

Deviations from Ideal Solutions Ratio Measures

Deviations from Ideal Stress-Strain Behavior

Deviations from Ideality in Terms of Excess Thermodynamic Functions

Deviations from dilute ideal solutions

Deviations from ideal behavior

Deviations from ideal flow

Deviations from ideal flow conditions

Deviations from ideal-gas mixtures

Deviations of Double-layer Capacitance from Ideal Behavior Representation by a Constant-phase Element (CPE)

Dilute ideal solutions small deviations from

Excess functions and deviation from ideality

First-order deviations from ideal-gas mixtures

Free radical polymerization deviation from ideal kinetics

Gases, deviation from ideal behavior

Ideal analytical model, deviations

Ideal behavior factors that cause deviation from

Ideal deviations from

Ideal flows, deviation from bypassing

Ideal flows, deviation from channeling

Ideal flows, deviation from dispersion

Ideal gas deviations

Ideal structures, deviations from

Ideality, deviation from

Ideality, deviation from INDEX

Ideality, deviation from functions

Ideality, deviation from gases

Ideality, deviation from virial function

Models allowing for the deviations from ideality

Molecular geometry deviation from ideal bond angles

Negative Deviations from Ideal Solution Behavior (Type III)

Negative deviation from ideal solution

Negative deviation from ideality

Physicochemical properties deviations from ideal

Positive deviation from ideal solution

Positive deviations from ideality

Real Gases Deviations from Ideal Behavior

Real Gases Exhibit Deviations from Ideal Behavior at High Pressures

Single deviations from ideal crystal structure

Small Deviations from Symmetric Ideal (SI) Solutions

Studies concerning the deviation from ideal plug flow conditions

Symmetrical ideal deviations from

The ideal gas and small deviation from ideality

© 2024 chempedia.info