The Second and Third Laws of Thermodynamics

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Thermodynamics

The Second and Third Laws of Thermodynamics

OpenStaxCollege

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Learning Objectives

By the end of this section, you will be able to:

State and explain the second and third laws of thermodynamics
Calculate entropy changes for phase transitions and chemical reactions under standard conditions

The Second Law of Thermodynamics

In the quest to identify a property that may reliably predict the spontaneity of a process, we have identified a very promising candidate: entropy. Processes that involve an increase in entropy of the system (ΔS > 0) are very often spontaneous; however, examples to the contrary are plentiful. By expanding consideration of entropy changes to include the surroundings, we may reach a significant conclusion regarding the relation between this property and spontaneity. In thermodynamic models, the system and surroundings comprise everything, that is, the universe, and so the following is true:

\(\text{Δ}{S}_{\text{univ}}=\text{Δ}{S}_{\text{sys}}+\text{Δ}{S}_{\text{surr}}\)

To illustrate this relation, consider again the process of heat flow between two objects, one identified as the system and the other as the surroundings. There are three possibilities for such a process:

The objects are at different temperatures, and heat flows from the hotter to the cooler object. This is always observed to occur spontaneously. Designating the hotter object as the system and invoking the definition of entropy yields the following:
\(\text{Δ}{S}_{\text{sys}}=\phantom{\rule{0.2em}{0ex}}\frac{\text{−}{q}_{\text{rev}}}{{T}_{\text{sys}}}\phantom{\rule{2em}{0ex}}\text{and}\phantom{\rule{2em}{0ex}}\text{Δ}{S}_{\text{surr}}=\phantom{\rule{0.2em}{0ex}}\frac{{q}_{\text{rev}}}{{T}_{\text{surr}}}\)

The arithmetic signs of q_rev denote the loss of heat by the system and the gain of heat by the surroundings. Since T_sys > T_surr in this scenario, the magnitude of the entropy change for the surroundings will be greater than that for the system, and so the sum of ΔS_sys and ΔS_surr will yield a positive value for ΔS_univ. This process involves an increase in the entropy of the universe.
The objects are at different temperatures, and heat flows from the cooler to the hotter object. This is never observed to occur spontaneously. Again designating the hotter object as the system and invoking the definition of entropy yields the following:
\(\text{Δ}{S}_{\text{sys}}=\phantom{\rule{0.2em}{0ex}}\frac{{q}_{\text{rev}}}{{T}_{\text{sys}}}\phantom{\rule{2em}{0ex}}\text{and}\phantom{\rule{2em}{0ex}}\text{Δ}{S}_{\text{surr}}=\phantom{\rule{0.2em}{0ex}}\frac{\text{−}{q}_{\text{rev}}}{{T}_{\text{surr}}}\)

The arithmetic signs of q_rev denote the gain of heat by the system and the loss of heat by the surroundings. The magnitude of the entropy change for the surroundings will again be greater than that for the system, but in this case, the signs of the heat changes will yield a negative value for ΔS_univ. This process involves a decrease in the entropy of the universe.
The temperature difference between the objects is infinitesimally small, T_sys ≈ T_surr, and so the heat flow is thermodynamically reversible. See the previous section’s discussion). In this case, the system and surroundings experience entropy changes that are equal in magnitude and therefore sum to yield a value of zero for ΔS_univ. This process involves no change in the entropy of the universe.

These results lead to a profound statement regarding the relation between entropy and spontaneity known as the second law of thermodynamics: all spontaneous changes cause an increase in the entropy of the universe. A summary of these three relations is provided in [link].

The Second Law of Thermodynamics
ΔS_univ > 0	spontaneous
ΔS_univ < 0	nonspontaneous (spontaneous in opposite direction)
ΔS_univ = 0	reversible (system is at equilibrium)

For many realistic applications, the surroundings are vast in comparison to the system. In such cases, the heat gained or lost by the surroundings as a result of some process represents a very small, nearly infinitesimal, fraction of its total thermal energy. For example, combustion of a fuel in air involves transfer of heat from a system (the fuel and oxygen molecules undergoing reaction) to surroundings that are infinitely more massive (the earth’s atmosphere). As a result, q_surr is a good approximation of q_rev, and the second law may be stated as the following:

\(\text{Δ}{S}_{\text{univ}}=\text{Δ}{S}_{\text{sys}}+\text{Δ}{S}_{\text{surr}}=\text{Δ}{S}_{\text{sys}}+\frac{{q}_{\text{surr}}}{T}\)

We may use this equation to predict the spontaneity of a process as illustrated in [link].

