Thermodynamics, Practical - Chemistry, Study notes of Chemistry

Gibbs free energy euilibria between pure solid processes Euilibria involving mixtures

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Geochemistry 2005/2006
DM Sherman
Page 1 of 7
Practical 2: Thermodynamic Calculations
(SOLUTIONS)
Background: Gibbs Free Energy of a Chemical Reaction
As you will learn in the next few lectures, the Gibbs free energy (G) of a
substance at a temperature T (in K) given by
G = H - TS
where H is the enthalpy and S is the entropy. In practice, we take H to be that
required for the formation of the substance from the elements (designated ΔHf )
(This means that the ΔHf for any pure element is simply zero.). For a chemical
reaction from A to B, the change in G, ΔG, will be
Δ
G = (
Δ
HfB-
Δ
HfA) –T(SB-SA)
=
Δ
H - T
Δ
S
The problem is that H and S are functions of pressure (P) and temperature (T).
A pretty good approximation (valid when the change in heat capacity,
Δ
Cp = 0) is
that
ΔG(P,T)=ΔH(P0,T0)+TΔS(P0,T0)+ΔVdP
1
P
where
Δ
H(P0,T0) means
Δ
H when P=P0 and T=T0. P0 is usually 1 bar and T0 =
298 K.
Part I: Equilibria Between Pure Solid Phases
Most minerals are not very compressible; over the pressure range of the Earth’s
crust, the molar volume of a mineral is nearly constant. If the reaction involves
only mineral (solid) phases, then to a good approximation
Δ
V is constant. With
P0 = 1 bar, we have
Δ
G =
Δ
H1bar- T
Δ
S + (P-1)
Δ
V
where
Δ
V is the molar volume change of the reaction. If two substances A and
B are in chemical equilibrium, then the difference in free energy between them
will be zero:
Δ
G =
Δ
H1bar- T
Δ
S + (P-1)
Δ
V = 0
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DM Sherman

Practical 2: Thermodynamic Calculations

(SOLUTIONS)

Background: Gibbs Free Energy of a Chemical Reaction

As you will learn in the next few lectures, the Gibbs free energy (G) of a

substance at a temperature T (in K) given by

G = H - TS

where H is the enthalpy and S is the entropy. In practice, we take H to be that

required for the formation of the substance from the elements (designated ΔH f

(This means that the ΔH f for any pure element is simply zero.). For a chemical

reaction from A to B, the change in G, ΔG, will be

Δ G = ( Δ H

f

B

- Δ H f

A ) – T(S B

- S A ) = Δ H - T Δ S

The problem is that H and S are functions of pressure (P) and temperature (T).

A pretty good approximation (valid when the change in heat capacity, Δ C p = 0) is

that

Δ G ( P , T ) = Δ H ( P

0

, T

0

) + T Δ S ( P

0

, T

0 ) + Δ VdP

1

P

where Δ H(P 0

,T

0 ) means Δ H when P=P 0 and T=T 0

. P

0 is usually 1 bar and T 0

298 K.

Part I: Equilibria Between Pure Solid Phases

Most minerals are not very compressible; over the pressure range of the Earth’s

crust, the molar volume of a mineral is nearly constant. If the reaction involves

only mineral (solid) phases, then to a good approximation Δ V is constant. With

P

0 = 1 bar, we have

Δ G = Δ H

1bar

- T Δ S + (P-1) Δ V

where Δ V is the molar volume change of the reaction. If two substances A and

B are in chemical equilibrium , then the difference in free energy between them

will be zero:

Δ G = Δ H

1bar

- T Δ S + (P-1) Δ V = 0

DM Sherman

we can use this to calculate the boundary in P,T space between two phases.

Along this boundary, both phases will coexist.

1. Using the approximation that the P,T phase boundary is defined by

Δ H

1bar, 298K

- T Δ S

**298K

  • (P-1)** Δ V = 0, calculate the phase diagram (plot P vs

T) for calcite-aragonite given the following thermodynamic data: (Be careful!

