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Pressure and Volume

The properties of hydrocarbon gases are relatively simple since the parameters of pressure, volume and temperature (PVT) can be related by a single equation. The basis for this equation is an adaptation of a combination of the classical laws of Boyle, Charles and Avogadro. [Pg.105]

Nearly all experimental eoexistenee eurves, whether from liquid-gas equilibrium, liquid mixtures, order-disorder in alloys, or in ferromagnetie materials, are far from parabolie, and more nearly eubie, even far below the eritieal temperature. This was known for fluid systems, at least to some experimentalists, more than one hundred years ago. Versehaflfelt (1900), from a eareflil analysis of data (pressure-volume and densities) on isopentane, eoneluded that the best fit was with p = 0.34 and 8 = 4.26, far from the elassieal values. Van Laar apparently rejeeted this eonelusion, believing that, at least very elose to the eritieal temperature, the eoexistenee eurve must beeome parabolie. Even earlier, van der Waals, who had derived a elassieal theory of eapillarity with a surfaee-tension exponent of 3/2, found (1893)... [Pg.640]

Gas purification processes fall into three categories the removal of gaseous impurities, the removal of particulate impurities, and ultrafine cleaning. The extra expense of the last process is only justified by the nature of the subsequent operations or the need to produce a pure gas stream. Because there are many variables in gas treating, several factors must be considered (/) the types and concentrations of contaminants in the gas (2) the degree of contaminant removal desired (J) the selectivity of acid gas removal required (4) the temperature, pressure, volume, and composition of the gas to be processed (5) the carbon dioxide-to-hydrogen sulfide ratio in the gas and (6) the desirabiUty of sulfur recovery on account of process economics or environmental issues. [Pg.209]

Pressure, volume, and temperature relations for perfect gases p,Jp, = VJV,y- (10-61)... [Pg.915]

This equadon indicates diat for a given mass of a specific gas, PV/T has a consumt value. Since, at the same temperature and pressure, volume and mass must be directly proportional, diis statement may be e.xtended to... [Pg.126]

Many process components do not conform to the ideal gas laws for pressure, volume and temperature relationships. Therefore, when ideal concepts are applied by calculation, erroneous results are obtained—some not serious when the deviation from ideal is not significant, but some can be quite serious. Therefore, when data are available to confirm the ideality or non-ideality of a system, then the choice of approach is much more straightforward and can proceed with a high degree of confidence. [Pg.4]

R = gas constant, depends on units of pressure, volume, and temperature... [Pg.370]

Many gases at low pressure, i.e. atmospheric pressure and below for water vapour and up to several bar for gases such as nitrogen, oxygen and argon, obey simple relations between their pressure, volume and temperature, with sufficient accuracy for engineering purposes. Such gases are called ideal . [Pg.4]

Kinetic theory A theory of matter based on the mathematical description of the relationship between pressures, volumes, and temperatures of gases (PVT phenomena). This relationship is summarized in the laws of Boyle s law, Charle s law, and Avogadro s law. [Pg.638]

Gay-Lussac measured how the temperature of a gas affects its pressure, volume, and density. The Italian scientist Amedeo Avogadro made a further contribution that established the relation between the volume and the amount of molecules in the sample and thereby helped to establish belief in the reality of atoms. [Pg.267]

To extend our model, we should note that, at low pressures at least, all gases respond in the same way to changes in pressure, volume, and temperature. Therefore, for calculations of the type that we are doing in this chapter, it does not matter whether all the molecules in a sample are the same. A mixture of gases that do not react with one another behaves like a single pure gas. For instance, we can treat air as a single gas when we want to use the ideal gas law to predict its properties. [Pg.277]

The ideal gas equation can be combined with the mole-mass relation to find the molar mass of an unknown gas PV = nRT (ideal gas equation) and n — (mole-mass relation) if we know the pressure, volume, and temperature of a gas sample, we can use this information to calculate how many moles are... [Pg.302]

These relationships interrelate the parameters pressure, volume and temperature with the Gibbs free energy of a system. It may be pointed out that the results embodied in these equations are applicable to closed systems only. [Pg.241]