Will Ice Spontaneously Melt?
The entropy change for the process

\({\text{H}}_{2}\text{O}\left(s\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{H}}_{2}\text{O}\left(l\right)\)

is 22.1 J/K and requires that the surroundings transfer 6.00 kJ of heat to the system. Is the process spontaneous at −10.00 °C? Is it spontaneous at +10.00 °C?

Solution
We can assess the spontaneity of the process by calculating the entropy change of the universe. If ΔS_univ is positive, then the process is spontaneous. At both temperatures, ΔS_sys = 22.1 J/K and q_surr = −6.00 kJ.

At −10.00 °C (263.15 K), the following is true:

\(\begin{array}{cc}\hfill \text{Δ}{S}_{\text{univ}}& =\text{Δ}{S}_{\text{sys}}+\text{Δ}{S}_{\text{surr}}=\text{Δ}{S}_{\text{sys}}+\frac{{q}_{\text{surr}}}{T}\hfill \\ & =\text{22.1 J/K}+\frac{-6.00\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{3}\phantom{\rule{0.2em}{0ex}}\text{J}}{\text{263.15 K}}\phantom{\rule{0.2em}{0ex}}=-0.7\phantom{\rule{0.2em}{0ex}}\text{J/K}\hfill \end{array}\)

S_univ < 0, so melting is nonspontaneous (not spontaneous) at −10.0 °C.

At 10.00 °C (283.15 K), the following is true:

\(\begin{array}{}\\ \text{Δ}{S}_{\text{univ}}=\text{Δ}{S}_{\text{sys}}+\frac{{q}_{\text{surr}}}{T}\\ \\ =22.1\phantom{\rule{0.2em}{0ex}}\text{J/K}+\frac{-6.00\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}{10}^{3}\phantom{\rule{0.2em}{0ex}}\text{J}}{\text{283.15 K}}\phantom{\rule{0.2em}{0ex}}=\text{+0.9 J/K}\end{array}\)

S_univ > 0, so melting is spontaneous at 10.00 °C.

Check Your Learning
Using this information, determine if liquid water will spontaneously freeze at the same temperatures. What can you say about the values of S_univ?

Answer:

Entropy is a state function, and freezing is the opposite of melting. At −10.00 °C spontaneous, +0.7 J/K; at +10.00 °C nonspontaneous, −0.9 J/K.

The Third Law of Thermodynamics

The previous section described the various contributions of matter and energy dispersal that contribute to the entropy of a system. With these contributions in mind, consider the entropy of a pure, perfectly crystalline solid possessing no kinetic energy (that is, at a temperature of absolute zero, 0 K). This system may be described by a single microstate, as its purity, perfect crystallinity and complete lack of motion means there is but one possible location for each identical atom or molecule comprising the crystal (W = 1). According to the Boltzmann equation, the entropy of this system is zero.

\(S=k\phantom{\rule{0.2em}{0ex}}\text{ln}\phantom{\rule{0.2em}{0ex}}W=k\phantom{\rule{0.2em}{0ex}}\text{ln}\phantom{\rule{0.1em}{0ex}}\left(1\right)=0\)

This limiting condition for a system’s entropy represents the third law of thermodynamics: the entropy of a pure, perfect crystalline substance at 0 K is zero.

