Entropy | Sahithyan's Notes

Emerged from 2nd law of thermodynamics. Denoted by $S$ . Not a conserved property.

There exists a property of a closed system such that a change in its value is equal to $\int_1^2 \frac{\delta Q}{T}$ , for any reversible process undergone by the system between state 1 and state 2.

\Delta S = \int_1^2 \frac{\delta Q}{T}

For Reversible Process

\Delta S = \frac{\delta Q}{T}

Here:

$\Delta S$: the change in entropy
$\delta Q$: the heat transfer
$T$: the absolute temperature

For Irreversible Process

Entropy change of an irreversible process cannot be found. Entropy always increases.

Clausius Inequality

Also known as Clausius theorem. For a thermodynamic system exchanging heat with external thermal reservoirs, and undergoing a thermodynamic cycle, the following inequality holds:

\oint \frac{\delta Q}{T} \leq 0

If the the cycle is reversible, the inequality becomes an equality:

\oint \frac{\delta Q}{T} = \begin{cases} \lt 0 & \text{cycle is irreversible} \\ = 0 & \text{cycle is reversible} \\ \gt 0 & \text{cycle is impossible} \end{cases}

Principle of Increase of Entropy

For an isolated system, the entropy of the system never decreases. If the process undergone by the system is reversible, entropy remains constant. If the process is irreversible, entropy increases.

\Delta S_\text{isolated} \geq 0