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.

GPT,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

Derive the van't Hoff equation,

dlnKdT=ΔH°RT2

which gives the dependence of the equilibrium constant on temperature." Here H°is the enthalpy change of the reaction, for pure substances in their standard states (1 bar pressure for gases). Notice that if H°is positive (loosely speaking, if the reaction requires the absorption of heat), then higher temperature makes the reaction tend more to the right, as you might expect. Often you can neglect the temperature dependence ofH°; solve the equation in this case to obtain

lnKT2-lnKT1=ΔH°R1T1-1T2

Sketch qualitatively accurate graphs of G vs. P for the three phases of H20 (ice, water, and steam) at 0°C. Put all three graphs on the same set of axes, and label the point corresponding to atmospheric pressure. How would |the graphs differ at slightly higher temperatures?

A formula analogous to that for CP-CVrelates the isothermal and isentropic compressibilities of a material:

κT=κS+TVβ2CP.

(Here κS=-(1/V)(V/P)Sis the reciprocal of the adiabatic bulk modulus considered in Problem 1.39.) Derive this formula. Also check that it is true for an ideal gas.

In the previous section I derived the formula (F/V)T=-P. Explain why this formula makes intuitive sense, by discussing graphs of F vs. V with different slopes.

Suppose that a hydrogen fuel cell, as described in the text, is to be operated at 75°Cand atmospheric pressure. We wish to estimate the maximum electrical work done by the cell, using only the room temperature data at the back of this book. It is convenient to first establish a zero-point for each of the three substances, H2,O2,andH2O. Let us take Gfor both H2andO2to be zero at 25°C, so that G for a mole of H2Ois -237KJat 25°C.

(a) Using these conventions, estimate the Gibbs free energy of a mole of H2at 75°C. Repeat for O2andH2O.

(b) Using the results of part (a), calculate the maximum electrical work done by the cell at 75°C, for one mole of hydrogen fuel. Compare to the ideal performance of the cell at25°C.

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