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Temperatures variations

Thus from an adsorption isotherm and its temperature variation, one can calculate either the differential or the integral entropy of adsorption as a function of surface coverage. The former probably has the greater direct physical meaning, but the latter is the quantity usually first obtained in a statistical thermodynamic adsorption model. [Pg.645]

Temperature variations are found by the solution of the energy equation. I he finite element scheme used in this example is based on the implicit 0 time-stepping/continuous penalty scheme described in detail in Chapter 4, Section 5. [Pg.145]

From the third law of thermodynamics, the entiopy 5 = 0 at 0 K makes it possible to calculate S at any temperature from statistical thermodynamics within the hamionic oscillator approximation (Maczek, 1998). From this, A5 of formation can be found, leading to A/G and the equilibrium constant of any reaction at 298 K for which the algebraic sum of AyG for all of the constituents is known. A detailed knowledge of A5, which we already have, leads to /Gq at any temperature. Variation in pressure on a reacting system can also be handled by classical thermodynamic methods. [Pg.322]

Phenyl groups impart resistance to temperature variations, flexibility under heat, resistance to abrasion, and compatibility with organic products. [Pg.1023]

The accuracy and precision of FIA are comparable to that obtained by conventional methods of analysis. The precision of a flow injection analysis is influenced by variables that are not encountered in conventional methods, including the stability of the flow rate and the reproducibility of the sample s injection. In addition, results from FIA may be more susceptible to temperature variations. These variables, therefore, must be carefully controlled. [Pg.658]

Temperature variation is not only easy to implement experimentally, but is also more familiar to chemists than the frequency of mechanical oscillations. [Pg.182]

Figure 4.15 Geometrical representation of the temperature variation of the actual volume (solid line) and the occupied volume (broken line). The shaded difference indicates the free volume which decreases to a critical value at T . Figure 4.15 Geometrical representation of the temperature variation of the actual volume (solid line) and the occupied volume (broken line). The shaded difference indicates the free volume which decreases to a critical value at T .
We noted above that the presence of monomer with a functionality greater than 2 results in branched polymer chains. This in turn produces a three-dimensional network of polymer under certain circumstances. The solubility and mechanical behavior of such materials depend critically on whether the extent of polymerization is above or below the threshold for the formation of this network. The threshold is described as the gel point, since the reaction mixture sets up or gels at this point. We have previously introduced the term thermosetting to describe these cross-linked polymeric materials. Because their mechanical properties are largely unaffected by temperature variations-in contrast to thermoplastic materials which become more fluid on heating-step-growth polymers that exceed the gel point are widely used as engineering materials. [Pg.314]

Equation (6.32) allows us to conveniently assess the effect of temperature variation on the rate of polymerization. This effect is considered in the following example. [Pg.367]

Finally we recognize that a 1°C temperature variation can be approximated as dT and that (dRp/Rp) X 100 gives the approximate percent change in the rate of polymerization. Taking average values of E from the appropriate tables, we obtain E j = 145, E = 16.8, and Ep = 24.9 kJ mol . For thermally initiated polymerization... [Pg.368]

The proviso all other things being equal in discussing the last point clearly applies to temperature as well, since the kinetic constants are highly sensitive to temperature. To evaluate the effect of temperature variation on the molecular weight of an addition polymer, we follow the same sort of logic as was used in Example 6.3 ... [Pg.370]

This alternative notation is especially suited to describe changes in solvent goodness which arise from temperature variations for a fixed system. By contrast, the x notation is more descriptive of different solvents at a single temperature. [Pg.565]

Thermographic Sensitivity. The noise equivalent temperature difference (sensitivity to scene temperature variations ia degrees C) maybe expressed ia terms of the NEP ... [Pg.291]

Nonvolatile Solvents. In practice, some gases tend to Hberate such large amounts of heat when they are absorbed into a solvent that the operation caimot be assumed to be isothermal, as has been done thus far. The resulting temperature variations over the tower will displace the equiUbrium line on 2tj—x diagram considerably because the solubiUty usually depends strongly on temperature. Thus nonisothermal operation affects column performance drastically. [Pg.28]

Snap-Fit and Press-FitJoints. Snap-fit joints offer the advantage that the strength of the joint does not diminish with time because of creep. Press-fit joints are simple and inexpensive, but lose hoi ding power. Creep and stress relaxation reduce the effective interference, as do temperature variations, particularly with materials with different thermal expansions. [Pg.370]

Natural gas production and transmission systems are complemented by underground storage systems. These systems provide the capabdity to respond to short-term gas demands which exceed the immediate production levels or transmission capabdities. They also provide an opportunity to sustain some production by refilling the storage areas when seasonal temperature variations lead to periods of reduced gas demand. In the United States in 1990, there were 397 storage pools having a combined capacity of 2.2 x 10 (1). [Pg.173]

