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NCERT Solutions

Thermodynamics

Himachal Pradesh Board · Class 11 · Chemistry

NCERT Solutions for Thermodynamics — Himachal Pradesh Board Class 11 Chemistry.

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EXERCISES

5.1Choose the correct answer. A thermodynamic state function is a quantity
(i) used to determine heat changes
(ii) whose value is independent of path
(iii) used to determine pressure volume work
(iv) whose value depends on temperature only.
Show solution
Correct option: (ii) whose value is independent of path.

A state function is a property whose value depends only on the current state of the system (i.e., initial and final states) and not on the path taken to reach that state. Examples include internal energy (U), enthalpy (H), entropy (S), and Gibbs energy (G).
5.2For the process to occur under adiabatic conditions, the correct condition is:
(i) ΔT = 0
(ii) Δp = 0
(iii) q = 0
(iv) w = 0
Show solution
Correct option: (iii) q=0q = 0.

Adiabatic process is defined as a process in which no heat exchange takes place between the system and the surroundings. Therefore, the defining condition for an adiabatic process is q=0q = 0.
5.3The enthalpies of all elements in their standard states are:
(i) unity
(ii) zero
(iii) < 0
(iv) different for each element
Show solution
Correct option: (ii) zero.

By convention, the standard enthalpy of formation (ΔfH\Delta_f H^\circ) of every element in its most stable standard state is taken as zero. This is the reference point for all enthalpy calculations.
5.4ΔU\Delta U^\circ of combustion of methane is X kJ mol1-X\ \mathrm{kJ\ mol^{-1}}. The value of ΔH\Delta H^\circ is
(i) =ΔU= \Delta U^\circ
(ii) &gt; \Delta U^\circ
(iii) &lt; \Delta U^\circ
(iv) =0= 0
Show solution
Correct option: (iii) &lt; \Delta U^\circ.

Given: Combustion of methane:
CH4(g)+2O2(g)CO2(g)+2H2O(l)\mathrm{CH_4(g) + 2O_2(g) \rightarrow CO_2(g) + 2H_2O(l)}

Calculating Δng\Delta n_g:
Δng=moles of gaseous productsmoles of gaseous reactants\Delta n_g = \text{moles of gaseous products} - \text{moles of gaseous reactants}
Δng=1(1+2)=13=2\Delta n_g = 1 - (1+2) = 1 - 3 = -2

Using the relation:
ΔH=ΔU+ΔngRT\Delta H^\circ = \Delta U^\circ + \Delta n_g RT
ΔH=X+(2)RT\Delta H^\circ = -X + (-2)RT
ΔH=X2RT\Delta H^\circ = -X - 2RT

Since 2RT &gt; 0, we have \Delta H^\circ = -X - 2RT &lt; -X = \Delta U^\circ.

Therefore, \Delta H^\circ &lt; \Delta U^\circ.
5.5The enthalpy of combustion of methane, graphite and dihydrogen at 298 K are, 890.3 kJ mol1-890.3\ \mathrm{kJ\ mol^{-1}}, 393.5 kJ mol1-393.5\ \mathrm{kJ\ mol^{-1}}, and 285.8 kJ mol1-285.8\ \mathrm{kJ\ mol^{-1}} respectively. Enthalpy of formation of CH4(g)\mathrm{CH_4(g)} will be
(i) 74.8 kJ mol1-74.8\ \mathrm{kJ\ mol^{-1}}
(ii) 52.27 kJ mol1-52.27\ \mathrm{kJ\ mol^{-1}}
(iii) +74.8 kJ mol1+74.8\ \mathrm{kJ\ mol^{-1}}
(iv) +52.26 kJ mol1+52.26\ \mathrm{kJ\ mol^{-1}}
Show solution
Correct option: (i) 74.8 kJ mol1-74.8\ \mathrm{kJ\ mol^{-1}}.

