General Chemistry II · Chemical Thermodynamics
The Second Law of Thermodynamics
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In 30 seconds
The Second Law of Thermodynamics states that for any spontaneous process, the total entropy of the universe increases: ΔS_universe > 0. The universe is the system plus its surroundings, so ΔS_universe = ΔS_system + ΔS_surroundings. A spontaneous process may decrease the system's entropy (water freezing) as long as the surroundings' entropy increases by more. At equilibrium, ΔS_universe = 0. This is the fundamental, universal test of spontaneity — more fundamental than ΔG, which is a convenience derived from it.
Why this matters
The Second Law is arguably the most far-reaching law in science: it dictates the direction of heat flow, the arrow of time, the maximum efficiency of engines and refrigerators, and why perpetual-motion machines are impossible. In chemistry, it is the reason we can build spontaneity into a single handy criterion (ΔG) and predict reaction direction under any conditions.
The college version
Core Concept
The Second Law of Thermodynamics states that for any spontaneous process, the total entropy of the universe increases: ΔS_universe > 0. The universe is the system plus its surroundings, so ΔS_universe = ΔS_system + ΔS_surroundings. A spontaneous process may decrease the system's entropy (water freezing) as long as the surroundings' entropy increases by more. At equilibrium, ΔS_universe = 0. This is the fundamental, universal test of spontaneity — more fundamental than ΔG, which is a convenience derived from it.
Key Ideas
- Universe = system + surroundings. The surroundings are everything outside the system that can exchange heat with it.
- The decisive quantity. A process is spontaneous if and only if ΔS_universe > 0; it is at equilibrium when ΔS_universe = 0.
- Heat transfer drives ΔS_surroundings. For a process at constant temperature, ΔS_surroundings = −ΔH_system / T.
- Exothermic favors spontaneity. When ΔH_system < 0, the surroundings gain heat, so ΔS_surroundings > 0 — an exothermic reaction pushes the universe toward higher entropy.
- Temperature moderates the effect. The same heat transfer produces a larger surroundings-entropy change at low T than at high T (dividing by T).
Equations and Variables
| Symbol | Meaning | Common units |
|---|---|---|
| ΔS_univ | Entropy change of the universe | J/(mol·K) |
| ΔS_sys | Entropy change of the system | J/(mol·K) |
| ΔS_surr | Entropy change of the surroundings | J/(mol·K) |
| ΔH_sys | Enthalpy change of the system | J/mol |
| T | Absolute temperature | K |
ΔS_univ = ΔS_sys + ΔS_surr, with ΔS_surr = −ΔH_sys / T.
How It Works
- Any process transfers energy and redistributes matter between the system and surroundings.
- Compute the system's entropy change (from tables or ΔS = q_rev/T for reversible paths).
- Compute the surroundings' change: heat −ΔH_sys leaves or enters the surroundings, changing its entropy by −ΔH_sys/T.
- Add the two. If the sum is positive, the process is spontaneous; if zero, equilibrium; if negative, the process is nonspontaneous (its reverse is spontaneous).
Worked Example
Is ice melting spontaneous at 25 °C? Use ΔS_universe.
Melting: H₂O(s) → H₂O(l), with ΔH_fus = +6.01 kJ/mol = +6010 J/mol.
- ΔS_sys = ΔH_fus / T_m = 6010 J/mol ÷ 273 K = +22.0 J/(mol·K) (entropy increases on melting).
- ΔS_surr = −ΔH_sys / T = −6010 J/mol ÷ 298 K = −20.2 J/(mol·K) (surroundings lose heat to the endothermic melting).
- ΔS_univ = +22.0 + (−20.2) = +1.8 J/(mol·K) > 0, so melting is spontaneous at 25 °C.
At exactly 0 °C (273 K), ΔS_surr = −6010/273 = −22.0 J/(mol·K), making ΔS_univ = 0 — the melting point is the equilibrium (phase-transition) temperature.
How it works
- Any process transfers energy and redistributes matter between the system and surroundings.
- Compute the system's entropy change (from tables or ΔS = q_rev/T for reversible paths).
- Compute the surroundings' change: heat −ΔH_sys leaves or enters the surroundings, changing its entropy by −ΔH_sys/T.
- Add the two. If the sum is positive, the process is spontaneous; if zero, equilibrium; if negative, the process is nonspontaneous (its reverse is spontaneous).