Continuous recuperative furnaces employing metallic recuperators (heat exchangers) have been in use since the 1940s. Operation of these furnaces is simplified and the combustion process is more precisely controlled no reversal of air flow causes temperature variations. The recuperator metal must be caretiiUy selected because of chemical attack at high temperature. Recuperative furnaces are often used in the production of textile fiber glass because they maintain a constant temperature. [Pg.306]

The experimentally measured dependence of the rates of chemical reactions on thermodynamic conditions is accounted for by assigning temperature and pressure dependence to rate constants. The temperature variation is well described by the Arrhenius equation. [Pg.513]

Scanning thermal microscopy uses the world s smallest thermometer, actually a tiny thermocouple tip, to measure temperature variations as small as 10 microdegrees on a scale of <100 nm. [Pg.333]

Propylene oxide is a colorless, low hoiling (34.2°C) liquid. Table 1 lists general physical properties Table 2 provides equations for temperature variation on some thermodynamic functions. Vapor—liquid equilibrium data for binary mixtures of propylene oxide and other chemicals of commercial importance ate available. References for binary mixtures include 1,2-propanediol (14), water (7,8,15), 1,2-dichloropropane [78-87-5] (16), 2-propanol [67-63-0] (17), 2-methyl-2-pentene [625-27-4] (18), methyl formate [107-31-3] (19), acetaldehyde [75-07-0] (17), methanol [67-56-1] (20), ptopanal [123-38-6] (16), 1-phenylethanol [60-12-8] (21), and / /f-butanol [75-65-0] (22,23). [Pg.133]

Fig. 2. Slow oxidation, spontaneous ignition, and explosion as a function of pressure and temperature variations in hydrocarbon mixtures (1). Fig. 2. Slow oxidation, spontaneous ignition, and explosion as a function of pressure and temperature variations in hydrocarbon mixtures (1).
To a good approximation, thermal conductivity at room temperature is linearly related to electrical conductivity through the Wiedemann-Eran2 rule. This relationship is dependent on temperature, however, because the temperature variations of the thermal and the electrical conductivities are not the same. At temperatures above room temperature, thermal conductivity of pure copper decreases more slowly than does electrical conductivity. Eor many copper alloys the thermal conductivity increases, whereas electrical conductivity decreases with temperature above ambient. The relationship at room temperature between thermal and electrical conductivity for moderate to high conductivity alloys is illustrated in Eigure 5. [Pg.222]

Because there are many other properties that also are important, coatings cannot be selected only on this basis. The mechanical and chemical properties of the coating, change of properties with temperature, dielectric and adhesion properties, and particulady the cost of fabrication are all important parameters. Coatings can also be used to transport heat created away from a component and keep the component functioning as designed, or to protect a component from temperature variations in the environment. [Pg.123]

A given enzyme may be assayed by its action on soluble substrates under chemical and physical conditions different from those encountered in a real-life wash. Such experiments indicate the enzyme s performance with respect to pH and temperature variations, or in conjunction with other soluble substances, etc. The analytical data thus obtained are not necessarily representative of the wash performance of the enzyme, and real wash trials are necessary to evaluate wash performance of detergent enzymes. [Pg.293]

An extensive coverage of the general pressure and temperature variation of thermal conductivity is given in the monograph by Vargaftik,... [Pg.362]

Treatment of radiative transfer in combustion chambers is available at varying levels of complexity, including allowance for temperature variation in both gas and refractory walls (Hottel and Sarofim,... [Pg.586]

The equations for nozzle flow, Eqs. (6-114) through (6-118), remain valid for the nozzle section even in the presence of the discharge pipe. Equations (6-116) and (6-120), for the temperature variation, may also be used for the pipe, with Mo, po replacing Mi, pi since they are valid for adiabatic flow, with or without friction. [Pg.650]


See other pages where Temperatures variations is mentioned: [Pg.813]    [Pg.163]    [Pg.100]    [Pg.83]    [Pg.200]    [Pg.201]    [Pg.204]    [Pg.245]    [Pg.250]    [Pg.535]    [Pg.389]    [Pg.353]    [Pg.155]    [Pg.182]    [Pg.222]    [Pg.59]    [Pg.61]    [Pg.71]    [Pg.383]    [Pg.115]    [Pg.476]    [Pg.400]    [Pg.476]    [Pg.579]   
See also in sourсe #XX -- [ Pg.68 ]

See also in sourсe #XX -- [ Pg.187 ]

See also in sourсe #XX -- [ Pg.15 ]




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Activation energy, definition variation with temperature

