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As a function of temperature

Figure 1 shows second virial coefficients for four pure fluids as a function of temperature. Second virial coefficients for typical fluids are negative and increasingly so as the temperature falls only at the Boyle point, when the temperature is about 2.5 times the critical, does the second virial coefficient become positive. At a given temperature below the Boyle point, the magnitude of the second virial coefficient increases with... [Pg.29]

P the other terms provide corrections which at low or moderate pressure are close to unity. To use Equation (2), we require vapor-pressure data and liquid-density data as a function of temperature. We also require fugacity coefficients, as discussed in Chapter 3. [Pg.40]

In typical situations, we do not have the necessary experimental data to find constants b... To obtain these constants, we need experimental vapor-liquid equilibria (i.e. activity coefficients) as a function of temperature. [Pg.88]

In Equation (15a), the first term h is found from Equation (5) where x s replace y s and the fugacities of the pure condensables are found as a function of temperature from Equation (16). The... [Pg.88]

Standard-state fugacities at zero pressure are evaluated using the Equation (A-2) for both condensable and noncondensable components. The Rackett Equation (B-2) is evaluated to determine the liquid molar volumes as a function of temperature. Standard-state fugacities at system temperature and pressure are given by the product of the standard-state fugacity at zero pressure and the Poynting correction shown in Equation (4-1). Double precision is advisable. [Pg.308]

The acentric factor can be determined as a function of temperature by finding the exact properties supplied by the DIPPR. [Pg.113]

This relation is used only for temperatures greater than 0°C. The average error is about 5 kJ/kg. Figure 4.5 gives the enthalpy for petroleum fractions whose is 11.8 as a function of temperature. For K, factors different from 11.8, a correction identical to that used for Cpi is used (to... [Pg.124]

In Mehrotra s method, the dynamic viscosity is expressed as a function of temperature according to the relation ... [Pg.128]

Solubility of water in jet fuels as a function of temperature (Jet A is a variant] of Jet Al, used in the USA for domestic flights. Jet A has a freezing point higher than that of Jet Al). ... [Pg.228]

Volatility is generally characterized by a distillation curve (the quantity distilled as a function of temperature). Often, only the initial and final boiling points are taken into account along with, possibly, a few intermediary points. [Pg.273]

The surface free energy can be regarded as the work of bringing a molecule from the interior of a liquid to the surface, and that this work arises from the fact that, although a molecule experiences no net forces while in the interior of the bulk phase, these forces become unbalanced as it moves toward the surface. As discussed in connection with Eq. Ill-IS and also in the next sections, a knowledge of the potential function for the interaction between molecules allows a calculation of the total surface energy if this can be written as a function of temperature, the surface free energy is also calculable. [Pg.56]

Barnes and Hunter [290] have measured the evaporation resistance across octadecanol monolayers as a function of temperature to test the appropriateness of several models. The experimental results agreed with three theories the energy barrier theory, the density fluctuation theory, and the accessible area theory. A plot of the resistance times the square root of the temperature against the area per molecule should collapse the data for all temperatures and pressures as shown in Fig. IV-25. A similar temperature study on octadecylurea monolayers showed agreement with only the accessible area model [291]. [Pg.148]

As a quite different and more fundamental approach, the isotherms of Fig. XI-10 allowed a calculation of X as a function of temperature. The plot of In K versus 1 /T gave an enthalpy quantity that should be just the difference between the heats of immersion of the Graphon in benzene and in n-heptane, or 2.6 x 10 cal/m [141]. The experimental heat of immersion difference is 2.4 x 10 cal/m, or probably indistinguishable. The... [Pg.411]

Fig. XVIII-27. Specific rates of CO oxidation on single crystal and supported catalysts as a function of temperature. (From Ref 308. Reprinted with permission from American Chemical Society, copyright 1988.)... Fig. XVIII-27. Specific rates of CO oxidation on single crystal and supported catalysts as a function of temperature. (From Ref 308. Reprinted with permission from American Chemical Society, copyright 1988.)...
Simple collision theories neglect the internal quantum state dependence of a. The rate constant as a function of temperature T results as a thennal average over the Maxwell-Boltzmaim velocity distribution p Ef. [Pg.776]

Midey A J and Viggiano A A 1998 Rate constants for the reaction of Ar" with O2 and CO as a function of temperature from 300 to 1400 K derivation of rotational and vibrational energy effects J. Chem. Phys. at press... [Pg.825]

The enthalpy of fomiation is obtained from enthalpies of combustion, usually made at 298.15 K while the standard entropy at 298.15 K is derived by integration of the heat capacity as a function of temperature from T = 0 K to 298.15 K according to equation (B 1.27.16). The Gibbs-FIehiiholtz relation gives the variation of the Gibbs energy with temperature... [Pg.1904]

The mechanical behaviour of a polymer as a function of temperature is summarized in figure C2.1.15. The... [Pg.2531]