Given reactions:

(1) CH4(g)+2O2(g)CO2(g)+2H2O(l)\mathrm{CH_4(g) + 2O_2(g) \rightarrow CO_2(g) + 2H_2O(l)}; ΔcH=890.3 kJ mol1\Delta_c H^\circ = -890.3\ \mathrm{kJ\ mol^{-1}}

(2) C(graphite)+O2(g)CO2(g)\mathrm{C(graphite) + O_2(g) \rightarrow CO_2(g)}; ΔcH=393.5 kJ mol1\Delta_c H^\circ = -393.5\ \mathrm{kJ\ mol^{-1}}

(3) H2(g)+12O2(g)H2O(l)\mathrm{H_2(g) + \frac{1}{2}O_2(g) \rightarrow H_2O(l)}; ΔcH=285.8 kJ mol1\Delta_c H^\circ = -285.8\ \mathrm{kJ\ mol^{-1}}

Target reaction (formation of methane):
C(graphite)+2H2(g)CH4(g)\mathrm{C(graphite) + 2H_2(g) \rightarrow CH_4(g)}

Applying Hess's Law: Target = (2) + 2×(3) − (1)

ΔfH[CH4]=ΔcH[C]+2ΔcH[H2]ΔcH[CH4]\Delta_f H^\circ[\mathrm{CH_4}] = \Delta_c H^\circ[\mathrm{C}] + 2\Delta_c H^\circ[\mathrm{H_2}] - \Delta_c H^\circ[\mathrm{CH_4}]

=(393.5)+2(285.8)(890.3)= (-393.5) + 2(-285.8) - (-890.3)

=393.5571.6+890.3= -393.5 - 571.6 + 890.3

=74.8 kJ mol1= -74.8\ \mathrm{kJ\ mol^{-1}}
5.6A reaction, A+BC+D+qA + B \rightarrow C + D + q is found to have a positive entropy change. The reaction will be
(i) possible at high temperature
(ii) possible only at low temperature
(iii) not possible at any temperature
(iv) possible at any temperature
Show solution
Correct option: (iv) possible at any temperature.

The reaction A+BC+D+qA + B \rightarrow C + D + q releases heat, so \Delta H &lt; 0 (exothermic). It is also given that \Delta S &gt; 0 (positive entropy change).

Using ΔG=ΔHTΔS\Delta G = \Delta H - T\Delta S:
- ΔH\Delta H is negative (−)
- TΔST\Delta S is positive (+), so TΔS-T\Delta S is negative (−)

Therefore \Delta G = (\text{negative}) - (\text{positive}) &lt; 0 at all temperatures.

Since \Delta G &lt; 0 at every temperature, the reaction is spontaneous at any temperature.
5.7In a process, 701 J of heat is absorbed by a system and 394 J of work is done by the system. What is the change in internal energy for the process?Show solution
Given:
- Heat absorbed by the system: q=+701 Jq = +701\ \mathrm{J} (positive, as heat is added to system)
- Work done by the system: w=394 Jw = -394\ \mathrm{J} (negative, as work is done by the system)

Formula (First Law of Thermodynamics):
ΔU=q+w\Delta U = q + w

Calculation:
ΔU=701 J+(394 J)\Delta U = 701\ \mathrm{J} + (-394\ \mathrm{J})
ΔU=307 J\boxed{\Delta U = 307\ \mathrm{J}}
5.8The reaction of cyanamide, NH2CN\mathrm{NH_2CN}(s), with dioxygen was carried out in a bomb calorimeter, and ΔU\Delta U was found to be 742.7 kJ mol1-742.7\ \mathrm{kJ\ mol^{-1}} at 298 K. Calculate enthalpy change for the reaction at 298 K.
NH2CN(s)+32O2(g)N2(g)+CO2(g)+H2O(l)\mathrm{NH_2CN(s) + \frac{3}{2}O_2(g) \rightarrow N_2(g) + CO_2(g) + H_2O(l)}
Show solution
Given:
NH2CN(s)+32O2(g)N2(g)+CO2(g)+H2O(l)\mathrm{NH_2CN(s) + \frac{3}{2}O_2(g) \rightarrow N_2(g) + CO_2(g) + H_2O(l)}
ΔU=742.7 kJ mol1\Delta U = -742.7\ \mathrm{kJ\ mol^{-1}}, T=298 KT = 298\ \mathrm{K}

Calculating Δng\Delta n_g:
Δng=moles of gaseous productsmoles of gaseous reactants\Delta n_g = \text{moles of gaseous products} - \text{moles of gaseous reactants}