Common confusions
- "The entropy of the system must increase for any spontaneous process." — Wrong. Only ΔS_universe must increase; water freezing is spontaneous with ΔS_sys < 0.
- "ΔS_surroundings = ΔH/T." — Wrong sign. Heat leaving the system (exothermic) increases surroundings entropy, so ΔS_surr = −ΔH_sys/T.
- "Temperature can be in °C." — Wrong. Must use Kelvin; using °C gives nonsense (and division by zero near 0 °C).
- "ΔS_universe = 0 means nothing is happening." — Wrong. It means the system is at equilibrium — forward and reverse processes balance.
- "The Second Law forbids local order." — Wrong. Local order (crystallization, life) can and does form; it is always paid for by a larger entropy increase elsewhere.
Quick review
- Second Law: spontaneous ⇒ ΔS_universe > 0; equilibrium ⇒ ΔS_universe = 0.
- ΔS_univ = ΔS_sys + ΔS_surr.
- ΔS_surr = −ΔH_sys/T (Kelvin).
- Exothermic helps spontaneity by raising surroundings entropy.
- A decrease in system entropy can still be spontaneous if surroundings entropy rises more.

Eli explains
The same idea, in plain words
Explain it like I’m 10
Imagine the universe as two connected rooms: your bedroom (the system) and the rest of the house (the surroundings). You can make your bedroom tidy (low entropy) — but only by dumping all the mess into the hallway, which gets messier. The Second Law says the whole house never gets tidier on its own. Spontaneous things happen because the total mess — system plus surroundings — always grows. (The limit: "mess" here really means energy spread among microscopic arrangements, and "temperature" decides how much the hallway's mess grows when you throw heat into it.)
Worked example
Worked Example
Is ice melting spontaneous at 25 °C? Use ΔS_universe.
Melting: H₂O(s) → H₂O(l), with ΔH_fus = +6.01 kJ/mol = +6010 J/mol.
- ΔS_sys = ΔH_fus / T_m = 6010 J/mol ÷ 273 K = +22.0 J/(mol·K) (entropy increases on melting).
- ΔS_surr = −ΔH_sys / T = −6010 J/mol ÷ 298 K = −20.2 J/(mol·K) (surroundings lose heat to the endothermic melting).
- ΔS_univ = +22.0 + (−20.2) = +1.8 J/(mol·K) > 0, so melting is spontaneous at 25 °C.
At exactly 0 °C (273 K), ΔS_surr = −6010/273 = −22.0 J/(mol·K), making ΔS_univ = 0 — the melting point is the equilibrium (phase-transition) temperature.
Key takeaways
- ### High-Yield Facts
- Second Law: ΔS_universe > 0 for spontaneous processes, = 0 at equilibrium.
- ΔS_univ = ΔS_sys + ΔS_surr.
- ΔS_surr = −ΔH_sys / T (T in Kelvin).
- Exothermic reactions (ΔH < 0) increase the surroundings' entropy, favoring spontaneity.
- A process can be spontaneous even when ΔS_sys < 0, if ΔS_surr > 0 outweighs it (e.g., water freezing).
- ΔS_univ < 0 means the process is nonspontaneous (the reverse is spontaneous).
- ΔG = −T·ΔS_univ, which is why ΔG < 0 ⇔ ΔS_univ > 0.
Quick check
2 questions here. Answers stay hidden until you check.
The third law of thermodynamics states that:
Study tools & related lessonsYou’ll learn to · Related
You’ll learn to
- State the Second Law of Thermodynamics in terms of the entropy of the universe.
- Explain the difference between ΔS_system, ΔS_surroundings, and ΔS_universe.
- Calculate ΔS_surroundings from the enthalpy change and temperature.
- Use ΔS_universe to judge whether a process is spontaneous or at equilibrium.
Sources & references
- OpenStax, *Chemistry 2e*, Ch. 16.3 "The Second and Third Laws of Thermodynamics." https://openstax.org/books/chemistry-2e/pages/16-3-the-second-and-third-laws-of-thermodynamics
- OpenStax, *Chemistry 2e*, Ch. 16.2 "Entropy." https://openstax.org/books/chemistry-2e/pages/16-2-entropy
- NIST Chemistry WebBook. https://webbook.nist.gov/chemistry/
This lesson was adapted from the open educational references above; their licenses and attributions are preserved. See Copyright & Licensing.
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