1. The Clausius Inequality: The theorem states that for any thermodynamic cycle, the cyclic integral of $\frac{dQ}{T}$ must satisfy:
$$\oint \frac{dQ}{T} \leq 0$$
2. Interpreting the Integral: The value of this cyclic integral tells us about the nature of the cycle:
• Case 1 (Reversible Cycle): If the cycle is perfectly reversible (no friction, no rapid expansions, and heat transfer only across infinitesimal temperature differences), then:
$$\oint \frac{dQ}{T} = 0$$
• Case 2 (Irreversible Cycle): If there are any internal or external irreversibilities (which occur in all real-world processes), then:
$$\oint \frac{dQ}{T} \lt 0$$
• Case 3 (Impossible Cycle): If the integral is greater than zero, the cycle violates the Second Law of Thermodynamics.