The relationship between pressure, volume and temperature for fluids is described by equations of state. For example, if a gas is initially at a specified pressure, volume and temperature and two of the three variables are changed, the third variable can be calculated from an equation of state. [Pg.57]

Arts. From the pressure, volume, and temperature data, we can calculate the number of moles of gas present. From the number of moles and the mass, we can calculate the molecular weight. [Pg.201]

Combined gas law Amount (n) Pressure, volume, and temperature (K) (PiVO/Tj = (P2V2)/T2... [Pg.82]

Gas law experiments generally involve pressure, volume, and temperature measurements. In a few cases, other measurements such as mass and time are necessary. You should remember that AP, for example, is NOT a measurement the initial and final pressure measurements are the actual measurements made in the laboratory. Another common error is the application of gas law type information and calculations for non-gaseous materials. Typical experiments involving these concepts are numbers 3 and 5 in the Experimental chapter. [Pg.112]

The ideal gas law is a powerful tool that the chemist—and now you—can use to determine the molar mass of an unknown gas. By measuring the temperature, pressure, volume, and mass of a gas sample, you can calculate the molar mass of the gas. [Pg.54]

A typical use for this model would be to solve for the number of moles of a gas, given its identity, pressure, volume, and temperature. The iterative solver is used for this purpose. You must decide which variable to choose for iteration and what a reasonable initial guess is. Real gases approach ideal behavior at low pressure and moderate temperatures. Since the compressibility factor z is 1 for an ideal gas, and since knowing z along with P, V, and T allows a calculation of n, we choose z as the iteration variable and 1.0 as the initial guess. [Pg.114]

Fig. 1.4 Pressure-volume and enthalpy-entropy diagrams for rocket propulsion. Fig. 1.4 Pressure-volume and enthalpy-entropy diagrams for rocket propulsion.
Wannenburg T, Schulman SP, Burkhoff D. End-systolic pressure-volume and MV02-pressure-volume area relations of isolated rat hearts. Am. J. Physiol. 1992 262 H1287-93. [Pg.63]

The product may be analyzed by hydrolysis with excess 10% HC1 on a vacuum system. The ethane produced is passed through a trap held at-78° (Dry Ice), is condensed in another trap at -196° (liquid nitrogen), and finally is measured as a gas by pressure, volume, and temperature determination. [Pg.80]

The critical point is defined as that point for which both (< p/dV)T and (<92p/<92V2)T are zero the values of the pressure, volume, and temperature at this point - the critical constants - are designated by pc,Vc, and Tc, respectively. [Pg.195]

Such a diagram is presented in Fig 4.1-1, p 238 of Ref 3. The adjective "critical is also applied to temperature, pressure, volume and density existing at that point (Ref 1, p 269). Methods for determining critical point on the "critical isotherm are given in Ref 3, pp 357-63 (See also under "Corresponding States and under "Critical Phenomena )... [Pg.202]


See other pages where Pressure and Volume is mentioned: [Pg.248]    [Pg.438]    [Pg.443]    [Pg.36]    [Pg.956]    [Pg.576]    [Pg.629]    [Pg.633]    [Pg.134]    [Pg.229]    [Pg.11]    [Pg.248]    [Pg.288]    [Pg.508]    [Pg.330]    [Pg.454]    [Pg.318]    [Pg.318]    [Pg.157]    [Pg.21]    [Pg.22]    [Pg.19]    [Pg.107]    [Pg.39]    [Pg.106]   
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Atomization air pressures and volumes

Boyles Law Pressure and Volume

Changes in Volume and Pressure

Effects of Volume and Pressure Changes

Free Volume and the Pressure

Heat Capacity, Thermal Conductivity and Pressure—Volume—Temperature of PLA

Measurement of mass, volume, and pressure

Molar volume at standard temperature and pressure

Molar volume vapor pressure and

Pressure Effects and the Volume of Activation

Pressure and volume, changes

Pressure molar volume and temperature

Temperature Derivatives of Pressure and Volume

The Combined Gas Law Pressure, Volume, and Temperature

The Ideal Gas Law Pressure, Volume, Temperature, and Moles

The Relationship Between Volume and Pressure Boyles Law

Volume and Pressure as Fundamental Variables Bulk Modulus

Volume at Standard Temperature and Pressure

Volume, pressure and temperature

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