1. Using the values of DHf° and S° provided, calculate the quantities listed below for the following phase change in ethanol,
CH3CH2OH.
CH3CH2OH(l) ⇄ CH3CH2OH(g)
DHf° [CH3CH2OH(l)] = -277.69 kJ/mol DHf° [CH3CH2OH(g)] = -235.10 kJ/mol
S°[CH3CH2OH(l)] = 160.7 J/mol·K S°[CH3CH2OH(g)] = 282.7 J/mol·K
The sign of DS°total will inform us as to whether the evaporation of ethanol is spontaneous under standard conditions (P = 1 bar and T = 25°C). If DS°total is positive then the process is spontaneous under standard conditions; if DS°total is negative then the process is non-spontaneous under standard conditions.
(a) What intermolecular attractive forces are being overcome in this phase change?
The following intermolecular attractive forces are present between liquid phase ethanol molecules.
Dispersion forces
Dipole-dipole interactions
Hydrogen “bonds”
(b) Calculate DS°system at 25.0°C.
DS°system = [(1)(282.7 J/mol·K)] – [(1)(160.7 J/mol·K)] = 122.0 J/mol·K
(c) Calculate DS°surroundings at 25.0°C.
DS°surroundings = – DH°system/T
DH°system = [(1)(-235.10 kJ/mol)] – [(1)(-277.69 kJ/mol)] = 42.59 kJ/mol
DH°system = 42590 J/mol (4 sig. fig.)
DS°surroundings = – (42590 J/mol)/298.15 K = -142.8 J/mol·K
(d) Calculate DS°otal at 25.0°C.
DS°total = DS°system + DS°surroundings
DS°total = 122.0 J/mol·K + (-142.8 J/mol·K) = – 20.8 J/mol·K
(e) Is this phase change spontaneous under standard conditions? Explain your reasoning.
Since DS°total < 0 the evaporation of ethanol, according to the data provided, is not spontaneous under standard conditions.
2. Calculate the following quantities for the evaporation of ethanol.
(a) Using the values of DHf° and S° provided in problem 1, calculate DGrxn° at 25.0°C.
DGrxn° = DHrxn° – TDSrxn°
DHrxn° = 42.59 kJ/mol (from 1c)
DSrxn° = 122.0 J/mol·K = 0.1220 kJ/ mol·K (from 1b)
DGrxn° = 42.59 kJ/mol – [(298.15 K)(0.1220 kJ/ mol·K)]
DGrxn° = 42.59 kJ/mol – 36.37 kJ/mol = 6.22 kJ/mol
(b) Calculate the value of the equilibrium constant at 25.0°C.
K = e–DG° / RT = e -6.22 kJ/mol / [(0.008314 kJ/KCmol)(298.15 K)]
K = e-2.51 = 0.0813
(c) Calculate the equilibrium vapor pressure (in torr) at 25.0°C.
For evaporation and sublimation the equilibrium constant K is equal to the equilibrium vapor pressure divided by the standard pressure P°. The standard pressure by convention is 1 bar.
K = Peq/P° so Peq = K x P°
Peq = 0.0813 x 1bar = 0.0813 bar
Peq = (0.0813 bar) x (1 atm/1.01325 bar) x (760 torr/1 atm)
Peq = 61.0 torr
(d) Calculate DGrxn at 25.0°C if the partial pressure of ethanol is 30.0 torr. Is the evaporation of ethanol
spontaneous under these conditions? Explain your reasoning.
DGrxn = DGrxn° + RTlnQ where Q is the reaction quotient.
For evaporation and sublimation Q = P/P° where P is the vapor pressure of the liquid or solid and
P° = 1 bar.
We first need to convert the given pressure (30.0 torr) to bar.
(30.0 torr) x (1 atm/760 torr) x (1.01325 bar/1 atm) = 0.0400 bar
Q = 0.0400 bar/1 bar = 0.0400
DGrxn = 6.22 kJ/mol + [(8.314 x 10-3 kJ/K·mol)(298.15 K)ln(0.0400)]
DGrxn = 6.22 kJ/mol + (-7.979 kJ/mol) = – 1.76 kJ/mol
Since DGrxn is < 0, the evaporation of ethanol is spontaneous under these conditions (P = 30.0 torr and
T = 25°C).
(e) Calculate DGrxn at 25.0°C if the partial pressure of ethanol is 75.0 torr. Is the evaporation of ethanol
spontaneous under these conditions? Explain your reasoning.
DGrxn = DGrxn° + RTlnQ where Q is the reaction quotient.
