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Selected temperature coefficients for heat capacities

H2Se(g) 2.32030E+0I 3.23156E-02 - 8.89220E-06 3.05500E+02 I.46472E+05 298 1500 [Pg.63]

SeF2(g) 6.5060OE+0I - 3.94790E-03 8.I9000E-07 - 5.20470E+03 I.02790E+05 298 2000 [Pg.63]

SeFjfg) 1.22798E+02 - 8.48620E-03 1.763I0E-06 - I.I1220E+04 - 9.65900E+04 298 2000 [Pg.63]

SeFo(g) 1.96298E+02 -2.58210E-02 6.44800E-06 -2.57220E+04 6.70400E+05 298 1500 [Pg.63]

SeOF2(g) 9.67972E+01 - 7.47720E-03 1.49940E-06 - 1.1 1580E+04 5.38060E+05 298 2000 [Pg.63]


Table III-3 Selected temperature coefficients for heat capacities marked with in Table Ill-l according to the form C° T) = a + bT + cT +dT +eT. The functions are valid between the temperatures and Tmax (in K). The notation E nm indicates the power of 10. Units for C° are J-K" -mor. ... Table III-3 Selected temperature coefficients for heat capacities marked with in Table Ill-l according to the form C° T) = a + bT + cT +dT +eT. The functions are valid between the temperatures and Tmax (in K). The notation E nm indicates the power of 10. Units for C° are J-K" -mor. ...
Table 111-3 Selected temperature coefficients for heat capacities.58... Table 111-3 Selected temperature coefficients for heat capacities.58...
Table III-3 Selected temperature coefficients for heat capacities in the form -2, rp-2 functions are valid between the temperatures... Table III-3 Selected temperature coefficients for heat capacities in the form -2, rp-2 functions are valid between the temperatures...
Regulation 543-01-03 allows for the cross sectional area of the protective conductor to be calculated using the formula S= (I t)Vk. S is the cross sectional area in mm T is the fault current t is the operating time in seconds of the disconnecting device for a current off amps k is a factor that takes account of resistivity, temperature coefficient and heat capacity of the conductor material, and the appropriate initial and final temperatures. Alternatively, the size can readily be selected from Table 54G. There is a series of tables, 54B to 54F, which can be used to select the value of k for different types of conductor. [Pg.151]

The standard temperature selected for the values given in this book is 18° Centigrade, following the procedure of the thermochemistry section (Bichowsky1) of the International Critical Tables. The authors have been reluctant not to use the almost universally accepted standard temperature of 25° Centigrade for thermodynamic calculations but the selection of 18° as the standard temperature is practically necessary in this case because all of the monumental work of Julius Thomsen and of Marcellin Berthelot was done at or near 18° and there are not now available sufficient heat capacity data with which to make accurate conversion to 25° (this is especially important for reactions involving substances in aqueous solution where the temperature coefficient is usually very large). In later years, as the data on heat capacities become available, or as the heats of many of the reactions, which have until the present time been measured only by Thomsen or Berthelot or both, are redetermined, it will be quite feasible to use 25° as the standard temperature. [Pg.7]

For a numerical base case, the kinetic and process parameters given in Table 2.1 are selected. Reactors with several design values of conversion and over a range of temperatures are sized. The purpose is to see the effect of these parameters on the size of the reactor and its heat transfer area. The effects of changes in the base case parameters, such as feed flowrate, heat of reaction, and overall heat transfer coefficient, will also be explored. Densities and heat capacities are assumed to be constant. [Pg.34]

Chemical reactors are the most important features of a chemical process. A reactor is a piece of equipment in which the feedstock is converted to the desired product. Various factors are considered in selecting chemical reactors for specific tasks. In addition to economic costs, the chemical engineer is required to choose the right reactor that will give the highest yields and purity, minimize pollution, and maximize profit. Generally, reactors are chosen that will meet the requirements imposed by the reaction mechanisms, rate expressions, and the required production capacity. Other pertinent parameters that must be determined to choose the correct type of reactor are reaction heat, reaction rate constant, heat transfer coefficient, and reactor size. Reaction conditions must also be determined including temperature of the heat transfer medium, temperature of the inlet reaction mixture, inlet composition, and instantaneous temperature of the reaction mixture. [Pg.218]