Gaseous products: N2(g)\mathrm{N_2(g)} = 1 mol, CO2(g)\mathrm{CO_2(g)} = 1 mol → total = 2 mol

Gaseous reactants: O2(g)\mathrm{O_2(g)} = 32\frac{3}{2} mol (NH₂CN is solid)

Δng=232=+12\Delta n_g = 2 - \frac{3}{2} = +\frac{1}{2}

Using the relation:
ΔH=ΔU+ΔngRT\Delta H = \Delta U + \Delta n_g RT
ΔH=742.7+(12)(8.314×103 kJ mol1K1)(298 K)\Delta H = -742.7 + \left(\frac{1}{2}\right)(8.314 \times 10^{-3}\ \mathrm{kJ\ mol^{-1}K^{-1}})(298\ \mathrm{K})
ΔH=742.7+(0.5)(2.477)\Delta H = -742.7 + (0.5)(2.477)
ΔH=742.7+1.239\Delta H = -742.7 + 1.239
ΔH=741.5 kJ mol1\boxed{\Delta H = -741.5\ \mathrm{kJ\ mol^{-1}}}
5.9Calculate the number of kJ of heat necessary to raise the temperature of 60.0 g of aluminium from 35°C to 55°C. Molar heat capacity of Al is 24 J mol⁻¹ K⁻¹.Show solution
Given:
- Mass of Al = 60.0 g
- Molar mass of Al = 27 g mol⁻¹
- Molar heat capacity, Cp=24 J mol1 K1C_p = 24\ \mathrm{J\ mol^{-1}\ K^{-1}}
- ΔT=5535=20 K\Delta T = 55 - 35 = 20\ \mathrm{K}

Number of moles of Al:
n=60.027=2.222 moln = \frac{60.0}{27} = 2.222\ \mathrm{mol}

Formula:
q=n×Cp×ΔTq = n \times C_p \times \Delta T

Calculation:
q=2.222 mol×24 J mol1 K1×20 Kq = 2.222\ \mathrm{mol} \times 24\ \mathrm{J\ mol^{-1}\ K^{-1}} \times 20\ \mathrm{K}
q=2.222×480q = 2.222 \times 480
q=1066.56 Jq = 1066.56\ \mathrm{J}
q1.067 kJ\boxed{q \approx 1.067\ \mathrm{kJ}}
5.10Calculate the enthalpy change on freezing of 1.0 mol of water at 10.0°C to ice at -10.0°C. ΔfusH=6.03 kJ mol1\Delta_{fus}H = 6.03\ \mathrm{kJ\ mol^{-1}} at 0°C.
Cp[H2O(l)]=75.3 J mol1 K1C_p[\mathrm{H_2O(l)}] = 75.3\ \mathrm{J\ mol^{-1}\ K^{-1}}
Cp[H2O(s)]=36.8 J mol1 K1C_p[\mathrm{H_2O(s)}] = 36.8\ \mathrm{J\ mol^{-1}\ K^{-1}}
Show solution
The overall process is carried out in three steps:

Step 1: Cooling liquid water from 10°C to 0°C
ΔH1=n×Cp[H2O(l)]×ΔT=1.0×75.3×(010)\Delta H_1 = n \times C_p[\mathrm{H_2O(l)}] \times \Delta T = 1.0 \times 75.3 \times (0 - 10)
ΔH1=75.3×(10)=753 J=0.753 kJ\Delta H_1 = 75.3 \times (-10) = -753\ \mathrm{J} = -0.753\ \mathrm{kJ}

Step 2: Freezing water at 0°C (phase change)
ΔH2=ΔfusH=6.03 kJ mol1\Delta H_2 = -\Delta_{fus}H = -6.03\ \mathrm{kJ\ mol^{-1}}
(Negative because freezing is the reverse of fusion)

Step 3: Cooling ice from 0°C to −10°C
ΔH3=n×Cp[H2O(s)]×ΔT=1.0×36.8×(100)\Delta H_3 = n \times C_p[\mathrm{H_2O(s)}] \times \Delta T = 1.0 \times 36.8 \times (-10 - 0)
ΔH3=36.8×(10)=368 J=0.368 kJ\Delta H_3 = 36.8 \times (-10) = -368\ \mathrm{J} = -0.368\ \mathrm{kJ}

