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Thermodynamic relationships

Thermodynamic relationships between thermoelectric E.M.F., Thomson effect, and Peltier effect. [Pg.367]

Since electrical energy can be converted at will into mechanical energ , a thermoelectric current, is capable of doing work at the expense of the heat which is supplied from the outside to the circuit at the hot junction (E E. In his classical thermodynamical theory W. Thomson assumed that the thermoelectrical phenomena were strictly reversible, except for the production of Joule heat, which becomes negligible as the current strength approaches zero. In this limiting case, therefore, the heat produced or absorbed at the junctions is equal [Pg.367]

By the first law the electrical energy produced is equal to the heat absorbed less the heat given out, i.e. [Pg.368]

By the second law the ratio of the amount of heat transformed into work to the total heat absorbed by the system is equal to the ratio of the difference in temperature to the temperature of the hot junction. [Pg.368]

Neglecting crgdT in comparison with the finite amount of heat [Pg.368]

The first law of thermodynamics states that for a closed system the enthalpy change AH is  [Pg.76]

Under constant volume conditions A(PF) = VAP, the work due to change of pressure. For electrochemical systems where changes in kinetic and potential energy are small  [Pg.76]

Depending on the sign of AS, AH can be smaller or larger than AG. For example, in the electrolysis of water (see Example 2.9), the overall reaction  [Pg.77]

As we said at the beginning of this section, an energy balance of the process is essential. A major user of energy is the electrochemical reactor, which will be considered next. [Pg.77]

From the If constant, estimated graphically from the Vanselow exchange selectivity coefficient, a number of thermodynamic parameters can be estimated. For example, [Pg.223]

from Keq, the standard enthalpy of exchange, AH° can be calculated (Table 4.2) using the van t Hoff equation  [Pg.224]

Based on Reaction 4.70 one may observe the requirements of AS0 and AH0 in order for K 1, or for the reactants in their standard state to be converted spontaneously to their products in their standard state. If AH0 is negative and AS0 is positive, the reaction will be spontaneous. If, on the other hand, AH° is positive and AS0 is negative, the reaction will not be spontaneous. Finally, if AH0 and AS0 have the same sign, the reaction may or may not be spontaneous, depending on the magnitude of AS0, AH0, and temperature (see Daniels and Alberty, 1975). [Pg.224]

To understand the behavior of Pb in soils, you need to understand how Pb partitions  [Pg.225]

The following arsenate (AsO -) adsorption data was obtained by adding 20.42 g of kaolinite to 200 mL of arsenate solution,  [Pg.225]

The use of the true volume of the liquid phase in the column as the void volume can lead to the principal difficulties in the interpretation of the retention of polar analytes that are also excluded from the contact with the adsorbent surface. The retention volume of these analytes will be lower than the column void volume, and thus their retention factors will be negative. A logarithm of negative retention factors does not exist that shows the applicability limit of the approximate theory described above. In a general sense the void volume should not change as a function of the type and organic composition. Table 2-1 demonstrates the compatibility of the void volume measured using different thermodynamically consistent methods. [Pg.49]

If we disengage ourselves from the consideration of mobile and stationary phases and assume (as a very rough approximation) that column void volume is the volume of the mobile phase = Yo) and leave stationary-phase volume [Pg.49]

TABLE 2-1. Void Volume Values Measured with MeCNAVater, MeOH/Water, and THF/Water aud a Deuterated Elueut Component for a Set of Columns Packed with Adsorbents Modified with Mono-alkylsilanes of Different Chain Length [Pg.49]

Source. Reprinted from reference 18, with permission. [Pg.49]

Application of the partitioning mechanism for the description of the retention process leads to another theoretical consequence applicable to ideal chromatographic systems that is, only one retention mechanism is present and no secondary equilibria effects are observed. Liquid chromatography is a competitive process, where analyte molecules compete with the eluent molecules for the retention on the stationary phase based on that, the standard state of [Pg.50]

If the process is conducted reversibly, dQ = TdS where S is the entropy of the elastic body. Substitution of this expression for dQ in Eq. (5) will require dW to represent the element of reversible work. In order to comply with this requirement, the coefficients P and / in Eq. (6) must be assigned their equilibrium values. In particular, / will henceforth represent the equilibrium tension for a given state of the system, which may be specified variously by aS, F, and L, by T, F, and L, or by T, P, and L. Then [Pg.440]

This equation expresses the differential of the free energy in terms of the differentials of the experimentally most convenient independent variables, P, T, and L, It follows from Eq. (8) that [Pg.440]

Since the second derivative obtained by differentiating dF/dL)r,p with respect to T at constant P and L is identical with that obtained by differentiating (dF/dT)p,L with respect to L at constant T and P, we obtain from Eqs. (9) and (11) [Pg.441]

Other forms of the elastic equation of state will appear below. [Pg.441]

Before proceeding further it is desirable to point out that dH/dL)T,p will differ indiscernibly from dE/dL)T,p in any likely application to rubberlike elastic phenomena. This may be seen by observing that the second term on the right-hand side of the relation [Pg.441]

The most important relationship governing mixtures of dissimilar components 1 and 2 is  [Pg.11]

