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Nernst isotherm

Isotherms plot of distribution ratios K, that is, a plot of concentration of the component in the stationary phase versus concentration in the mobile phase. Isotherms represent the relative attraction of a solute for the stationary and mobile phases, the plot is linear for a symmetrical Gaussian peak, non linear isotherms lead to unsymmetrical peaks, e.g. peak fronting and tailing. Langmuir isotherms describe the equilibrium process in adsorption chromatography, Nernst isotherms relate to partition chromatography. [Pg.534]

Figure 19. Electrochemical isotherm for Ti () 5Zr0 5 V0 5 Ni,, Fe0 2 Mn 0 2. The /)( is calculated from the equilibrium voltage,, by the Nernst equation 156]. Figure 19. Electrochemical isotherm for Ti () 5Zr0 5 V0 5 Ni,, Fe0 2 Mn 0 2. The /)( is calculated from the equilibrium voltage,, by the Nernst equation 156].
This relationship led to an early formulation of the Third Law known as the Nernst heat theorem, which states that for any isothermal process... [Pg.164]

Adsorption Isotherms, Nernst Equation and Potential-Work Function Equivalence... [Pg.313]

In order to calculate the dilational contribution exactly a considerable quantity of data is needed. The temperature dependence of the volume, the iso-baric expansivity and the isothermal compressibility is seldom available from 0 K to elevated temperatures and approximate equations are needed. The Nernst-Lindeman relationship [7] is one alternative. In this approximation cP,m -Cv,m is given by... [Pg.246]

In order to transform eqns. (174) into more explicit expressions, use is made of (i) the Nernst equation, relating E, cQ and cR (ii) the general rule that any isotherm is of the form (3jCj = f(Pj) (iii) the thermodynamic relationship [144, 145]... [Pg.316]

The sorption of a weak electrolyte by a charged polymer membrane is another case where Nernst + Langmuir-like dual mode sorption, involving the undissociated and dissociated species respectively, may be expected. The concentration of each species in solution follows, of course, from the dissociation constant of the electrolyte. The sorption isotherms of acetic acid and its fluoroderivatives have been analysed in this manner, and the concentration dependence of the diffusion coefficient of acetic acid interpreted resonably successfully, using Nylon 6 as the polymer substrate 87). In this case the major contribution to the overall diffusion coefficient is that of the Nernst species consequently DT2 could not be determined with any precision. By contrast, in the case of HC1, which was also investigated 87 no Nernst sorption or diffusion component could be discerned down to pH = 2 and the overall diffusion coefficient obeyed the relation D = DT2/( 1 — >1D), which is the limiting form of Eq. (25) when p — 00. [Pg.114]

Factors leading to insolubility in water were discussed in Section 10.2.1.1. Provided they are not highly polymerized, such hydrophobic substances are generally soluble in non-aqueous solvents. In a two-phase system formed by an aqueous phase and a second phase immiscible with it a solute will partition between them until its activity is the same in both. The Nernst partition isotherm quantifies this relationship in the form... [Pg.538]

The Nernst partition isotherm applies to each individual species in an equilibrium mixture. The analyst is more directly concerned with the experimentally determinable distribution ratio, D, defined as... [Pg.538]

When two immiscible solvents are placed in contact, any substance soluble in both of them will distribute or partition between the two phases in a definite proportion. According to the Nernst partition isotherm, the following relationship holds for a solute partitioning between two phases a and b ... [Pg.46]

Isothermal chemistry in fuel cells. Barclay (2002) wrote a paper which is seminal to this book, and may be downloaded from the author s listed web site. The text and calculations of this paper are reiterated, and paraphrased, extensively in this introduction. Its equations are used in Appendix A. The paper, via an equilibrium diagram, draws attention to isothermal oxidation. The single equilibrium diagram brings out the fact that a fuel cell and an electrolyser which are the thermodynamic inverse of each other need, relative to existing devices, additional components (concentration cells and semi-permeable membranes), so as to operate at reversible equilibrium, and avoid irreversible diffusion as a gas transport mechanism. The equilibrium fuel cell then turns out to be much more efficient than a normal fuel cell. It has a greatly increased Nernst potential difference. In addition the basis of calculation of efficiency obviously cannot be the calorific value of the... [Pg.4]

Complete fuel cells are engineered for isothermal oxidation by the addition of perm-selective membranes and isothermal concentration cells. They would, if developed, generate much higher Nernst potential difference than an existing incomplete fuel cell. That would give a chance for fuel cells to draw level, a chance the industry does not seem to understand. [Pg.120]

In Figure A.4 water and methane, each proceeding from store, while being driven by circulators via perm-selective membranes, are reacted isothermally in a notional and conceptually quite new isothermal reformer resembling a fuel cell bounded by perm-selective membranes. The circulators are isothermal concentration cells with Nernst potential differences. [Pg.165]