Total enthalpy change:
ΔHtotal=ΔH1+ΔH2+ΔH3\Delta H_{total} = \Delta H_1 + \Delta H_2 + \Delta H_3
ΔHtotal=0.753+(6.03)+(0.368)\Delta H_{total} = -0.753 + (-6.03) + (-0.368)
ΔHtotal=7.151 kJ mol1\boxed{\Delta H_{total} = -7.151\ \mathrm{kJ\ mol^{-1}}}
5.11Enthalpy of combustion of carbon to CO₂ is 393.5 kJ mol1-393.5\ \mathrm{kJ\ mol^{-1}}. Calculate the heat released upon formation of 35.2 g of CO₂ from carbon and dioxygen gas.Show solution
Given:
C(graphite)+O2(g)CO2(g); ΔcH=393.5 kJ mol1\mathrm{C(graphite) + O_2(g) \rightarrow CO_2(g)};\ \Delta_c H^\circ = -393.5\ \mathrm{kJ\ mol^{-1}}

Molar mass of CO₂ = 12 + 32 = 44 g mol⁻¹

Moles of CO₂ formed:
n=35.2 g44 g mol1=0.8 moln = \frac{35.2\ \mathrm{g}}{44\ \mathrm{g\ mol^{-1}}} = 0.8\ \mathrm{mol}

Heat released:
q=n×ΔcH=0.8 mol×393.5 kJ mol1q = n \times |\Delta_c H^\circ| = 0.8\ \mathrm{mol} \times 393.5\ \mathrm{kJ\ mol^{-1}}
q=314.8 kJ\boxed{q = 314.8\ \mathrm{kJ}}

The heat released upon formation of 35.2 g of CO₂ is 314.8 kJ.
5.12Enthalpies of formation of CO(g), CO₂(g), N₂O(g) and N₂O₄(g) are 110-110, 393-393, 8181 and 9.7 kJ mol19.7\ \mathrm{kJ\ mol^{-1}} respectively. Find the value of ΔrH\Delta_r H for the reaction:
N2O4(g)+3CO(g)N2O(g)+3CO2(g)\mathrm{N_2O_4(g) + 3CO(g) \rightarrow N_2O(g) + 3CO_2(g)}
Show solution
Given:
- ΔfH[CO(g)]=110 kJ mol1\Delta_f H^\circ[\mathrm{CO(g)}] = -110\ \mathrm{kJ\ mol^{-1}}
- ΔfH[CO2(g)]=393 kJ mol1\Delta_f H^\circ[\mathrm{CO_2(g)}] = -393\ \mathrm{kJ\ mol^{-1}}
- ΔfH[N2O(g)]=81 kJ mol1\Delta_f H^\circ[\mathrm{N_2O(g)}] = 81\ \mathrm{kJ\ mol^{-1}}
- ΔfH[N2O4(g)]=9.7 kJ mol1\Delta_f H^\circ[\mathrm{N_2O_4(g)}] = 9.7\ \mathrm{kJ\ mol^{-1}}

Formula:
ΔrH=ΔfH(products)ΔfH(reactants)\Delta_r H = \sum \Delta_f H^\circ(\text{products}) - \sum \Delta_f H^\circ(\text{reactants})

Calculation:
ΔrH=[ΔfH(N2O)+3ΔfH(CO2)][ΔfH(N2O4)+3ΔfH(CO)]\Delta_r H = [\Delta_f H^\circ(\mathrm{N_2O}) + 3\Delta_f H^\circ(\mathrm{CO_2})] - [\Delta_f H^\circ(\mathrm{N_2O_4}) + 3\Delta_f H^\circ(\mathrm{CO})]

=[81+3(393)][9.7+3(110)]= [81 + 3(-393)] - [9.7 + 3(-110)]

=[811179][9.7330]= [81 - 1179] - [9.7 - 330]

=[1098][320.3]= [-1098] - [-320.3]

