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Calcium carbonate, CaCO3, has two common crystalline forms, calcite and aragonite. Thermodynamic data for these phases can be found at the back of this book.

(a) Which is stable at earth's surface, calcite or aragonite?

(b) Calculate the pressure (still at room temperature) at which the other phase

should become stable.

Short Answer

Expert verified

The aragonite is more stable than calcite at pressure of 3.6 kbar

Step by step solution

01

Given information

A crystal with a lower Gibbs free energy is more stable at a given temperature and pressure. The Gibbs free energy per mole of two crystals is used to compare their stability.

02

Explanation 

(a) The Gibbs free energy of calcite and aragonite are

GC=-1128·8kJGa=-1127·8kJS

Under typical conditions, the Gibbs free energy of 1 mole of calcite is 1-0KJ lower than that of a mole of aragonite, based on the above numbers. As a result, at room temperature and air pressure, or at the earth's surface, calcite is in a more stable phase.

03

Concept

The volume of the substance determines the dependency of the Gibbs free energy on pressure.

∂G∂PT,N=V

Where,

G is Gibbs free energy

P is the atmospheric pressure

V is the volume of substance

The volumes of calcite and aragonite are

Vc=36.93cm3Va=34.15cm3

Converting it into kJ/kbar

Vc=36.93cm310-1kJ/kbar1cm3=3.693kJ/kbarVa=34.15cm310-1kJ/kbar1cm3=3.415kJ/kbar

Because the Aragonite has a smaller volume, it should be stable at high pressure.

Set Gc=0at P=Ibarfor simplicity; then Ga=1.0kJatP=1bar

For calcite and aragonite, the equations relating Gibbs free energy, pressure, and volume are as follows:

GC=VCPGa=VaP+1·0kJ

04

Calculations

Gashould equal Gc, at the place where the graphs for Gibbs free energy and pressure for Calcite and Aragonite intersect.

GC=Ga

Substituting the values of GcandGa

VcP=VaP+1·0kJ

Substituting the values and solving for P

P=1·0kJVC-VaP=1.0kJ3·693kJ/kbar-3.415kJ/kbarP=3.6kbar

The aragonite is more stable than calcite at pressure of 3.6 kbar

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Most popular questions from this chapter

Consider again the aluminosilicate system treated in Problem 5.29. Calculate the slopes of all three phase boundaries for this system: kyanite andalusite, kyanite-sillimanite, and andalusite-sillimanite. Sketch the phase diagram, and calculate the temperature and pressure of the triple point.

Suppose that an unsaturated air mass is rising and cooling at the dry adiabatic lapse rate found in problem 1.40. If the temperature at ground level is 25 C and the relative humidity there is 50%, at what altitude will this air mass become saturated so that condensation begins and a cloud forms (see Figure 5.18)? (Refer to the vapor pressure graph drawn in Problem 5.42)

Problem 5.58. In this problem you will model the mixing energy of a mixture in a relatively simple way, in order to relate the existence of a solubility gap to molecular behaviour. Consider a mixture of A and B molecules that is ideal in every way but one: The potential energy due to the interaction of neighbouring molecules depends upon whether the molecules are like or unlike. Let n be the average number of nearest neighbours of any given molecule (perhaps 6 or 8 or 10). Let n be the average potential energy associated with the interaction between neighbouring molecules that are the same (4-A or B-B), and let uAB be the potential energy associated with the interaction of a neighbouring unlike pair (4-B). There are no interactions beyond the range of the nearest neighbours; the values of μoandμABare independent of the amounts of A and B; and the entropy of mixing is the same as for an ideal solution.

(a) Show that when the system is unmixed, the total potential energy due to neighbor-neighbor interactions is 12Nnu0. (Hint: Be sure to count each neighbouring pair only once.)

(b) Find a formula for the total potential energy when the system is mixed, in terms of x, the fraction of B.

(c) Subtract the results of parts (a) and (b) to obtain the change in energy upon mixing. Simplify the result as much as possible; you should obtain an expression proportional to x(1-x). Sketch this function vs. x, for both possible signs of uAB-u0.

(d) Show that the slope of the mixing energy function is finite at both end- points, unlike the slope of the mixing entropy function.

(e) For the case uAB>u0, plot a graph of the Gibbs free energy of this system

vs. x at several temperatures. Discuss the implications.

(f) Find an expression for the maximum temperature at which this system has

a solubility gap.

(g) Make a very rough estimate of uAB-u0for a liquid mixture that has a

solubility gap below 100°C.

(h) Use a computer to plot the phase diagram (T vs. x) for this system.

Derive the thermodynamic identity for G (equation 5.23), and from it the three partial derivative relations 5.24.

Imagine that you drop a brick on the ground and it lands with a thud. Apparently the energy of this system tends to spontaneously decrease. Explain why.

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