We first need to convert the given pressure (75.0 torr) to bar.
(75.0 torr) x (1 atm/760 torr) x (1.01325 bar/1 atm) = 0.100 bar
Q = 0.100 bar/1 bar = 0.100
DGrxn = 6.22 kJ/mol + [(8.314 x 10-3 kJ/K·mol)(298.15 K)ln(0.100)]
DGrxn = 6.22 kJ/mol + (- 5.708 kJ/mol) = 0.51 kJ/mol
Since DGrxn is > 0, the evaporation of ethanol is not spontaneous under these conditions (P = 75.0 torr and T = 25°C).
3. Using the values of DHf° and S° provided, calculate the quantities listed below for the following phase change in
naphthalene, C10H8.
naphthalene
C10H8(s) ⇄ C10H8(g)
DHf° [C10H8(s)] = 77.9 kJ/mol DHf° [C10H8(g)] = 150.6 kJ/mol
S° [C10H8(s)] = 167.5 J/K·mol S° [C10H8(g)] = 333.2 J/K·mol
(a) What intermolecular attractive forces are being overcome in this phase change?
Since naphthalene is nonpolar, dispersion forces must be overcome in order to sublime naphthalene.
(b) Calculate DGrxn° at 25.0°C. Is the sublimation of naphthalene spontaneous under standard conditions? Explain your reasoning.
DGrxn° = DHrxn° – TDSrxn°
DHrxn° = (1)(150.6 kJ/mol) – (1)(77.9 kJ/mol) = 72.7 kJ/mol
DSrxn° = (1)(333.2 J/mol·K) – (1)(167.5 J/mol·K) = 165.7 J/mol·K
DSrxn° = 0.1657 kJ/mol·K
DGrxn° = 72.7 kJ/mol – [(298.15 K)(0.1657 kJ/mol·K)]
DGrxn° = 72.7 kJ/mol – 49.40 kJ/mol = 23.3 kJ/mol
Since DGrxn° is > 0, the sublimation of naphthalene is not spontaneous under standard conditions.
(c) Calculate the value of the equilibrium constant at 25.0°C.
K = e–DG°/ RT = e -23.3 kJ/mol / [(0.008314 kJ/K·mol)(298.15 K)]
K = e-9.40 = 8.28 x 10-5
(d) Calculate the equilibrium vapor pressure (in torr) at 25.0°C.
For evaporation and sublimation the equilibrium constant K is equal to the equilibrium vapor pressure divided by the standard pressure P°. The standard pressure by convention is 1 bar.
K = Peq/P° so Peq = K x P°
Peq = (8.28 x 10-5) x 1bar = 8.28 x 10-5 bar
Peq = (8.28 x 10-5 bar) x (1 atm/1.01325 bar) x (760 torr/1 atm)
Peq = 0.0621 torr
(e) Calculate DGrxn at 25.0°C if the partial pressure of naphthalene is 1.00 torr. Is the sublimation of naphthalene spontaneous under these conditions? Explain your reasoning.
DGrxn = DGrxn° + RTlnQ where Q is the reaction quotient.
For evaporation and sublimation Q = P/P° where P is the vapor pressure of the liquid or solid and
P° = 1 bar.
We first need to convert the given pressure (1.00 torr) to bar.
(1.00 torr) x (1 atm/760 torr) x (1.01325 bar/1 atm) = 0.00133 bar
Q = 0.00133 bar/1 bar = 0.00133
DGrxn = 23.3 kJ/mol + [(8.314 x 10-3 kJ/mol·K)(298.15 K)ln(0.00133)]
DGrxn = 23.3 kJ/mol + (-16.42 kJ/mol) = 6.9 kJ/mol
Since DGrxn is > 0, the sublimation of naphthalene is not spontaneous under these conditions (P = 1.00 torr and T = 25°C).
4. Use the following data to calculate the value of Kp at 298 K for the reaction
N2(g) + 2 O2(g) ⇄ 2 NO2(g)
N2(g) + O2(g) ⇄ 2 NO(g) DG° = 173.2 kJ/mol
2 NO(g) + O2(g) ⇄ 2 NO2(g) DG° = – 69.7 kJ/mol
Remember that Kp and DG° are related to each other by the following equation
Kp = e–DG° / RT
You need to recognize that the desired chemical equation is the sum of the two chemical equations given. Hence, the standard Gibbs free-energy change for the desired reaction is obtained by adding the DG° values of the given reactions.