=1098+320.3= -1098 + 320.3

ΔrH=777.7 kJ mol1\boxed{\Delta_r H = -777.7\ \mathrm{kJ\ mol^{-1}}}
5.13Given
N2(g)+3H2(g)2NH3(g); ΔrH=92.4 kJ mol1\mathrm{N_2(g) + 3H_2(g) \rightarrow 2NH_3(g)};\ \Delta_r H^\circ = -92.4\ \mathrm{kJ\ mol^{-1}}
What is the standard enthalpy of formation of NH₃ gas?
Show solution
Given:
N2(g)+3H2(g)2NH3(g); ΔrH=92.4 kJ mol1\mathrm{N_2(g) + 3H_2(g) \rightarrow 2NH_3(g)};\ \Delta_r H^\circ = -92.4\ \mathrm{kJ\ mol^{-1}}

The standard enthalpy of formation refers to the formation of 1 mole of NH₃ from its elements in their standard states:
12N2(g)+32H2(g)NH3(g)\mathrm{\frac{1}{2}N_2(g) + \frac{3}{2}H_2(g) \rightarrow NH_3(g)}

The given reaction produces 2 moles of NH₃, so:
ΔfH[NH3]=ΔrH2=92.42\Delta_f H^\circ[\mathrm{NH_3}] = \frac{\Delta_r H^\circ}{2} = \frac{-92.4}{2}

ΔfH[NH3]=46.2 kJ mol1\boxed{\Delta_f H^\circ[\mathrm{NH_3}] = -46.2\ \mathrm{kJ\ mol^{-1}}}
5.14Calculate the standard enthalpy of formation of CH₃OH(l) from the following data:
(i) CH3OH(l)+32O2(g)CO2(g)+2H2O(l)\mathrm{CH_3OH(l) + \frac{3}{2}O_2(g) \rightarrow CO_2(g) + 2H_2O(l)}; ΔrH=726 kJ mol1\Delta_r H^\circ = -726\ \mathrm{kJ\ mol^{-1}}
(ii) C(graphite)+O2(g)CO2(g)\mathrm{C(graphite) + O_2(g) \rightarrow CO_2(g)}; ΔrH=393 kJ mol1\Delta_r H^\circ = -393\ \mathrm{kJ\ mol^{-1}}
(iii) H2(g)+12O2(g)H2O(l)\mathrm{H_2(g) + \frac{1}{2}O_2(g) \rightarrow H_2O(l)}; ΔrH=286 kJ mol1\Delta_r H^\circ = -286\ \mathrm{kJ\ mol^{-1}}
Show solution
Target reaction (formation of methanol):
C(graphite)+2H2(g)+12O2(g)CH3OH(l)\mathrm{C(graphite) + 2H_2(g) + \frac{1}{2}O_2(g) \rightarrow CH_3OH(l)}

Applying Hess's Law:

Target = (ii) + 2×(iii) − (i)

ΔfH[CH3OH]=ΔrH(ii)+2ΔrH(iii)ΔrH(i)\Delta_f H^\circ[\mathrm{CH_3OH}] = \Delta_r H^\circ_{(ii)} + 2\Delta_r H^\circ_{(iii)} - \Delta_r H^\circ_{(i)}

=(393)+2(286)(726)= (-393) + 2(-286) - (-726)

=393572+726= -393 - 572 + 726

=965+726= -965 + 726

ΔfH[CH3OH(l)]=239 kJ mol1\boxed{\Delta_f H^\circ[\mathrm{CH_3OH(l)}] = -239\ \mathrm{kJ\ mol^{-1}}}
5.15Calculate the enthalpy change for the process
CCl4(g)C(g)+4 Cl(g)\mathrm{CCl_4(g) \rightarrow C(g) + 4\ Cl(g)}
and calculate bond enthalpy of C–Cl in CCl₄(g).
ΔvapH(CCl4)=30.5 kJ mol1\Delta_{vap}H^\circ(\mathrm{CCl_4}) = 30.5\ \mathrm{kJ\ mol^{-1}}
ΔfH(CCl4)=135.5 kJ mol1\Delta_f H^\circ(\mathrm{CCl_4}) = -135.5\ \mathrm{kJ\ mol^{-1}}
ΔaH(C)=715.0 kJ mol1\Delta_a H^\circ(\mathrm{C}) = 715.0\ \mathrm{kJ\ mol^{-1}} (enthalpy of atomisation)
ΔaH(Cl2)=242 kJ mol1\Delta_a H^\circ(\mathrm{Cl_2}) = 242\ \mathrm{kJ\ mol^{-1}}
Show solution
Step 1: Calculate ΔH\Delta H for CCl4(g)C(g)+4 Cl(g)\mathrm{CCl_4(g) \rightarrow C(g) + 4\ Cl(g)}

