William M. White - Geochemistry

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Geochemistry: краткое содержание, описание и аннотация

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A Comprehensive Introduction to the “Geochemist Toolbox” – the Basic Principles of Modern Geochemistry In the new edition of William M. White’s
, undergraduate and graduate students will find each of the core principles of geochemistry covered. From defining key principles and methods to examining Earth’s core composition and exploring organic chemistry and fossil fuels, this definitive edition encompasses all the information needed for a solid foundation in the earth sciences for beginners and beyond. 
For researchers and applied scientists, this book will act as a useful reference on fundamental theories of geochemistry, applications, and environmental sciences. The new edition includes new chapters on the geochemistry of the Earth’s surface (the “critical zone”), marine geochemistry, and applied geochemistry as it relates to environmental applications and geochemical exploration.
● A review of the fundamentals of geochemical thermodynamics and kinetics, trace element and organic geochemistry
● An introduction to radiogenic and stable isotope geochemistry and applications such as geologic time, ancient climates, and diets of prehistoric people
● Formation of the Earth and composition and origins of the core, the mantle, and the crust
● New chapters that cover soils and streams, the oceans, and geochemistry applied to the environment and mineral exploration
In this foundational look at geochemistry, new learners and professionals will find the answer to the essential principles and techniques of the science behind the Earth and its environs.

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Geochemistry - изображение 511

where a and b are Δ /R and Δ /R, respectively. If we can assume that Δ H and Δ S are constant over some temperature range (this is likely to be the case provided the temperature interval is small), then a plot of ln K vs. 1/ T will have a slope of Δ /R and an intercept of Δ /R. Thus, measurements of ln K made over a range of temperatures and plotted vs. 1/ T provide estimates of Δ and Δ . Even if Δ H and Δ S are not constant, they can be estimated from the instantaneous slope and intercept of a curve of ln K plotted against 1/ T . This is illustrated in Figure 3.17, which shows measurements of the solubility constant for barite (BaSO 4) plotted in this fashion (though in this case the log 10rather than natural logarithm is used). From changes of Δ H and Δ S with changing temperature and knowing the heat capacity of barite, we can also estimate heat capacities of the Ba 2+and SO 4 2–ions, which would obviously be difficult to measure directly. We can, of course, also calculate ΔG directly from eqn. 3.86. Thus, a series of measurements of the equilibrium constant for simple systems allows us to deduce the fundamental thermodynamic data needed to predict equilibrium in more complex systems.

Figure 317 Log of the solubility constant of barite plotted against the - фото 512

Figure 3.17 Log of the solubility constant of barite plotted against the inverse of temperature. The slope of a tangent to the curve is equal to −Δ H / R . The intercept of the tangent (which occurs at 1/ T = 0 and is off the plot) is equal to Δ S / R . After Blount (1977).

Example 3.8Calculating equilibrium constants and equilibrium concentrations

The hydration of olivine to form chrysotile (a serpentine mineral) may be represented in a pure Mg system as:

If this reaction controlled the concentration of Mg 2of the metamorphic fluid - фото 513

If this reaction controlled the concentration of Mg 2+of the metamorphic fluid, what would the activity of Mg 2+be in that fluid if it had a pH of 4.0 at 300° C?

Answer : Helgeson (1967) gives the thermodynamic data shown in the table below for the reactants at 300° C. From these data, we use Hess's law to calculate картинка 514and as 23138 kJ and 25301 JK respectively The equilibrium constant for the - фото 515as −231.38 kJ and −253.01 J/K respectively. The equilibrium constant for the reaction may be calculated as:

Species ΔH kJ S JK Mg 3Si 2O 5OH 4 427287 43484 Mg 2 36646 - фото 516
Species ΔH° kJ S° J/K
Mg 3Si 2O 5(OH) 4 −4272.87 434.84
Mg 2+ −366.46 109.05
H + 44.87 106.68
Mg 2SiO 4 −2132.75 186.02
H 2O −232.19 211.50

The equilibrium constant for this reaction can be written as:

Geochemistry - изображение 517

which reduces to Geochemistry - изображение 518if we take the activities of water, chrysotile, and forsterite as 1. Since pH = – log aH +, we may rearrange and obtain the activity of the magnesium ion as:

Taking the derivative with respect to temperature of both sides of eqn - фото 519

Taking the derivative with respect to temperature of both sides of eqn. 3.95(while holding pressure constant), we have:

(3.96) This equation is known as the vant Hoff equation 396 Pressure dependence - фото 520

This equation is known as the van't Hoff equation .

3.9.6 Pressure dependence of equilibrium constant

Since

Geochemistry - изображение 521

and

Geochemistry - изображение 522

then

(3.97) If Δ V rdoes not depend on pressure this equation can be integrated to obtain - фото 523

If Δ V rdoes not depend on pressure, this equation can be integrated to obtain:

(3.97a) This assumption will be pretty good for solids because their compressibilities - фото 524

This assumption will be pretty good for solids because their compressibilities are very low, but slightly less satisfactory for reactions involving liquids (such as dissolution), because they are more compressible. This assumption will be essentially totally invalid for reactions involving gases, because their volumes are highly pressure-dependent.

3.10 PRACTICAL APPROACH TO ELECTROLYTE EQUILIBRIUM

With the equilibrium constant now in our geochemical toolbox, we have the tools necessary to roll up our sleeves and get to work on some real geochemical problems. Even setting aside nonideal behavior, electrolyte solutions (geologic ones in particular) often have many components and can be extremely complex. Predicting their equilibrium state can therefore be difficult. There are, however, a few rules for approaching problems of electrolyte solutions that, when properly employed, make the task much more tractable.

3.10.1 Choosing components and species

We emphasized at the beginning of the chapter the importance of choosing the components in a system. How well we choose components will make a difference to how easily we can solve a given problem. Morel and Hering (1993) suggested these rules for choosing components and species in aqueous systems:

1 All species should be expressible as stoichiometric functions of the components, the stoichiometry being defined by chemical reactions.

2 Each species has a unique stoichiometric expression as a function of the components.

3 H2O should always be chosen as a component.

4 H+ should always be chosen as a component.

H +activity, or pH, is very often the critical variable, also called the master variable , in problems in natural waters. In addition, recall that we define the free energy of formation of H +as 0. For these reasons, it is both convenient and important that H +be chosen as a component.

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