Illustrated · 2 min
Entropy is possibly the most important concept in all of thermodynamics. Unfortunately, entropy is also an incredibly difficult concept to fully grasp. This lesson will give an overview of the necessary basics, but is in no way comprehensive. For a more in depth understanding of entropy, a strong background in statistics is required.
Microstates and Macrostates
Let's play a game.
I roll a single, fair, 6 sided die. What number most likely comes up?
As you probably guessed, it's impossible to tell what I am going to roll. All of the options are equally likely.
Let's say I roll two fair 6 sided dice. What sum most likely comes up?
The answer is 7. But why exactly is that?
When we roll 2 dice, each die has 6 possible outcomes. This means that in total we have unique outcomes when we roll two dice. But if we only want the sum of the dice, we don't care if we get a result of 7 from rolling 3 and 4, or 4 and 3. We only care that the sum is 7. In more technical terms we can say that the macrostate of the system is 7, and that the particular combination (i.e. 3 and 4) is the microstate.
When we roll 2 dice, 7 may be the most likely outcome, but even the least likely outcomes, 2 and 12, show up of the time. Now let's blow this example up.

As we can see from the graphs above, as the number of dice increases, the system begins to exhibit a smaller and smaller percent of available macrostates. Imagine what the histogram of dice would look like. In physical scenarios we are typically dealing with numbers of this magnitude.
Entropy and State
People often say that entropy is a measure of the disorder of a system. This is an oversimplification. Entropy is the tendency of a system to approach the most likely macrostate. Think back to our dice. Every microstate of our dice was equally likely to occur, but when we looked at the sum, certain sums were more likely to occur than others. Particles are exactly the same. Every microstate of particles is equally likely to be observed, but the vast majority of microstates correspond to a single macrostate. Since the properties of the macrostate are what we are generally interested in, it is easier to just consider the system as the macrostate. It turns out that the relevant "dice rolls" for particles are energy, , volume, , and number of particles, . This is to say, the entropy, , of our system depends on these three variables. Mathematically, entropy is a state function, and most commonly seen in the differential form shown below.