We construct this using the following thermochemical equations:

(1) CCl4(l)CCl4(g)\mathrm{CCl_4(l) \rightarrow CCl_4(g)}; ΔH=+30.5 kJ mol1\Delta H = +30.5\ \mathrm{kJ\ mol^{-1}} (vaporisation)

(2) C(graphite)+2Cl2(g)CCl4(l)\mathrm{C(graphite) + 2Cl_2(g) \rightarrow CCl_4(l)}; ΔfH=135.5 kJ mol1\Delta_f H^\circ = -135.5\ \mathrm{kJ\ mol^{-1}}

(3) C(graphite)C(g)\mathrm{C(graphite) \rightarrow C(g)}; ΔaH=+715.0 kJ mol1\Delta_a H^\circ = +715.0\ \mathrm{kJ\ mol^{-1}}

(4) Cl2(g)2 Cl(g)\mathrm{Cl_2(g) \rightarrow 2\ Cl(g)}; ΔaH=+242 kJ mol1\Delta_a H^\circ = +242\ \mathrm{kJ\ mol^{-1}}

Target: CCl4(g)C(g)+4 Cl(g)\mathrm{CCl_4(g) \rightarrow C(g) + 4\ Cl(g)}

Target = −(1) − (2) + (3) + 2×(4)

ΔH=30.5(135.5)+715.0+2(242)\Delta H = -30.5 - (-135.5) + 715.0 + 2(242)
=30.5+135.5+715.0+484= -30.5 + 135.5 + 715.0 + 484
=1304 kJ mol1= 1304\ \mathrm{kJ\ mol^{-1}}

Step 2: Calculate bond enthalpy of C–Cl

In CCl₄, there are 4 C–Cl bonds. The enthalpy change for breaking all 4 bonds:
ΔH=4×Bond enthalpy of C–Cl\Delta H = 4 \times \text{Bond enthalpy of C–Cl}

Bond enthalpy of C–Cl=13044\text{Bond enthalpy of C–Cl} = \frac{1304}{4}

Bond enthalpy of C–Cl=326 kJ mol1\boxed{\text{Bond enthalpy of C–Cl} = 326\ \mathrm{kJ\ mol^{-1}}}
5.16For an isolated system, ΔU=0\Delta U = 0, what will be ΔS\Delta S?Show solution
For an isolated system: No exchange of energy or matter with surroundings occurs.

Given: ΔU=0\Delta U = 0

For any spontaneous process in an isolated system, the entropy of the system increases. According to the second law of thermodynamics:

\Delta S &gt; 0

Conclusion: For an isolated system with ΔU=0\Delta U = 0, the entropy change ΔS\Delta S will be greater than zero (\Delta S &gt; 0). The entropy of an isolated system increases for any spontaneous (irreversible) process, and remains constant only for a reversible (equilibrium) process.
5.17For the reaction at 298 K,
2A+BC2A + B \rightarrow C
ΔH=400 kJ mol1\Delta H = 400\ \mathrm{kJ\ mol^{-1}} and ΔS=0.2 kJ K1 mol1\Delta S = 0.2\ \mathrm{kJ\ K^{-1}\ mol^{-1}}
At what temperature will the reaction become spontaneous considering ΔH\Delta H and ΔS\Delta S to be constant over the temperature range?
Show solution
Given:
- ΔH=+400 kJ mol1\Delta H = +400\ \mathrm{kJ\ mol^{-1}} (endothermic)
- ΔS=+0.2 kJ K1 mol1\Delta S = +0.2\ \mathrm{kJ\ K^{-1}\ mol^{-1}}

