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When carbon dioxide "dissolves" in water, essentially all of it reacts to form carbonic acid, H2CO3:

CO2(g)+H2O(l)⟷H2CO3(aq)

The carbonic acid can then dissociate into H* and bicarbonate ions,

H2CO3(aq)⟷H+(aq)+HCO3-(aq)

(The table at the back of this book gives thermodynamic data for both of these reactions.) Consider a body of otherwise pure water (or perhaps a raindrop) that is in equilibrium with the atmosphere near sea level, where the partial pressure of carbon dioxide is 3.4 x 10-4 bar (or 340 parts per million). Calculate the molality of carbonic acid and of bicarbonate ions in the water, and determine the pH of the solution. Note that even "natural" precipitation is somewhat acidic.

Short Answer

Expert verified

Therefore,

mH2CO3=1.141×10-5mol/LiterpH=5.67

Step by step solution

01

Given information

When carbon dioxide "dissolves" in water, essentially all of it reacts to form carbonic acid, H2CO3

CO2(g)+H2O(l)⟷H2CO3(aq)

The carbonic acid can then dissociate into H* and bicarbonate ions,

H2CO3(aq)⟷H+(aq)+HCO3-(aq)

Consider a body of otherwise pure water (or perhaps a raindrop) that is in equilibrium with the atmosphere near sea level, where the partial pressure of carbon dioxide is 3.4x 10 bar (or 340 parts per million).

02

Explanation

Consider the following two reactions, each of which symbolises the carbon dioxide dissolving in water:

CO2+H2O↔H2CO3H2CO3↔H++HCO3-

The concentration of carbon acid in terms of partial pressure and the change in the Gibbs free energy can be calculated using Henry's law:

mH2CO3PCO2/P°=exp-ΔG°RTmH2CO3=PCO2P°exp-ΔG°RT(1)

We need to find the change in the Gibbs free energy

G°(kJ)H2CO3-623.08H2O-237.13CO2-394.36

Change in Gibbs free energy is:

ΔG°=GH2CO3°-GH2O°-GCO2°=-623.08kJ+237.13kJ+394.36kJ=8.41kJ

03

Calculations

Substitute the values in the equation

mH2CO3=3.4×10-4bar1barexp-8.41×103J(8.314J/mol·K)(298K)mH2CO3=1.141×10-5mol/Liter

Using the law of mass action for the second reaction, we can write the concentration as:

mH+mHCO3-mH2CO3=e-ΔG°/RT(2)

To find ΔG°

G°(kJ)H2CO3-623.08H+0HCO3--586.77

Change in Gibbs energy is:

ΔG°=GH+°+GHCO3-°-GH2CO3°=-586.77kJ+623.08kJ=36.31kJ

04

Calculations

The molarity of the HT ions equals the molarity of the bicarbonate ions, so equation (2) will become:

mHCO3-2mH2CO3=e-ΔG°/RTmHCO3-2=mH2CO3e-ΔG°/RTmHCO3-=mH2CO3e-ΔG°/RT

Substituting the values,

mHCO3-=1.141×10-5mol/Litere-36310J/(8.314J/mol·K)(298K)=2.22×10-6mol/Liter

The molarity of the H+ ions is:

mH+=mHCO3-=2.22×10-6mol/Liter

The pH of solution is:

pH=-log10mH+=-log102.22×10-6mol/Liter=5.67

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Most popular questions from this chapter

The enthalpy and Gibbs free energy, as defined in this section, give special treatment to mechanical (compression-expansion) work, -PdV. Analogous quantities can be defined for other kinds of work, for instance, magnetic work." Consider the situation shown in Figure 5.7, where a long solenoid ( Nturns, total length N) surrounds a magnetic specimen (perhaps a paramagnetic solid). If the magnetic field inside the specimen is B→and its total magnetic moment is M→, then we define an auxilliary field H→(often called simply the magnetic field) by the relation

H→≡1μ0B→-M→V,

where μ0is the "permeability of free space," 4π×10-7N/A2. Assuming cylindrical symmetry, all vectors must point either left or right, so we can drop the -→symbols and agree that rightward is positive, leftward negative. From Ampere's law, one can also show that when the current in the wire is I, the Hfield inside the solenoid is NI/L, whether or not the specimen is present.

(a) Imagine making an infinitesimal change in the current in the wire, resulting in infinitesimal changes in B, M, and H. Use Faraday's law to show that the work required (from the power supply) to accomplish this change is Wtotal=VHdB. (Neglect the resistance of the wire.)

(b) Rewrite the result of part (a) in terms of Hand M, then subtract off the work that would be required even if the specimen were not present. If we define W, the work done on the system, †to be what's left, show that W=μ0HdM.

(c) What is the thermodynamic identity for this system? (Include magnetic work but not mechanical work or particle flow.)

(d) How would you define analogues of the enthalpy and Gibbs free energy for a magnetic system? (The Helmholtz free energy is defined in the same way as for a mechanical system.) Derive the thermodynamic identities for each of these quantities, and discuss their interpretations.

Assume that the air you exhale is at 35°C, with a relative humidity of 90%. This air immediately mixes with environmental air at 5°C and unknown relative humidity; during the mixing, a variety of intermediate temperatures and water vapour percentages temporarily occur. If you are able to "see your breath" due to the formation of cloud droplets during this mixing, what can you conclude about the relative humidity of your environment? (Refer to the vapour 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 a formula, similar to equation 5.90, for the shift in the freezing temperature of a dilute solution. Assume that the solid phase is pure solvent, no solute. You should find that the shift is negative: The freezing temperature of a solution is less than that of the pure solvent. Explain in general terms why the shift should be negative.

The formula for Cp-Cv derived in the previous problem can also be derived starting with the definitions of these quantities in terms of U and H. Do so. Most of the derivation is very similar, but at one point you need to use the relation P=-(∂F/∂V)T.

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