Figure C2.1.15. Schematic representation of tire typicai compiiance of a poiymer as a function of temperature. (C) VOGEL-FULCHER AND WILLIAMS-LANDEL-FERRY EQUATIONS... Figure C2.1.15. Schematic representation of tire typicai compiiance of a poiymer as a function of temperature. (C) VOGEL-FULCHER AND WILLIAMS-LANDEL-FERRY EQUATIONS...
Figure C2.5.6. Thennodynamic functions computed for the sequence whose native state is shown in figure C2.5.7. (a) Specific heat (dotted curve) and derivative of the radius of gyration with respect to temperature dR /dT (broken curve) as a function of temperature. The collapse temperature Tg is detennined from the peak of and found to be 0.83. Tf, is very close to the temperature at which d (R )/d T becomes maximum (0.86). This illustrates... Figure C2.5.6. Thennodynamic functions computed for the sequence whose native state is shown in figure C2.5.7. (a) Specific heat (dotted curve) and derivative of the radius of gyration with respect to temperature dR /dT (broken curve) as a function of temperature. The collapse temperature Tg is detennined from the peak of and found to be 0.83. Tf, is very close to the temperature at which d (R )/d T becomes maximum (0.86). This illustrates...
A lustrous metal has the heat capacities as a function of temperature shown in Table 1-4 where the integers are temperatures and the floating point numbers (numbers with decimal points) are heat capacities. Print the curve of Cp vs. T and Cp/T vs. T and determine the entropy of the metal at 298 K assuming no phase changes over the interval [0, 298]. Use as many of the methods described above as feasible. If you do not have a plotting program, draw the curves by hand. Scan a table of standard entropy values and decide what the metal might he. [Pg.29]

To evaluate this integral, we must know Cv as a function of temperature, and usually this is not known. [Pg.321]

The heat capacity of thiazole was determined by adiabatic calorimetry from 5 to 340 K by Goursot and Westrum (295,296). A glass-type transition occurs between 145 and 175°K. Melting occurs at 239.53°K (-33-62°C) with an enthalpy increment of 2292 cal mole and an entropy increment of 9-57 cal mole °K . Table 1-44 summarizes the variations as a function of temperature of the most important thermodynamic properties of thiazole molar heat capacity Cp, standard entropy S°, and Gibbs function - G°-H" )IT. [Pg.86]

TABLE 1-44. VARIATION OF SOME THERMODYNAMIC PROPERTIES OF THIAZOLE AS A FUNCTION OF TEMPERATURE (29.3)... [Pg.86]

Table 5.24 Thermal Conductivities of Gases as a Function of Temperature 5.148... Table 5.24 Thermal Conductivities of Gases as a Function of Temperature 5.148...
TABLE 8.20 Potentials of Reference Electrodes in Volts as a Function of Temperature Liquid-junction potential included. [Pg.940]

A diblock copolymer, 71% polyisoprene (1) by weight and 29% polybutadiene (B), was blended in different proportions into a 71%-29% mixture of the individual homopolymers. The loss tangent was measured as a function of temperature for various proportions of copolymer. Two peaks are observed ... [Pg.183]

In this section and the last, we have examined the lattice model of the Flory-Huggins theory for general expressions relating AHj and ASj to the composition of the mixture. The separate components can therefore be put together to give an expression for AGj as a function of temperature and composition ... [Pg.524]

Fig. 7. Useful lifetime of Parylenes N, C, and D as a function of temperature in air. Failure = 50% loss in tensile strength. Fig. 7. Useful lifetime of Parylenes N, C, and D as a function of temperature in air. Failure = 50% loss in tensile strength.
Eig. 6. Decomposition of polymers as a function of temperature during heating. A, polymethylene B, polytetrafluoroethylene C, silicone D, phenoHc resin ... [Pg.6]


See other pages where As a function of temperature is mentioned: [Pg.211]    [Pg.219]    [Pg.262]    [Pg.393]    [Pg.190]    [Pg.267]    [Pg.828]    [Pg.1904]    [Pg.2501]    [Pg.2598]    [Pg.2882]    [Pg.2936]    [Pg.322]    [Pg.150]    [Pg.314]    [Pg.942]    [Pg.239]    [Pg.195]   


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Affinity as a function of temperature

ArG and K as Functions of Temperature

As function of temperature, Fig

Behavior as a function of temperature and pressure

Carbon as a function of temperature

Conductivity as a Function of Temperature

Conversion as a function of temperature

Defect Concentration as a Function of Temperature and Pressure

Density common fluids, as function of temperature

Density of Solvents as a Function Temperature

Density solvents, as function of temperature

Dielectric constant common fluids, as function of temperature

EMF as function of temperature

Enthalpy as a function of temperature

Enthalpy change as a function of temperature

Enthalpy common fluids, as function of temperature

Entropy as a function of pressure and temperature

Entropy as a function of temperature and volume

Entropy common fluids, as function of temperature

Equilibrium Compositions as Functions of Pressure and Temperature

Equilibrium SO2 Oxidized as a Function of Temperature

Equilibrium constant as function of temperature

Excess thermodynamic functions in the region of a critical solution temperature

Function of temperature

Growth rate as a function of temperature

Heat capacity common fluids, as function of temperature

Inorganic compounds solubility as a function of temperature

Minerals solubility as a function of temperature

Molar conductivity as a function of temperature and density

NMR measurements of reaction velocities and equilibrium constants as a function temperature

Permeability as a function of temperature

Polarization studies as a function of temperature

Proton Conductivity as a Function of Composition and Temperature

Reaction rate as a function of temperature

Solubility as a Function of Temperature and Henrys Constant at 25C for Gases in Water

Solubility as function of temperature

Solvents as a Function of Temperature

Sound velocity air, as function of temperature

Specific conductivity as a function of temperature, concentration and density

Strength as a function of temperature

Temperature as a function

Temperature as a function of reduced

Temperature atmosphere, as function of altitude

Temperature, N.M.R. measurements of reaction velocities and equilibrium constants as a function

Thermodynamic Properties as a Function of Temperature

Thermodynamic properties common fluids, as function of temperature

Two Phases at Equilibrium as a Function of Pressure and Temperature

Viscosity common fluids, as function of temperature

Viscosity, as a function of temperature

Weight as a function of temperature

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