Condition for spontaneity: \Delta G &lt; 0

\Delta G = \Delta H - T\Delta S &lt; 0

T\Delta S &gt; \Delta H

T &gt; \frac{\Delta H}{\Delta S}

T &gt; \frac{400\ \mathrm{kJ\ mol^{-1}}}{0.2\ \mathrm{kJ\ K^{-1}\ mol^{-1}}}

T &gt; 2000\ \mathrm{K}

Conclusion: The reaction will become spontaneous at temperatures above 2000 K. Since both \Delta H &gt; 0 and \Delta S &gt; 0, the reaction is non-spontaneous at low temperatures but becomes spontaneous at high temperatures.
5.18For the reaction,
2 Cl(g)Cl2(g)2\ \mathrm{Cl(g) \rightarrow Cl_2(g)}
what are the signs of ΔH\Delta H and ΔS\Delta S?
Show solution
Analysis of the reaction: 2 Cl(g)Cl2(g)\mathrm{2\ Cl(g) \rightarrow Cl_2(g)}

Sign of ΔH\Delta H:
This reaction involves formation of a Cl–Cl bond from two chlorine atoms. Bond formation releases energy. Therefore, the reaction is exothermic.
\Delta H &lt; 0\ (\text{negative})

Sign of ΔS\Delta S:
Two moles of gaseous atoms combine to form one mole of gaseous molecule. The number of moles of gas decreases from 2 to 1, which means the disorder (randomness) of the system decreases.
\Delta S &lt; 0\ (\text{negative})

Conclusion: Both ΔH\Delta H and ΔS\Delta S are negative for this reaction.
5.19For the reaction
2A(g)+B(g)2D(g)2A(g) + B(g) \rightarrow 2D(g)
ΔU=10.5 kJ\Delta U^\circ = -10.5\ \mathrm{kJ} and ΔS=44.1 J K1\Delta S^\circ = -44.1\ \mathrm{J\ K^{-1}}
Calculate ΔG\Delta G^\circ for the reaction, and predict whether the reaction may occur spontaneously.
Show solution
Given:
- ΔU=10.5 kJ\Delta U^\circ = -10.5\ \mathrm{kJ}
- ΔS=44.1 J K1=0.0441 kJ K1\Delta S^\circ = -44.1\ \mathrm{J\ K^{-1}} = -0.0441\ \mathrm{kJ\ K^{-1}}
- T=298 KT = 298\ \mathrm{K}

Step 1: Calculate ΔH\Delta H^\circ

For the reaction 2A(g)+B(g)2D(g)\mathrm{2A(g) + B(g) \rightarrow 2D(g)}:
Δng=2(2+1)=23=1\Delta n_g = 2 - (2+1) = 2 - 3 = -1

ΔH=ΔU+ΔngRT\Delta H^\circ = \Delta U^\circ + \Delta n_g RT
=10.5+(1)(8.314×103)(298)= -10.5 + (-1)(8.314 \times 10^{-3})(298)
=10.5+(2.478)= -10.5 + (-2.478)
=12.978 kJ mol1= -12.978\ \mathrm{kJ\ mol^{-1}}

Step 2: Calculate ΔG\Delta G^\circ
ΔG=ΔHTΔS\Delta G^\circ = \Delta H^\circ - T\Delta S^\circ
=12.978(298)(0.0441)= -12.978 - (298)(-0.0441)
=12.978+13.14= -12.978 + 13.14
=+0.162 kJ mol1= +0.162\ \mathrm{kJ\ mol^{-1}}

ΔG+0.16 kJ mol1\boxed{\Delta G^\circ \approx +0.16\ \mathrm{kJ\ mol^{-1}}}

Prediction: Since \Delta G^\circ &gt; 0, the reaction is non-spontaneous under standard conditions.
5.20The equilibrium constant for a reaction is 10. What will be the value of ΔG\Delta G^\circ? R=8.314 J K1 mol1R = 8.314\ \mathrm{J\ K^{-1}\ mol^{-1}}, T=300 KT = 300\ \mathrm{K}.Show solution
Given:
- K=10K = 10
- R=8.314 J K1 mol1R = 8.314\ \mathrm{J\ K^{-1}\ mol^{-1}}
- T=300 KT = 300\ \mathrm{K}

