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Equation ideal gas

The kinetic theory of gases reduces to a remarkably simple mathematical form, known as the Ideal gas equation. [Pg.162]

The ideal gas equation shows that P, V, n and T are not independent. These variables cannot take on any values we like - nature has dictated that if three of them are known, then the fourth is fixed. [Pg.162]

The equation contains no factor which is specific to any gas. The type of gas (helium, chlorine, oxygen, water vapour, etc.) is irrelevant. [Pg.162]

The rearranged forms of the ideal gas equation are often used in calculations  [Pg.162]

The inter-relationships between P, V, n and T, summarized in the gas laws of Charles, Boyle and Avogadro, are inbuilt into the ideal gas equation, and the equation makes the separate use of these laws in calculations redundant. For example, the ideal gas equation shows that if the pressure and the number of moles of gas does not change, then V is proportional to T. In other words, it predicts Charles law. [Pg.162]

When the postulates of the kinetic theory are not valid, the observed gas will not obey the ideal gas equation. In many cases, including a variety of important engineering applications, gases need to be treated as nonideal, and empirical mathematical descriptions must be devised. There are many equations that may be used to describe the behavior of a real gas the most commonly used is probably the [Pg.181]

An empirical equation contains one or more adjustable parameters that are found from a best ft to observed data rather than from a theoretical model. [Pg.181]

In Example Problem 5.1, we considered a CH4 storage tank with a volume of 49.0 L. en empty, the tank has a mass of 55.85 kg, and when filled, its mass is 62.07 kg. Calculate the pressure of CH4 in the tank at an ambient temperature of [Pg.182]

21°C using both the ideal gas equation and the van der Waals equation. What is the percentage correction achieved by using the more realistic van der Waals equation  [Pg.183]

We will use two different models to describe the same gas, and each model will be represented by its own equation. So we will do two independent calculations, solving for P in each case. We can find the mass of CH4 from the given data, and then convert that mass into the number of moles by using the molar mass. And the van der Waals constant for CH4 can be found in Table 5.2. Th calculate the percentage difference we will divide the difference of the two numbers by the value for the ideal gas case. [Pg.183]


Coefficients for calculation of the enthalpy of an ideal gas (equation 4.77) for common light components. [Pg.418]

On the other hand, as applied to the submonolayer region, the same comment can be made as for the localized model. That is, the two-dimensional non-ideal-gas equation of state is a perfectly acceptable concept, but one that, in practice, is remarkably difficult to distinguish from the localized adsorption picture. If there can be even a small amount of surface heterogeneity the distinction becomes virtually impossible (see Section XVll-14). Even the cases of phase change are susceptible to explanation on either basis. [Pg.653]

The importance of the van der Waals equation is that, unlike the ideal gas equation, it predicts a gas-liquid transition and a critical point for a pure substance. Even though this simple equation has been superseded, its... [Pg.184]

Real gases follow the ideal-gas equation (A2.1.17) only in the limit of zero pressure, so it is important to be able to handle the tliemiodynamics of real gases at non-zero pressures. There are many semi-empirical equations with parameters that purport to represent the physical interactions between gas molecules, the simplest of which is the van der Waals equation (A2.1.50). However, a completely general fonn for expressing gas non-ideality is the series expansion first suggested by Kamerlingh Onnes (1901) and known as the virial equation of state ... [Pg.354]

It is sometimes convenient to retain the generality of the limiting ideal-gas equations by introducing the activity a, an effective pressure (or, as we shall see later in the case of solutions, an effective mole fraction. [Pg.355]

But since the ideal gas equation requires that = pRT/M, this reduces finally to... [Pg.128]

The behavior of all gases that obey the laws of Boyle and Charles, and Avogadro s hypothesis, can be expressed by the ideal gas equation ... [Pg.528]

The Ideal Gas The simplest equation of state is the ideal gas equation ... [Pg.516]

As long as the volume flow is kept near design point, both the deflection angle and pressure drop can be corrected. Temperature differential increase is limited by metallurgy, so it is neglected in analytical calculations. This evaluation is based on inlet pressure changes. The new volume at a different pressure is calculated by the ideal gas equation ... [Pg.468]

Tabulation showing percent changes in P arid Tj needed to cause AVo change in air compressor efficiency. Ideal gas equations are used. [Pg.664]