In order to select materials that will maintain acceptable mechanical characteristics and dimensional stability one must be aware of both the normal and extreme thermal operating environments to which a product will be subjected. TS plastics have specific thermal conditions when compared to TPs that have various factors to consider which influence the product s performance and processing capabilities. TPs properties and processes are influenced by their thermal characteristics such as melt temperature (Tm), glass-transition temperature (Tg), dimensional stability, thermal conductivity, specific heat, thermal diffusivity, heat capacity, coefficient of thermal expansion, and decomposition (Td) Table 1.2 also provides some of these data on different plastics. There is a maximum temperature or, to be more precise, a maximum time-to-temperature relationship for all materials preceding loss of performance or decomposition. Data presented for different plastics in Figure 1.5 show 50% retention of mechanical and physical properties obtainable at room temperature, with plastics exposure and testing at elevated temperatures. [Pg.17]

This chapter presents the chemical thermodynamic data set for selenium species which has been selected in this review. Table lll-l contains the reeommended thermodynamic data of the selenium species, Table III-2 the recommended thermodynamic data of chemical equilibrium reactions by which the selenium compounds and complexes are formed, and Table III-3 the temperature coefficients of the heat capacity data of Table lll-lwhere available (see Appendix E for additional selenium data, cf. Section 11.7). [Pg.39]

Refractory oxides are an important class of materials that enable processes to exploit extreme environments. A wide variety of unary, binary, and ternary oxides can be considered refractory, based on their melting temperatures. Refractory oxides are generally prepared from powdered precursors using standard ceramic forming techniques such as casting, pressing, or extrusion, and subsequently sintered to achieve final density. In addition to chemical compatibility, the physical properties of refractory oxides such as thermal expansion coefficient, thermal conductivity, modulus of elasticity, and heat capacity must be considered when selecting an oxide for a specific application. [Pg.108]

Numerical calculations of phase equilibria require thermodynamic data or correlations of data. For pure components, the requisite data may include saturation pressures (or temperatures), heat capacities, latent heate, and volumetric properties. For mixtures, one requires a PVTx equation of state (for determination of d/), and/or an expression for the molar excess Gibbs energy (fw determination of yt). We have discussed in Sections 1.3 and 1.4 the correlating capabilities of selected equations of state and expressions for g, and the behavior of the fugacity coefficients and activity coefficients derived ftom them. [Pg.54]

The selection of the thermal management materials for electronic packaging purposes demands close examination of thermophysical characteristics, such as thermal conductivity and diffusivity, specific heat capacity, coefficient of thermal expansion, and thermal shock resistance. A variety of measurement techniques have been developed to evaluate these properties, but this chapter focuses on thermal conductivity and diffusivity evaluation methods. Each of them is suitable for a limited range of materials, depending on the thermal properties and the medium temperature. The precise determination of the thermal properties of bulk composite materials is challenging. For instance, loss terms for the heat input intended to flow through the sample usually exist and can be difficult to quantify. [Pg.200]

Example 5.7. If a parallel flow heat exchanger had been selected to cool the high-pressure gas stream in Example 5.6, determine the effectiveness of the heat exchanger, exit temperatures for the two fluids, and the heat-transfer rate for such an exchanger. Assume the same mass flow rates, same average heat capacities, and same exchanger area and overall heat-transfer coefficient as in Example 5.6. [Pg.223]


See other pages where Selected temperature coefficients for heat capacities is mentioned: [Pg.58]    [Pg.58]    [Pg.218]    [Pg.130]    [Pg.43]    [Pg.40]    [Pg.39]    [Pg.101]    [Pg.369]    [Pg.70]    [Pg.30]    [Pg.727]    [Pg.90]    [Pg.178]    [Pg.80]   


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Selective coefficient

Selective heating

Selectivity coefficient

Selectivity temperature

Temperature coefficient

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