second law of thermodynamics
E700593
The second law of thermodynamics is a fundamental physical principle stating that the total entropy of an isolated system can never decrease over time, establishing the direction of natural processes and the concept of irreversibility.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Second Law of Thermodynamics | 1 |
| second law of thermodynamics canonical | 1 |
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
law of thermodynamics
ⓘ
physical law ⓘ |
| alsoKnownAs | law of entropy increase ⓘ |
| appliesTo | macroscopic systems ⓘ |
| ClausiusStatement | heat cannot spontaneously flow from a colder body to a hotter body ⓘ |
| concerns |
entropy
ⓘ
irreversibility ⓘ isolated systems ⓘ spontaneous processes ⓘ |
| constrains |
direction of chemical reactions in isolated systems
ⓘ
possible thermodynamic processes ⓘ |
| describes | entropy increase in isolated systems ⓘ |
| entropyStatement | the entropy of an isolated system tends to increase and approaches a maximum ⓘ |
| field |
physics
ⓘ
thermodynamics ⓘ |
| formulation |
Clausius statement
NERFINISHED
ⓘ
Kelvin–Planck statement NERFINISHED ⓘ entropy statement ⓘ statistical mechanics formulation ⓘ |
| foundationFor |
concept of free energy in spontaneous processes
ⓘ
non-equilibrium thermodynamics ⓘ thermodynamic definition of temperature ⓘ |
| historicallyDevelopedBy |
Ludwig Boltzmann
NERFINISHED
ⓘ
Rudolf Clausius NERFINISHED ⓘ William Thomson, 1st Baron Kelvin NERFINISHED ⓘ |
| implies |
Carnot efficiency is the maximum efficiency of a heat engine operating between two temperatures
NERFINISHED
ⓘ
efficiency limits for heat engines ⓘ existence of a preferred direction of time ⓘ heat flows spontaneously from hot to cold ⓘ natural processes are irreversible ⓘ perpetual motion machines of the second kind are impossible ⓘ there is a thermodynamic arrow of time ⓘ |
| KelvinPlanckStatement | it is impossible to construct a cyclic engine whose sole effect is to convert heat from a single reservoir completely into work ⓘ |
| mathematicalForm | dS ≥ δQ_rev / T for closed systems ⓘ |
| predicts | entropy production in irreversible processes ⓘ |
| relatedConcept |
Boltzmann entropy
NERFINISHED
ⓘ
entropy ⓘ heat death of the universe ⓘ microstates and macrostates ⓘ thermodynamic equilibrium ⓘ |
| states | the total entropy of an isolated system never decreases over time ⓘ |
| statisticalNature | it is overwhelmingly probable rather than absolutely unavoidable ⓘ |
| timePeriodOfDevelopment | 19th century ⓘ |
| usedIn |
design of heat engines
ⓘ
information theory analogies ⓘ refrigeration cycles ⓘ statistical mechanics ⓘ |
Referenced by (2)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Second Law of Thermodynamics