The flow sheet in Figure A.6 then requires the addition of isothermal concentration cells to give their contribution to the power, and increase the Nernst potential difference. These would be immediately adjacent to the fuel cell in the methane and oxygen supply lines. The rearranged flow sheet is shown as Figure A.7. [Pg.167]

I he simplest is the partition of a solute between two immiscible solvents. In this case [0] /[Z)], = K, where K is the partition coefficient. This equilibrium is often referred to as the Nernst distribution. When [Z)], is plotted against [Z)], at constant temperature the curve is a straight line which terminates at the point when both the fibre and the dyebath are saturated. There are slight deviations from the linearity of the curve, particularly as the solutions become more concentrated. This system is probably exhibited in its ideal form when dyeing cellulose acetate rayon from an alcoholic dye solution, but it is also essentially true in the case of the application of disperse dyes in aqueous suspension to cellulose acetate, because the dyes are all soluble in water to a very limited extent and the undissolved particles act as a reservoir to maintain the concentration of the solution. The curve for this isotherm is shown in Fig. 12.14. [Pg.326]

It thus appears that when the concentration is very great, the amount of dissociation is very small, and vice versd, when the concentration is small the amount of dissociation is very great. Complete dissociation can perhaps never be obtained. The graphic curve (Fig. 30), called, by Nernst, the dissociation isotherm, is asymptotic towards the two axes, but when drawn on a small scale the curve appears to cut the ordinate axis. [Pg.112]

Historically, the third law of thermodynamics emerges from the heat theorem, by Nernst which states A chemical reaction between pure crystalline phases that occurs at absolute zero produces no entropy change. This means that adiabatic and isothermal processes approach each other at very low temperatures. The importance of Nernst s theorem is that it gives a solid base for the calculation of thermodynamic equilibria. [Pg.134]

A similar situation is also found in systems using insertion materials where there is a high concentration of the ion being exchanged. The notion of apparent standard potential is again used in writing the Nernst law, in which only the insertion rate appears. One also refers to insertion isotherm. [Pg.58]

Figure 16. The equivalent hydrogen pressure as a function of cathodic overpotential on Pd foil, 10 jLtm thick, in (O) 0.5 M H2SO4 or (x) with the addition of 2 x 10 Af thiourea (Maoka and Enyo ). Curves are for the Nernst equation (broken line) and the theoretical lines are for the Langmuir (solid lines) and Temkin (dotted lines, with m = 5) isotherms, with mo = 3 or 10 and 00 = 0.1. Figure 16. The equivalent hydrogen pressure as a function of cathodic overpotential on Pd foil, 10 jLtm thick, in (O) 0.5 M H2SO4 or (x) with the addition of 2 x 10 Af thiourea (Maoka and Enyo ). Curves are for the Nernst equation (broken line) and the theoretical lines are for the Langmuir (solid lines) and Temkin (dotted lines, with m = 5) isotherms, with mo = 3 or 10 and 00 = 0.1.
Nernst, Koref, and Lindematm (1910) described an aneroid drop calorimeter for the measurement of specific heat capacities. Figure 7.14 shows the design of this instrument. The entire system is located in isothermal surroundings such as melting ice. Of particular interest is the measurement of the temperature change of the calorimeter substance by means of 10 iron-constantan thermocouples mounted between the calorimeter substance and the isothermal Ud. [Pg.164]

It is appropriate to indicate now an approximate form of flux-force relation in a binary isothermal liquid mixture in the presence of an electrical potential gradient. It is called the Nernst-Planck relation and is used for systems containing ions ... [Pg.97]

The third law of thermodynamics was first stated by Nernst For certain isothermal chemical reactions between solids, the entropy changes approach zero as the thermodynamic temperature approaches zero. Nernst based this statement on his analysis of experimental data obtained by T. W. Richards, who studied the entropy changes of chemical reactions between solids as the temperature was made lower and lower. The statement of Nernst was sometimes called Nernst s heat theorem, although it is a statement of experimental fact and not a mathematical theorem. [Pg.139]


See other pages where Nernst isotherm is mentioned: [Pg.296]    [Pg.326]    [Pg.296]    [Pg.326]    [Pg.226]    [Pg.77]    [Pg.327]    [Pg.110]    [Pg.106]    [Pg.295]    [Pg.331]    [Pg.395]    [Pg.11]    [Pg.13]    [Pg.134]    [Pg.226]    [Pg.508]    [Pg.12]    [Pg.392]    [Pg.244]    [Pg.226]    [Pg.229]    [Pg.31]    [Pg.395]    [Pg.183]   
See also in sourсe #XX -- [ Pg.36 , Pg.133 , Pg.151 ]




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