Activity temperature variation

Activity variation with temperature

Affinity with temperature, variation

Analytic methods variation with temperature

Anderson variation with temperature

Association temperature variation

Atomic force microscopy temperature variation

Axial Variation of Fuel, Clad, and Coolant Temperatures

Axial variation of temperature

Benzene vapor pressure, variation with temperature

Blocking temperature, variation with

Body temperature variation

Bond valence variations, high temperature

Cell potential variation with temperature

Chemical shifts, temperature variation

Chemiluminescence temperature variations

Climatic temperature variations

Climatic temperature variations assumed

Conductivity variation with temperature

Daily and annual variations in ambient air wet-bulb temperatures

Density variation with temperature

Deposition temperature, variation

Deposition zone temperature variation

Dielectric constant 2 temperature variation

Diethyl ether variation with temperature

Diffusion coefficient temperature variation

Diffusion coefficient variation with temperature

Diffusion temperature variation

Diffusivity variation with temperature

Dipole temperature variation

Dissipation temperature variation

Dynamic moduli variation with temperature

Electrical conductivity temperature variation

Electrical conductivity variation with temperature

Electrical resistivity variation with temperature, metals

Electrons temperature variation

Energy landscape temperature variations

Enthalpy change variation with temperature

Enthalpy variation with temperature

Entropy variation with temperature

Equilibrium constant variation with temperature

Equilibrium constant, temperature variation

Equilibrium variation with temperature

Error temperature variation

Examples of modulus variations versus temperature for an amorphous and a semicrystalline thermoplastic

Exchange rate constant temperature variation

Flow path temperature variations

Fluid properties variation with temperature

Free energy variation with temperature

Fuel cells stack temperature variations

Fugacity temperature variation

Gibbs energy variation with temperature

Gibbs free energy variation with temperature

Glass transition temperature compositional variation

Heat capacity variation with temperature

Hydrogen bonding temperature, variation

Immiscibility variation with temperatur

Internal energy variation with temperature

Ionization constants variation with temperature

Liquid Surface Tension Variation by Temperature

Liquid viscosities variation with temperature

Liquids analysis temperature variations effect

Liquids variation with temperature

Magnetic hyperfine field variation with temperature

Maxwell distribution variation with temperature

Melting temperature variations

Mercury, temperature variations

Mixtures temperature variations

Mobility variation with temperature

Multilayer temperature variation

Oven temperature, variations

Packed columns temperature variation

Periodic temperature variations

Plateau Variation with temperature

Polarization variation with temperature

Power temperature variations

Prediction viscosity variation with temperature

Product variation with temperature

Propagation constant, variation with temperature

Quadrupole splitting temperature variation

Rate coefficient temperature variation

Reaction enthalpy, variation with temperature

Reaction rate variation with temperature

Relative permittivity variation with temperature

Resistance variation with temperature

Retention variation with temperature

Saturation state variation with temperature

Seasonal temperature variations

Solubility temperature variation

Solubility variation with temperature

Spectral moment temperature variation

Stability constants temperature, variation with

Standard Gibbs energy change variation with temperature

Standard enthalpy change variation with temperature

Standard entropy change variation with temperature

Standard potential variation with temperature

Subject Variation with temperature

Surface energy temperature variation

Surface tension variation with temperature

Temperature Gibbs energy variation

Temperature Variation and Intrinsic Diffusion

Temperature Variation in a Neutral Atmosphere

Temperature Variation of Paramagnetism

Temperature Variation of the Diffusion Coefficient

Temperature and Pressure Variation

Temperature variation and vibration isolation

Temperature variation, normalised

Temperature variation. Activation energy

Temperature, surface variation

The Variation of Reaction Enthalpy with Temperature

The Variation of Vapor Pressure with Temperature

The effect of temperature variations

The variation of Gibbs energy with temperature

The variation of Newtonian viscosity with temperature

The variation of entropy with temperature

Thermal utilization variation with temperature

Thermoplastics temperature variations

Transient regimes temperature variation

Vapor pressure variation with temperature

Vapour pressure variation with temperature

Variation of Dynamic Moduli with Strain Amplitude (at Constant Frequency and Temperature)

Variation of Free Energy with Temperature

Variation of Friction with Life for an In-Situ Film at Different Temperatures

Variation of Temperature

Variation of glass transition temperature with

Variation of the gyration swelling with temperature

Variation of the screening length with temperature

Variation with temperature

Variation with temperature chemical equilibrium

Variation with temperature rate constant

Variations in Temperature and Concentration

Variations in temperature

Viscosity variation with temperatur

Viscosity variation with temperature

Volume variation with temperature

Water density, variation with temperature

Water vapor pressure, variation with temperature

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