We can make careful calorimetric measurements to determine the temperature dependence of a substance’s entropy and to derive absolute entropy values under specific conditions. Standard entropies are given the label \({S}_{298}^{°}\) for values determined for one mole of substance at a pressure of 1 bar and a temperature of 298 K. The standard entropy change (ΔS°) for any process may be computed from the standard entropies of its reactant and product species like the following:

\(\text{Δ}S\text{°}=\sum \nu {S}_{298}^{°}\text{(products)}\phantom{\rule{0.2em}{0ex}}-\sum \nu {S}_{298}^{°}\text{(reactants)}\)

Here, ν represents stoichiometric coefficients in the balanced equation representing the process. For example, ΔS° for the following reaction at room temperature

\(m\text{A}+n\text{B}\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}x\text{C}+y\text{D,}\)

is computed as the following:

\(=\left[x{S}_{298}^{°}\left(\text{C}\right)+y{S}_{298}^{°}\left(\text{D}\right)\right]\phantom{\rule{0.2em}{0ex}}-\phantom{\rule{0.2em}{0ex}}\left[m{S}_{298}^{°}\left(\text{A}\right)+n{S}_{298}^{°}\left(\text{B}\right)\right]\)

[link] lists some standard entropies at 298.15 K. You can find additional standard entropies in Appendix G.

Standard Entropies (at 298.15 K, 1 atm)
Substance	\({S}_{298}^{°}\) (J mol⁻¹ K⁻¹)
carbon
C(s, graphite)	5.740
C(s, diamond)	2.38
CO(g)	197.7
CO₂(g)	213.8
CH₄(g)	186.3
C₂H₄(g)	219.5
C₂H₆(g)	229.5
CH₃OH(l)	126.8
C₂H₅OH(l)	160.7
hydrogen
H₂(g)	130.57
H(g)	114.6
H₂O(g)	188.71
H₂O(l)	69.91
HCI(g)	186.8
H₂S(g)	205.7
oxygen
O₂(g)	205.03

Determination of ΔS°
Calculate the standard entropy change for the following process:

\({\text{H}}_{2}\text{O}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{H}}_{2}\text{O}\left(l\right)\)

Solution
The value of the standard entropy change at room temperature, \(\text{Δ}{S}_{298}^{°},\) is the difference between the standard entropy of the product, H₂O(l), and the standard entropy of the reactant, H₂O(g).

\(\begin{array}{}\\ \hfill \text{Δ}{S}_{298}^{°}& ={S}_{298}^{°}\left({\text{H}}_{2}\text{O}\left(l\right)\right)\phantom{\rule{0.2em}{0ex}}-{S}_{298}^{°}\left({\text{H}}_{2}\text{O}\left(g\right)\right)\hfill \\ & =\left(\text{70.0 J}{\phantom{\rule{0.2em}{0ex}}\text{mol}}^{\text{−1}}\phantom{\rule{0.2em}{0ex}}{\text{K}}^{\text{−1}}\right)\phantom{\rule{0.2em}{0ex}}-\phantom{\rule{0.2em}{0ex}}\left(\text{188.8 J}{\text{mol}}^{\text{−1}}\phantom{\rule{0.2em}{0ex}}{\text{K}}^{\text{−1}}\right)=-118.8\phantom{\rule{0.2em}{0ex}}\text{J}\phantom{\rule{0.2em}{0ex}}{\text{mol}}^{\text{−1}}\phantom{\rule{0.2em}{0ex}}{\text{K}}^{\text{−1}}\hfill \end{array}\)

The value for \(\text{Δ}{S}_{298}^{°}\) is negative, as expected for this phase transition (condensation), which the previous section discussed.

Check Your Learning
Calculate the standard entropy change for the following process:

\({\text{H}}_{2}\left(g\right)+{\text{C}}_{2}{\text{H}}_{4}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{C}}_{2}{\text{H}}_{6}\left(g\right)\)

Answer:

−120.6 J mol⁻¹ K⁻¹

Determination of ΔS°
Calculate the standard entropy change for the combustion of methanol, CH₃OH:

\(2{\text{CH}}_{3}\text{OH}\left(l\right)+3{\text{O}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2{\text{CO}}_{2}\left(g\right)+4{\text{H}}_{2}\text{O}\left(l\right)\)

Solution
The value of the standard entropy change is equal to the difference between the standard entropies of the products and the entropies of the reactants scaled by their stoichiometric coefficients.

