So far, we have encountered the first two laws of thermodynamics, and now it is time to see the third. For an ideal gas, recall how entropy, energy, and temperature are related where temperature is held constant. Now when volume is also held constant, work on the system , so . By the definition of heat in terms of heat capacity . To add up all the small incremental *dS*s, .

Now, what happens as ? Then, , where if *C* is not dependent on temperature, . Then, . Since ln(0) approaches -∞, then this means that gets infinitely large as , which is not good! So, there must be some temperature dependence in the heat capacity *C*.

The **Third Law of Thermodynamics** states that heat capacity *C* must go to zero faster than *ln(0)* goes to infinity, implying . So, the multiplicity Ω where must be which implies . So a more intuitive way to state the third law would be

*There's only one configuration for a system at 0 K.*

### Playing the GameEdit

A fun way to remember the **Three Laws of Thermodynamics** is with the following way:

**0th Law**

- You must play the game

**1st Law**

- You can't win the game

**2nd Law**

- You can't even break even

**3rd Law**

- Not even on a cold day

And there you have it: the Three Laws of Thermodynamics!