Big Chemical Encyclopedia

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

Articles Figures Tables About

Dependence on temperature and pressure

Sihcon nitride can be heated ia air up to 1450—1550°C. In nitrogen, inert gas, or reducing atmosphere, Si N can be heated up to 1750°C. Above 1750°C, decomposition and sublimating evaporation become severe. When in the presence of carbon, however, Si N stabiUty depends on temperature and pressure. The equiUbrium temperature for the reaction... [Pg.53]

Compressibility of Natural Gas All gases deviate from the perfect gas law at some combinations of temperature and pressure, the extent depending on the gas. This behavior is described by a dimensionless compressibility factor Z that corrects the perfect gas law for real-gas behavior, FV = ZRT. Any consistent units may be used. Z is unity for an ideal gas, but for a real gas, Z has values ranging from less than 1 to greater than 1, depending on temperature and pressure. The compressibihty faclor is described further in Secs. 2 and 4 of this handbook. [Pg.2366]

A variety of elements in different geometric forms, e.g. wire, tube and strip, corresponding to the commercial metals and alloys used in the process plant, are available. Also a variety of casings or housings are available depending on temperature and pressure requirements (Figs 19.53 and 19.54). [Pg.1136]

It is well known that biopolymers adsorbed water during dry storage and its quality depends on water content. For example the length of keratin depends on water content and therefore it is used as a hygrometer. The amount of adsorbed water depends on temperature and pressure of water vapor. [Pg.95]

Following this, elastomers can be swollen by some high-pressure gases (especially CO2) as the densities of these gases approach liquid-like levels, at appropriate temperatures they become supercritical fluids which possess a solubility parameter magnitudes that, however, are highly dependent on temperature and pressure... [Pg.645]

The stable phase of a substance depends on temperature and pressure. A phase diagram is a map of the pressure-temperature world showing the phase behavior of a substance. As Figure 11-38 shows, a phase diagram is aP-r graph that shows the ranges of temperature and pressure over which each phase is stable. Pressure is plotted along... [Pg.806]

Lanthanides with fractional valences have II, III and IV valences, as well as mixed II/III and III/IV valences. Depending on temperature and pressure, the degree of oxidation can change. This effect may result in a change in the different properties of nanoparticles, such as the stability, heat capacity, conductivity and magnetic susceptibility [218]. Valence fluctuation phenomena have been reported to occur... [Pg.255]

Equilibrium constants are also dependent on temperature and pressure. The temperature functionality can be predicted from a reaction s enthalpy and entropy changes. The effect of pressure can be significant when comparing speciation at the sea surface to that in the deep sea. Empirical equations are used to adapt equilibrium constants measured at 1 atm for high-pressure conditions. Equilibrium constants can be formulated from solute concentrations in units of molarity, molality, or even moles per kilogram of seawater. [Pg.112]

Fig. 7 Reactions of toluene with HO radical. HO can abstract a benzylic hydrogen atom (a) or add to the aromatic ring at the ipso (b), ortho (c), meta (d), and para (e) positions relative to the methyl group. Each resultant radical can decompose by various pathways, depending on temperature and pressure. Fig. 7 Reactions of toluene with HO radical. HO can abstract a benzylic hydrogen atom (a) or add to the aromatic ring at the ipso (b), ortho (c), meta (d), and para (e) positions relative to the methyl group. Each resultant radical can decompose by various pathways, depending on temperature and pressure.
Carbon dioxide, as can most other substances, can exist in any one of three phases—solid, liquid, or gas—depending on temperature and pressure. At low temperatures, carbon dioxide exists as a solid ("dry ice") at almost any pressure. At temperatures greater than about -76°F (-60°C), however, carbon dioxide may exist as a gas or as a liquid, depending on the pressure. At some combination of temperature and pressure, however, carbon dioxide (and other substances) enters a fourth phase, known as the supercritical phase, whose properties are a combination of gas and liquid properties. For example, supercritical carbon dioxide (often represented as SCC02, SC-C02, SC-CO2, or a similar acronym) diffuses readily and has a low viscosity, properties associated with gases, but is also a good solvent, a property one often associates with liquids. The critical temperature and pressure at which carbon dioxide becomes a supercritical fluid are 31.1°C (88.0°F) and 73.8 atm (1,070 pounds per square inch). [Pg.204]

Diffusion coefficients vary widely, depending on temperature, pressure, the type of the phase, and the composition of the phase. The dependence on temperature and pressure can be described well by the Arrhenius relation including a pressure term (Equation 1-88) ... [Pg.284]

Electrons in nonpolar liquids are either in the conduction band, trapped in a cavity in the liquid, or in special cases form solvent anions. The energy of the bottom of the conduction band is termed Vq. Vq has been measured for many liquids and its dependence on temperature and pressure has also been measured. New techniques have provided quite accurate values of Vq for the liquid rare gases. The energies of the trapped state have also been derived for several liquids from studies of equilibrium electron reactions. A characteristic of the trapped electron is its broad absorption spectrum in the infrared. [Pg.175]

The deformation potential model seems to provide a suitable framework to understand the quasi-free electron mobility in nonpolar liquids. Already several extensions or modifications on this theory have been proposed, and the dependence on temperature and pressure seems to be adequately explained. However, several authors have taken dilferent approaches to the problem showing that a consensus in our understanding has not yet been reached. [Pg.197]