\(\text{Δ}S\text{°}=\text{Δ}{S}_{298}^{°}=\sum \nu {S}_{298}^{°}\text{(products)}\phantom{\rule{0.2em}{0ex}}-\sum \nu {S}_{298}^{°}\text{(reactants)}\)

\(\begin{array}{c}\left[2{S}_{298}^{°}\left({\text{CO}}_{2}\left(g\right)\right)\phantom{\rule{0.2em}{0ex}}+\phantom{\rule{0.2em}{0ex}}4{S}_{298}^{°}\left({\text{H}}_{2}\text{O}\left(l\right)\right)\right]\phantom{\rule{0.2em}{0ex}}-\phantom{\rule{0.2em}{0ex}}\left[2{S}_{298}^{°}\left({\text{CH}}_{3}\text{OH}\left(l\right)\right)\phantom{\rule{0.2em}{0ex}}+3{S}_{298}^{°}\left({\text{O}}_{2}\left(g\right)\right)\right]\\ \\ =\mathbf{\left\{}\phantom{\rule{0.1em}{0ex}}\left[2\left(213.8\right)+4\phantom{\rule{0.2em}{0ex}}×\phantom{\rule{0.2em}{0ex}}70.0\right]\phantom{\rule{0.2em}{0ex}}-\phantom{\rule{0.2em}{0ex}}\left[2\left(126.8\right)+3\left(205.03\right)\right]\phantom{\rule{0.2em}{0ex}}\mathbf{\right\}}=-161.1\phantom{\rule{0.2em}{0ex}}\text{J/mol·K}\end{array}\)

Check Your Learning
Calculate the standard entropy change for the following reaction:

\(\text{Ca}{\left(\text{OH}\right)}_{2}\left(\text{s}\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}\text{CaO}\left(s\right)+{\text{H}}_{2}\text{O}\left(l\right)\)

Answer:

24.7 J/mol·K

Key Concepts and Summary

The second law of thermodynamics states that a spontaneous process increases the entropy of the universe, S_univ > 0. If ΔS_univ < 0, the process is nonspontaneous, and if ΔS_univ = 0, the system is at equilibrium. The third law of thermodynamics establishes the zero for entropy as that of a perfect, pure crystalline solid at 0 K. With only one possible microstate, the entropy is zero. We may compute the standard entropy change for a process by using standard entropy values for the reactants and products involved in the process.

Key Equations

\(\text{Δ}S\text{°}=\text{Δ}{S}_{298}^{°}=\sum \text{ν}{S}_{298}^{°}\text{(products)}\phantom{\rule{0.2em}{0ex}}-\sum \text{ν}{S}_{298}^{°}\text{(reactants)}\)
\(\text{Δ}S=\phantom{\rule{0.2em}{0ex}}\frac{{q}_{\text{rev}}}{T}\)
ΔS_univ = ΔS_sys + ΔS_surr
\(\text{Δ}{S}_{\text{univ}}=\text{Δ}{S}_{\text{sys}}+\text{Δ}{S}_{\text{surr}}=\text{Δ}{S}_{\text{sys}}+\frac{{q}_{\text{surr}}}{T}\)

Chemistry End of Chapter Exercises

What is the difference between ΔS, ΔS°, and \(\text{Δ}{S}_{298}^{°}\) for a chemical change?

Calculate \(\text{Δ}{S}_{298}^{°}\) for the following changes.

(a) \({\text{SnCl}}_{4}\left(l\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{SnCl}}_{4}\left(g\right)\)

(b) \({\text{CS}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{CS}}_{2}\left(l\right)\)

(c) \(\text{Cu}\left(s\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}\text{Cu}\left(g\right)\)

(d) \({\text{H}}_{2}\text{O}\left(l\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{H}}_{2}\text{O}\left(g\right)\)

(e) \(2{\text{H}}_{2}\left(g\right)+{\text{O}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2{\text{H}}_{2}\text{O}\left(l\right)\)

(f) \(2\text{HCl}\left(g\right)+\text{Pb}\left(s\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{PbCl}}_{2}\left(s\right)+{\text{H}}_{2}\left(g\right)\)

(g) \(\text{Zn}\left(s\right)+{\text{CuSO}}_{4}\left(s\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}\text{Cu}\left(s\right)+{\text{ZnSO}}_{4}\left(s\right)\)

(a) 107 J/K; (b) −86.4 J/K; (c) 133.2 J/K; (d) 118.8 J/K; (e) −326.6 J/K; (f) −171.9 J/K; (g) −7.2 J/K

Determine the entropy change for the combustion of liquid ethanol, C₂H₅OH, under standard state conditions to give gaseous carbon dioxide and liquid water.