Compressibility is experimentally derived from data about the actual behavior of a particular gas under pVT changes. The compressibility factor, Z, is a multiplier in the basic formula. It is the ratio of the actual volume at a given pT condition to ideal volume at the same pT condition. The ideal gas equation is therefore modified to ... [Pg.635]

If the gas is not ideal, so that the ideal gas equation cannot be used, we replace the pressurep in equations 20.198 and 20.199 by the fugacity,/, such that the ideal gas equation still holds if the pressure p is replaced by the fugacity, an effective pressure, when the real pressure is p. This form is most convenient because of the numerous ways in which non-ideality can be expressed, and we note that the fugacity is related to, but not necessarily proportional to the pressure. We can express the fugacity as a function of the pressure by introducing the fugacity coefficient, 7p, as / = y p, which then replacesp in equation 20.199 for the non-ideal case. The value of 7p tends to unity as the gas behaves more ideally, which means as the pressure decreases. [Pg.1232]

In the next chapter, we will return to the Carnot cycle, describe it quantitatively for an ideal gas with constant heat capacity as the working fluid in the engine, and show that the thermodynamic temperature defined through equation (2.34) or (2.35) is proportional to the absolute temperature, defined through the ideal gas equation pVm = RT. The proportionality constant between the two scales can be set equal to one, so that temperatures on the two scales are the same. That is, 7 °Absolute) = T(Kelvin).r... [Pg.61]

It is useful to compare the reversible adiabatic and reversible isothermal expansions of the ideal gas. For an isothermal process, the ideal gas equation can be written... [Pg.134]

Thus, p can be estimated from the observed pressure and the ideal pressure calculated from the molar volume and the ideal gas equation. Klotz and Rosenburg3 report that the error in using equation (6.23) to calculate p is less than 1% for O2 up to a pressure of 10 MPa. For CO2 (g) the error is 1% at 2.5 MPa and 4% at 5 MPa. [Pg.254]

Equation (7.123)w is often referred to as the law of Van t Hoff, since it was originally proposed by J. H. Van t Hoff. It is interesting to note that equation (7.123) is of the same form as the ideal gas equation, if one takes c as njVx Table 7.3 compares experimental values of II for aqueous sucrose solutions with those calculated using equations (7.120) and (7.123). We see that neither of the equations predicts n with high accuracy. However, the superiority of equation (7.120), especially at higher concentrations, is apparent. [Pg.372]

Example 10.4 Use Zm to derive the ideal gas equation Solution From Table 3.1... [Pg.553]

For a non-ideal gas, equation 2.15 is modified by including a compressibility factor Z which is a function of both temperature and pressure ... [Pg.34]

The independent variables in these equations are the dimensionless spatial coordinates, x and r. The dependent variables are the dimensionless velocity components (u the axial velocity, v the radial velocity, and w circumferential velocity), temperature , and pressure pm- The viscosity and thermal conductivity are given by p and A, and the mass density by p. Density is determined from the temperature and pressure via an ideal-gas equation of state. The dimen-... [Pg.338]


See other pages where Equation ideal gas is mentioned: [Pg.351]    [Pg.423]    [Pg.429]    [Pg.460]    [Pg.484]    [Pg.488]    [Pg.516]    [Pg.518]    [Pg.518]    [Pg.788]    [Pg.188]    [Pg.956]    [Pg.400]    [Pg.1233]    [Pg.88]    [Pg.98]    [Pg.120]    [Pg.162]    [Pg.34]    [Pg.296]    [Pg.296]    [Pg.88]    [Pg.294]    [Pg.118]   
See also in sourсe #XX -- [ Pg.28 , Pg.38 , Pg.52 , Pg.53 , Pg.55 , Pg.57 , Pg.107 , Pg.154 , Pg.203 , Pg.212 , Pg.221 ]

See also in sourсe #XX -- [ Pg.258 ]

See also in sourсe #XX -- [ Pg.405 ]

See also in sourсe #XX -- [ Pg.421 , Pg.551 ]




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Applications of the Ideal Gas Equation

Equation of state for ideal gases at very low temperatures

Equations of state for ideal and real gases

Equations of state for ideal gases

Equations of state ideal gas

Further Applications of the Ideal-Gas Equation

Gas equation

General equation of an ideal gas

Ideal gas equations for

Ideal gas equations of state and

Phenomenological Derivation of the Ideal Gas Equation

Stoichiometry ideal gas equation

The Ideal Gas Equation

The Ideal Gas Equation Determination of a Single Variable

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