Entropy Change Calculator
Calculate entropy change for isothermal, heating, phase change, and mixing processes.
Entropy Tracks Energy Dispersal and Thermodynamic Irreversibility
Entropy is a state function whose change can be calculated along a convenient reversible path even when the real process is irreversible. For reversible heat transfer, dS=δQrev/T. Heating an idealized material with constant heat capacity gives ΔS=mc ln(T2/T1), while an isothermal phase change gives ΔS=Qrev/T=ΔH/T.
For an isolated system, total entropy cannot decrease. A reversible process produces no entropy, while real friction, finite-temperature heat transfer, mixing, and other irreversible processes generate entropy. Entropy change of one subsystem can be negative as long as the total change of system plus surroundings satisfies the second law.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| S | Entropy | J/K. |
| Qrev | Reversible heat transfer | J along a reversible path. |
| T | Absolute temperature | K. |
| c | Specific heat capacity | J/(kg·K) for the constant-c heating approximation. |
Entropy is not directly “disorder” in a mechanical sense. In thermodynamics it quantifies the number or distribution of accessible energy states and constrains which macroscopic processes can occur spontaneously.
Entropy-change signs should follow the chosen system and process. Heating a body through a positive temperature rise gives a positive entropy change, while cooling gives a negative one. For mixing ideal components, the entropy of mixing should be nonnegative; a negative result usually indicates a sign or mole-fraction error.
Worked Examples
Common Mistakes
Temperature ratios and denominators in thermodynamics require absolute Kelvin temperature.
Irreversible adiabatic processes can generate entropy even though Q=0.
A subsystem can decrease in entropy if surroundings increase by enough to keep total entropy production nonnegative.
Frequently Asked Questions
Formula Explorer connections
Interpretation: This formula tracks heat, temperature, work, entropy or transport in a thermodynamic system. Assumption: Use absolute temperature where required and consistent energy units. Constant properties, equilibrium, ideal gases or negligible losses may be assumed.