In thermodynamics, the universe is often divided into the system and its surroundings. The “system” is the part we are focused on, while the "surroundings" include everything else. When dealing with problems like calculating entropy during a phase change, it's crucial to distinguish between these two categories.
The system here refers to the ethanol undergoing vaporization. Its entropy change (\(\Delta S_{\text{sys}}\)) gives a positive value as the molecules gain freedom and disorder. On the other hand, the surroundings experience an opposite, but equal change in entropy (\(\Delta S_{\text{surr}}\)). This is because as the ethanol absorbs heat from its surroundings, the available energy in the surroundings decreases resulting in a negative entropy change. The formula used is:
- \(\Delta S_{\text{surr}} = -\frac{\Delta H_{\text{vap}}}{T}\)
The universe's net entropy change, calculated as \(\Delta S_{\text{univ}}\), is the combination of both, thus in a reversible process at equilibrium it results in zero: \(\Delta S_{\text{univ}} = 0\). This highlights how system and surroundings are intricately related.