Determine the entropy change for the combustion of gaseous propane, C₃H₈, under standard state conditions to give gaseous carbon dioxide and water.

100.6 J/K

“Thermite” reactions have been used for welding metal parts such as railway rails and in metal refining. One such thermite reaction is \({\text{Fe}}_{2}{\text{O}}_{3}\left(s\right)+2\text{Al}\left(s\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{Al}}_{2}{\text{O}}_{3}\left(s\right)+2\text{Fe}\left(s\right).\)
Is the reaction spontaneous at room temperature under standard conditions? During the reaction, the surroundings absorb 851.8 kJ/mol of heat.

Using the relevant \({S}_{298}^{°}\) values listed in Appendix G, calculate \(\text{Δ}{S}_{298}^{°}\)
for the following changes:

(a) \({\text{N}}_{2}\left(g\right)+3{\text{H}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2{\text{NH}}_{3}\left(g\right)\)

(b) \({\text{N}}_{2}\left(g\right)+\phantom{\rule{0.2em}{0ex}}\frac{5}{2}{\text{O}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}{\text{N}}_{2}{\text{O}}_{5}\left(g\right)\)

(a) −198.1 J/K; (b) −348.9 J/K

From the following information, determine \(\text{Δ}{S}_{298}^{°}\) for the following:

\(\text{N}\left(g\right)+\text{O}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}\text{NO}\left(g\right)\phantom{\rule{5em}{0ex}}\text{Δ}{S}_{298}^{°}=?\)

\({\text{N}}_{2}\left(g\right)+{\text{O}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2\text{NO}\left(g\right)\phantom{\rule{5em}{0ex}}\text{Δ}{S}_{298}^{°}=\text{24.8 J/K}\)

\({\text{N}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2\text{N}\left(g\right)\phantom{\rule{5em}{0ex}}\text{Δ}{S}_{298}^{°}=\text{115.0 J/K}\)

\({\text{O}}_{2}\left(g\right)\phantom{\rule{0.2em}{0ex}}⟶\phantom{\rule{0.2em}{0ex}}2\text{O}\left(g\right)\phantom{\rule{5em}{0ex}}\text{Δ}{S}_{298}^{°}=\text{117.0 J/K}\)

By calculating ΔS_univ at each temperature, determine if the melting of 1 mole of NaCl(s) is spontaneous at 500 °C and at 700 °C.

\({S}_{\text{NaCl}\left(s\right)}^{°}=72.11\frac{\text{J}}{\text{mol·K}}\phantom{\rule{3em}{0ex}}{S}_{\text{NaCl}\left(l\right)}^{°}=95.06\phantom{\rule{0.2em}{0ex}}\frac{\text{J}}{\text{mol·K}}\phantom{\rule{3em}{0ex}}\text{Δ}{H}_{\text{fusion}}^{°}=\text{27.95 kJ/mol}\)

What assumptions are made about the thermodynamic information (entropy and enthalpy values) used to solve this problem?

As ΔS_univ < 0 at each of these temperatures, melting is not spontaneous at either of them. The given values for entropy and enthalpy are for NaCl at 298 K. It is assumed that these do not change significantly at the higher temperatures used in the problem.

Use the standard entropy data in Appendix G to determine the change in entropy for each of the reactions listed in [link]. All are run under standard state conditions and 25 °C.

(a) 2.86 J/K; (b) 24.8 J/K; (c) −113.2 J/K; (d) −24.7 J/K; (e) 15.5 J/K; (f) 290.0 J/K

Glossary

second law of thermodynamics: entropy of the universe increases for a spontaneous process

standard entropy (S°): entropy for a substance at 1 bar pressure; tabulated values are usually determined at 298.15 K and denoted \({S}_{298}^{°}\)

standard entropy change (ΔS°): change in entropy for a reaction calculated using the standard entropies, usually at room temperature and denoted \(\text{Δ}{S}_{298}^{°}\)

third law of thermodynamics: entropy of a perfect crystal at absolute zero (0 K) is zero

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