A table of crystal structures for the elements can be found in Table 1.11 (excluding the Lanthanide and Actinide series). Some elements can have multiple crystal structures, depending on temperature and pressure. This phenomenon is called allotropy and is very common in elemental metals (see Table 1.12). It is not unusual for close-packed crystals to transform from one stacking sequence to the other, simply through a shift in one of the layers of atoms. Other common allotropes include carbon (graphite at ambient conditions, diamond at high pressures and temperature), pure iron (BCC at room temperature, FCC at 912°C and back to BCC at 1394°C), and titanium (HCP to BCC at 882°C). [Pg.38]

The solubility of a solid-solution component varies depending on temperature and pressure. [Pg.146]

Depending on temperature and pressure, the behaviour of a supercritical fluid is sometimes similar to that of a gas and sometimes similar to that of a liquid. [Pg.95]

The closing pressure for the mold for making uniform foams may be obtained by knowing precisely how the volume of this gel depends on temperature and pressure. [Pg.134]

Figure 3.2 illustrates the relatively complex nature of the compressibility factor s dependence on temperature and pressure. It is evident that there can be very substantial departures from ideal-gas behavior. Whenever possible, it is useful to represent the equation of state as an algebraic relationship of pressure, temperature, and volume (density). Certainly, when applied in computational modeling, the benefits of a compact equation-of-state representation are evident. There are many ways that are used to accomplish this objective [332], most of which are beyond our scope here. [Pg.73]

The definition of phase can be carried further. Depending on temperature and pressure, solids can take on different crystalline forms. These constitute separate phases. The petroleum engineer normally is not concerned with the crystalline forms of solids therefore, we will consider only three phases gas, liquid, and solid. For the purpose of our discussion we will use the words vapor and gas interchangeably. Some authors try to distinguish between these two words, but the difference is unimportant to us. [Pg.46]

The equilibrium crystallographic form of ice depends on temperature and pressure. A phase diagram showing some of these is shown in Figure 6.9. [Pg.49]

Equilibrium between various components of the hydrospheric carbonate system depends on temperature and pressure, a combination of which correlates with pH so that, at a given temperature and pressure, equilibrium is only a function of pH = —lg[H+]. The effect of temperature on pH in the first approximation can be described by the equation (Ivanov, 1978), ApH= —0.0111AT, valid when pH e[7.5, 8.4], T e [1-30]°C, and salinity from 10%o to 40%o. The dependence of pH on pressure pc follows the dependence, pH = dApc, where, on average, d = —0.0254. A more accurate presentation of this law is given in Table 3.5. [Pg.170]

Grunze and Hirschwald [15] developed a vacuum micro thermobalance with cold fingers and studied the reduction of ZnO by H2 and CO in the temperature range 450—1000°C. By making sure that the reaction products, Zn and C02 or H20, were removed to cold traps as fast as they formed, they were able to measure the intrinsic surface reaction rates. The reaction order, n, depended on temperature and pressure for T> 700°C and p < 1 torr, n 1 and for T< 500°C and p > 1 torr, n 0.2 [16]. [Pg.127]

Procedure of creation of the heat machine based on periodic circulation of hydrogen and increase in the efficiency its operation demands the detailed information on methods of calculation equilibrium P-C-T (pressure - concentration - temperature) of characteristics, thermodynamic, thermalphysic (factors of specific heat conductivity X and heat transfers a depending on temperature and pressure) and kinetic properties of hydrides. Approach to designing HHP as to an individual kind of HHM can be broken on three part [1] ... [Pg.384]

Many organic chemicals exist in two or more crystalline forms, which are referred to as polymorphs. The preferred crystalline form depends on temperature and pressure however, multiple polymorphic forms can exist under identical temperature and pressure conditions. Generally, there is one stable form at any particular temperature and pressure, but one or more metastable forms may be produced under different experimental conditions. Typically, the conditions leading to different polymorphs include solvents, seeding, and external influences during precipitation. Often a desired polymorph can be produced from solution by initiating the nucleation with seeds of the desired polymorph. A metastable polymorph may convert to the stable form, but external influences may be required to increase the rate of the conversion. [Pg.239]


See other pages where Dependence on temperature and pressure is mentioned: [Pg.1115]    [Pg.326]    [Pg.209]    [Pg.319]    [Pg.7]    [Pg.58]    [Pg.160]    [Pg.187]    [Pg.704]    [Pg.706]    [Pg.495]    [Pg.75]    [Pg.30]    [Pg.230]    [Pg.274]    [Pg.61]    [Pg.116]    [Pg.75]    [Pg.26]    [Pg.169]    [Pg.91]    [Pg.87]    [Pg.696]   


SEARCH



Dependence of Model Parameters on Pressure and Temperature

Dependence of Vapor Fugacity on Temperature, Pressure, and Composition

Dependence on pressure

Dependence on temperature

Dependence on temperature and

Dependence on temperature and oxygen pressure

Pressure and temperature dependence

Pressure dependence

Temperature and pressure dependency

Temperature pressure and

The dependence of vapour -solution equilibria on temperature and pressure

© 2024 chempedia.info