DG° = 173.2 kJ/mol + (- 69.7 kJ/mol) = 103.5 kJ/mol
Kp = e–DG° / RT = e – (103.5 kJ/mol) / [(0.008314 kJ/K·mol)(298.15 K)]
Kp = e-41.75 = 7.4 x 10-19
5. In the gas phase, formic acid exits as an equilibrium of monomer and dimer molecules. (The dimer consists of two
molecules linked through hydrogen “bonds”.)
(a) Is the formation of a dimer molecule from monomer molecules endothermic or exothermic? Justify your reasoning.
A formic acid dimer results from the formation of two hydrogen bonds between two formic acid molecules. Thus, this process is exothermic.
(b) Calculate the equilibrium constant, Kp, at 25.0°C for the monomer-dimer equilibrium
2 HCOOH(g) ⇄ (HCOOH)2(g)
using the data given below. Is this process spontaneous under standard conditions? Explain your reasoning.
DHf° (kJ/mol) S° (J/K·mol)
HCOOH (g) – 362.63 251.0
(HCOOH)2 (g) – 785.34 347.7
DG° = DH°– TDS°
DH° = [(1)(- 785.34 kJ/mol)] – [(2)(- 362.63 kJ/mol)] = – 60.08 kJ/mol
DS° = [(1)(347.7 J/mol·K)] – [(2)(251.0 J/mol·K)] = – 154.3 J/mol·K = – 0.1543 kJ/mol·K
DG° = – 60.08 kJ/mol – [(298.15 K)(- 0.1543 kJ/mol·K)]
DG° = – 60.08 kJmol – (- 46.00 kJ/mol) = – 14.08 kJ/mol
Since DG° is < 0, this process is spontaneous under standard conditions.
Kp = e–DG° / RT = e – (-14.08 kJ/mol) / [(0.0083145 kJ/KCmol)(298.15 K)]
Kp = e+5.680 = 292.9
(c) Calculate the enthalpy change per hydrogen bond formed in the gas phase. Show your reasoning clearly.
The enthalpy change (DH) for the formation of two moles of hydrogen bonds is – 60.08 kJ. Thus, the enthalpy change per mole of hydrogen bond formed is – 30.04 kJ.
(d) As the temperature increases, in which direction does the equilibrium shift? How does an increase in temperature
affect the value of Kp? Justify your reasoning.
An increase in temperature will shift an equilibrium mixture in the endothermic direction. Since this is an exothermic process, the equilibrium mixture will shift to the left (to the reactants side). The value of Kp decreases with an increase in temperature.
6. (a) Calculate the Gibbs free energy of the following reaction at 1200 K (K = 6.8)
I2(g) ⇄ 2 I(g)
when the partial pressures of I2 and I are 0.13 bar and 0.98 bar, respectively.
Since the partial pressures of the two gases are not equal to 1 bar we need to calculate ΔG not ΔG°.
DG = DG° + RTlnQ where Q is the reaction quotient
ΔG° = – RTlnK = – [(8.314 x 10-3 kJ/mol·K)(1200 K)ln(6.8)] = – 19.12 kJ/mol
Q = PI2/PI2 = (0.98)2/0.13 = 7.4
RTlnQ = [(8.314 x 10-3 kJ/mol·K)(1200 K)ln(7.4)] = 19.97 kJ/mol
ΔG = – 19.12 kJ/mol + 19.97 kJ/mol = 0.85 kJ/mol
(b) What is the spontaneous direction of the reaction at these conditions? Explain your reasoning.
Since ΔG > 0 this reaction is spontaneous to the left and will produce more I2. Also note that since
Q > K (7.4 > 6.8) this reaction will proceed to the left.
7. Use the best-fit line obtained for the data plotted in the graph below to determine DHvap and DSvap for the evaporation of
1-propanol.
CH3CH2CH2OH(l) ⇄ CH3CH2CH2OH(g)
slope = – DHvap/R Þ DHvap = – slope x R
y-intercept = DSvap/R Þ DSvap = y-intercept x R
DHvap = – (- 5.70×103 K) x (8.314 J/mol·K) = 4.74×104 J/mol = 47.4 kJ/mol
DSvap = 15.4 x 8.314 J/mol·K = 128 J/mol·K
How does the value of DHvap for the evaporation of 1-propanol compare (greater, the same, or lesser) to the value of
DHvap for the evaporation of methanol (CH3OH)? Explain your reasoning.
The value of DHvap for 1-propanol is greater than the value of DHvap for methanol because the intermolecular attractive forces are stronger between 1-propanol molecules due to the longer hydrocarbon chain present in 1-propanol which results in stronger dispersion forces.