Formula:
ΔG=RTlnK\Delta G^\circ = -RT\ln K

Calculation:
ΔG=(8.314 J K1 mol1)(300 K)(ln10)\Delta G^\circ = -(8.314\ \mathrm{J\ K^{-1}\ mol^{-1}})(300\ \mathrm{K})(\ln 10)
=(8.314)(300)(2.303)= -(8.314)(300)(2.303)
=(8.314)(300)(2.303)= -(8.314)(300)(2.303)
=5744.14 J mol1= -5744.14\ \mathrm{J\ mol^{-1}}

ΔG=5744 J mol15.74 kJ mol1\boxed{\Delta G^\circ = -5744\ \mathrm{J\ mol^{-1}} \approx -5.74\ \mathrm{kJ\ mol^{-1}}}
5.21Comment on the thermodynamic stability of NO(g), given
12N2(g)+12O2(g)NO(g); ΔrH=90 kJ mol1\frac{1}{2}\mathrm{N_2(g)} + \frac{1}{2}\mathrm{O_2(g)} \rightarrow \mathrm{NO(g)};\ \Delta_r H^\circ = 90\ \mathrm{kJ\ mol^{-1}}
NO(g)+12O2(g)NO2(g); ΔrH=74 kJ mol1\mathrm{NO(g)} + \frac{1}{2}\mathrm{O_2(g)} \rightarrow \mathrm{NO_2(g)};\ \Delta_r H^\circ = -74\ \mathrm{kJ\ mol^{-1}}
Show solution
Reaction 1: Formation of NO(g) from elements:
12N2(g)+12O2(g)NO(g); ΔrH=+90 kJ mol1\frac{1}{2}\mathrm{N_2(g)} + \frac{1}{2}\mathrm{O_2(g)} \rightarrow \mathrm{NO(g)};\ \Delta_r H^\circ = +90\ \mathrm{kJ\ mol^{-1}}

Since \Delta_r H^\circ = +90\ \mathrm{kJ\ mol^{-1}} &gt; 0, the formation of NO from its elements is endothermic. This means NO has higher energy than its constituent elements. Therefore, NO is thermodynamically unstable with respect to its elements N2\mathrm{N_2} and O2\mathrm{O_2}.

Reaction 2: Conversion of NO to NO₂:
NO(g)+12O2(g)NO2(g); ΔrH=74 kJ mol1\mathrm{NO(g)} + \frac{1}{2}\mathrm{O_2(g)} \rightarrow \mathrm{NO_2(g)};\ \Delta_r H^\circ = -74\ \mathrm{kJ\ mol^{-1}}

Since \Delta_r H^\circ = -74\ \mathrm{kJ\ mol^{-1}} &lt; 0, the conversion of NO to NO₂ is exothermic. This means NO is also thermodynamically unstable with respect to NO₂.

Conclusion: NO(g) is thermodynamically unstable both with respect to its elements (N2,O2\mathrm{N_2, O_2}) and with respect to NO2\mathrm{NO_2}. However, it is kinetically stable (does not decompose rapidly at room temperature due to high activation energy).
5.22Calculate the entropy change in surroundings when 1.00 mol of H₂O(l) is formed under standard conditions. ΔrH=286 kJ mol1\Delta_r H^\circ = -286\ \mathrm{kJ\ mol^{-1}}.Show solution
Given:
- ΔrH=286 kJ mol1\Delta_r H^\circ = -286\ \mathrm{kJ\ mol^{-1}} (for formation of 1 mol H₂O(l))
- T=298 KT = 298\ \mathrm{K} (standard conditions)

Concept: The heat released by the system is absorbed by the surroundings.

Heat absorbed by surroundings:
qsurr=ΔrHsystem=(286)=+286 kJ mol1q_{\text{surr}} = -\Delta_r H^\circ_{\text{system}} = -(-286) = +286\ \mathrm{kJ\ mol^{-1}}

Formula for entropy change of surroundings:
ΔSsurr=qsurrT=+286×103 J mol1298 K\Delta S_{\text{surr}} = \frac{q_{\text{surr}}}{T} = \frac{+286 \times 10^3\ \mathrm{J\ mol^{-1}}}{298\ \mathrm{K}}

ΔSsurr=286000298\Delta S_{\text{surr}} = \frac{286000}{298}

ΔSsurr=+959.73 J K1 mol1\boxed{\Delta S_{\text{surr}} = +959.73\ \mathrm{J\ K^{-1}\ mol^{-1}}}

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