Use dimensional analysis to convert (P-1) Δ V into kJ/mole.)

Species Δ H f, 1bar

(kJ/mol)

S

298K

(kJ/mol-K)

V

(cm 3 /mole)

Calcite, CaCO 3

Aragonite, CaCO 3

Solution: For the reaction Calcite = Aragonite:

ΔH = - 1297.43-(-1207.37) = - 0.06 kJ/mole

ΔS = 0.08799-0.09171 = - 0.00372 kJ/mol-K

ΔV = 49.9 – 44.09 = - 2.78 cm 3 /mole

Thus

ΔG = - 0.06 (kJ/mole) – T(K)(-0.00372) kJ/mol-K)

  • (P-1)(bar)(-2.78 cm 3 /mole)(
  • 4 kJ/bar-cm 3 )

= - 0.06 + 0.00372T - (2.78 x 10

  • 4 )(P) + 2.78x - 4 = 0

or P (bar) = - 214.8 + 13.4T

DM Sherman

2. Calculate the phase diagram for the dehydration of brucite Mg(OH) 2 to

periclase MgO and H 2 O(gas) given the following thermodynamic data.

(Assume steam is an ideal gas; do we need to include the volume change of the

solids?)

Species Δ H f, 1bar

(kJ/mol)

S

(kJ/mol-K)

V

(cm 3 /mole)

Brucite (Mg(OH) 2

Periclase (MgO) - 601.49 0.02694 11.

Steam (H 2

O) - 241.81 0.18872 24789.

Solution:

For the reaction Mg(OH) 2 = MgO + H 2 O(g)

ΔH = - 241.81-601.49 - (-924.54) = 81.24 kJ/mole

ΔS = 0.18872 + 0.02694 – 0.06318 = 0.1525 kJ/mol-K

Δ VdP

1

P

∫ ≈^ VgasdP

1

P

∫ =^

RT

P

1

P

dP^ =^ RT^ ln^

P bar

1 bar

kJ

molK

T^ ( K )ln^

P bars

1 bar

Thus, along the reaction boundary:

ΔG = 81.24 – T (0.1525) + 0.00831T(ln(P bar/1bar)) = 0

or P (bar)/(1bar) = Exp(-9771/T + 18.2)

DM Sherman

Pressure (kbar)

Temperature (K)

Mg(OH) 2

MgO + H 2

O

Part III: Equilibria Involving Mixtures

In the two previous problems, the products and reactants were all separate pure

phases. Many problems in geochemistry involve phases that are mixtures of

several components. An example is an aqueous solution (e.g., 1 mole of NaCl in

water) or a solid solution between two endmembers (e.g., forsterite, Mg 2 SiO 4

and fayalite, Fe 2 SiO 4 in olivine). As we will derive in the next few lectures, the

free energy of a solution is defined in terms of the activities of the components.

For now, accept the following rules:

  1. the activity of an ion in aqueous solution is numerically equal to its molal

concentration (= moles/kg of water). The standard state is 1 molal with

the properties of infinite dilution (!).

  1. The activity of a gas phase component is numerically equal to its partial

pressure. The standard state is pure gas component at 1 bar pressure.

  1. The activity of a pure solid substance is 1.

  2. The activity of a component in a solid solution is a bit more

complicated…

For a chemical equilibrium aA + bB = cC + dD, we can write an equilibrium

constant

DM Sherman

3. Now calculate the effect of temperature on the log(K) for the dissolution

of galena at pH 2. Plot log[Pb] vs T. Is PbS very soluble at any T? How

do we form ore deposits of PbS?

Solution:

2.303log( K ) = ln( K ) =

−Δ H

RT

Δ S

R

log( K ) =

1

− 79.

0.00831 T

−0.

 =^

−4128.

T

− 0.

log( K ) = 2 log[ Pb ] + pH

log[ Pb ] =

1

2

(log( K )^ −^ pH ) =^

−2064.

T

− 1.

200 300 400 500 600 700

log[Pb

2+

]

Temperature (K)

pH =