third law of thermodynamics
E183516
The third law of thermodynamics is a fundamental principle stating that the entropy of a perfect crystal approaches zero as its temperature approaches absolute zero, forming a basis for absolute entropy measurements and low-temperature physics.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Nernst heat theorem | 1 |
| Third Law of Thermodynamics | 1 |
| third law of thermodynamics canonical | 1 |
Statements (45)
| Predicate | Object |
|---|---|
| instanceOf |
law of thermodynamics
ⓘ
physical law ⓘ |
| appliesTo | perfect crystal ⓘ |
| assumes |
absence of residual configurational disorder in a perfect crystal
ⓘ
unique ground state for a perfect crystal ⓘ |
| category | fundamental law of nature ⓘ |
| compatibleWith | quantum mechanics ⓘ |
| concernsConcept | absolute zero ⓘ |
| concernsQuantity |
entropy
ⓘ
temperature ⓘ |
| contrastsWith |
First Law of Thermodynamics
ⓘ
surface form:
first law of thermodynamics
second law of thermodynamics ⓘ zeroth law of thermodynamics ⓘ |
| defines | zero point of entropy scale ⓘ |
| domain | equilibrium thermodynamics ⓘ |
| field |
low-temperature physics
ⓘ
statistical mechanics ⓘ thermodynamics ⓘ |
| formulatedBy | Walther Nernst ⓘ |
| formulationDate | early 20th century ⓘ |
| hasConsequence |
entropy change for any isothermal process tends to zero as temperature approaches absolute zero
ⓘ
establishes absolute entropy scale ⓘ heat capacities tend to zero as temperature approaches absolute zero for many systems ⓘ |
| hasInterpretation | entropy measures disorder relative to a perfectly ordered ground state ⓘ |
| hasLimitation |
does not strictly apply to glasses and amorphous solids
ⓘ
does not strictly apply to systems with degenerate ground states ⓘ |
| hasName | third law of thermodynamics ⓘ |
| implies |
entropy of a perfect crystal at 0 K is zero
ⓘ
it is impossible to reach absolute zero in a finite number of steps ⓘ |
| influenced |
development of chemical thermodynamics
ⓘ
standard entropy tables ⓘ |
| mathematicalForm | S → 0 as T → 0 for a perfect crystal ⓘ |
| precedes | development of quantum statistics ⓘ |
| provides | reference point for absolute entropy ⓘ |
| relatedTo |
third law of thermodynamics
self-linksurface differs
ⓘ
surface form:
Nernst heat theorem
Nernst unattainability principle ⓘ |
| statedAs | The entropy of a perfect crystal approaches zero as its temperature approaches absolute zero. ⓘ |
| usedFor |
calculation of absolute entropies
ⓘ
calorimetric entropy measurements ⓘ determination of equilibrium constants at low temperature ⓘ |
| usedIn |
cryogenics
ⓘ
low-temperature thermodynamics ⓘ |
| usedToExplain |
behavior of specific heat at low temperatures
ⓘ
limitations on cooling processes ⓘ |
| validAt | temperatures approaching 0 K ⓘ |
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Nernst heat theorem
this entity surface form:
Third Law of Thermodynamics