Negative values of Eq. 2.2 (even though AGm 0) can yield an area of the phase diagram where the mixture will separate into a phase rich in component 1 and a phase rich in component 2. [Pg.11]

while liquid-hquid and polymer-solvent mixtures (that are borderline in miscibility) usually exhibit upper critical solution temperatures (ucst), polymer-polymer mixtures generally exhibit lower critical solution temperatures (lest). This behavior is illustrated in Fig. 2.1 with an illustration of the free energy composition at key temperatures noted in Fig. 2.2. The binodal and spinodal curves (binodal and spinodal phase separation processes are discussed later in this chapter) are illustrated on the phase diagrams. The spinodal curve is related to the position where [Pg.11]

The binodal curve is related to the equilibrium phase boundary between the single phase and the phase separated region. In a binary system, this is related to the chemical potentials of an individual component being equal in both phases as expressed by the following relationships  [Pg.12]


Other thermodynamic relationships are developed during the course of this... [Pg.49]

A very important thermodynamic relationship is that giving the effect of surface curvature on the molar free energy of a substance. This is perhaps best understood in terms of the pressure drop AP across an interface, as given by Young and Laplace in Eq. II-7. From thermodynamics, the effect of a change in mechanical pressure at constant temperature on the molar h ee energy of a substance is... [Pg.53]

The preceding material of this section has focused on the most important phenomenological equation that thermodynamics gives us for multicomponent systems—the Gibbs equation. Many other, formal thermodynamic relationships have been developed, of course. Many of these are summarized in Ref. 107. The topic is treated further in Section XVII-13, but is worthwhile to give here a few additional relationships especially applicable to solutions. [Pg.76]

If the dependence on temperature as well as on composition is known for a solution, enthalpies and entropies of adsorption may be calculated from the appropriate thermodynamic relationships [82]. Neam and Spaull [147] have, for example, calculated the enthalpies of surface adsorption for a series of straight-chain alcohols. They find an increment in enthalpy of about 1.96 kJ/mol per CH2 group. [Pg.91]

The variation of the integral capacity with E is illustrated in Fig. V-12, as determined both by surface tension and by direct capacitance measurements the agreement confrrms the general correctness of the thermodynamic relationships. The differential capacity C shows a general decrease as E is made more negative but may include maxima and minima the case of nonelectrolytes is mentioned in the next subsection. [Pg.200]

Interestingly, a general thermodynamic relationship allows the surface area of a porous system (without ink bottles) to be calculated from porosimetry data, note Section XVII-16B. The equation is [45]... [Pg.580]

Brunauer and co-workers [211, 212] proposed a modelless method for obtaining pore size distributions no specific capillary shape is assumed. Use is made of the general thermodynamic relationship due to Kiselev [213]... [Pg.667]

Fig. 9. Brayton cycle, where A = compressor inlet, B = combustor inlet, C = power turbine inlet, and D = exhaust (a) thermodynamic relationships and... Fig. 9. Brayton cycle, where A = compressor inlet, B = combustor inlet, C = power turbine inlet, and D = exhaust (a) thermodynamic relationships and...
Properties of steam can be divided iato thermodynamic, transport, physical, and chemical properties. In addition, the molecular stmcture and chemical composition of steam are of iaterest. It was at the start of iadustrialization, ca 1763, that thermodynamic relationships were first measured by Watt. A century later, ia 1859, Rankiae pubUshed his Manual of the Steam Engine, which gave a practical thermodynamic basis for the design and performance of steam engines. [Pg.350]

Thermodynamic Relationships. A closed container with vapor and liquid phases at thermodynamic equiUbrium may be depicted as in Figure 2, where at least two mixture components ate present in each phase. The components distribute themselves between the phases according to their relative volatiUties. A distribution ratio for mixture component i may be defined using mole fractions ... [Pg.156]

SemiempiricalRelationships. Exact thermodynamic relationships can be approximated, and the unknown parameters then adjusted or estimated empirically. The virial equation of state, tmncated after the second term, is an example of such a correlation (3). [Pg.232]

This chapter presents some basic thermodynamic relationships that apply to all compressors. Equations that apply to a particular type of compressor will be covered in the chapter addressing that compressor. In most cases, the derivations will not be presented, as these are available in the literature. The references given are one possible source for additional background information. [Pg.14]

For practical applications of the numerous thermodynamic relationships, it is necessary to have available the properties of the system. In general, a given property of a pure substance can be expressed in terms of any other two properties to completely define the state of the substance. Thus one can represent an equation of state by the functional relationship ... [Pg.223]

Nemst Equation the thermodynamic relationship between the equilibrium potential of an electrochemical reaction and the activities of the species involved in that reaction. [Pg.1370]

The temperature coefficient of the reaction free energy follows, through thermodynamic relationships [7], by partial differentiation of Eq. (15) ... [Pg.12]

Selectivity of sorption of organic ions by crosslinked polyelectrolytes in competition with small ions, in particular with metal ions, should be considered on the basis of the analysis of thermodynamic relationships of ion exchange. [Pg.17]


See other pages where Thermodynamic relationships is mentioned: [Pg.76]    [Pg.79]    [Pg.314]    [Pg.153]    [Pg.155]    [Pg.248]    [Pg.253]    [Pg.47]    [Pg.786]    [Pg.212]    [Pg.910]    [Pg.233]    [Pg.3]    [Pg.105]    [Pg.107]    [Pg.109]    [Pg.111]    [Pg.113]    [Pg.115]    [Pg.117]    [Pg.119]    [Pg.121]    [Pg.123]    [Pg.123]    [Pg.125]    [Pg.127]    [Pg.129]    [Pg.131]    [Pg.133]    [Pg.135]    [Pg.137]    [Pg.139]    [Pg.141]    [Pg.143]   
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