15.7 Statistical Interpretation of Entropy and the Second Law of Thermodynamics: The Underlying Explanation
3 min read•june 18, 2024
is all about disorder and randomness in systems. It's like measuring how messy your room is on a molecular level. The more ways particles can be arranged, the higher the entropy. This concept is key to understanding how energy flows and changes in the universe.
helps us make sense of entropy. By looking at the of different arrangements, we can predict how systems will behave over time. This approach connects the microscopic world of atoms to the macroscopic world we experience every day.
Statistical Interpretation of Entropy
Statistical nature of entropy
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Entropy measures disorder or randomness in a system
Higher entropy signifies more disorder and randomness (gas molecules randomly distributed in a container)
Lower entropy signifies more order and less randomness (a crystal structure with atoms arranged in a regular pattern)
Entropy relates to the number of possible microscopic arrangements () of a system
A system with more possible microstates has higher entropy (a deck of cards in random order)
A system with fewer possible microstates has lower entropy (a deck of cards in a specific order)
The states that the total entropy of an isolated system always increases over time
Systems naturally tend towards states of higher probability with more microstates (a broken glass will not spontaneously reassemble)
Entropy increases until the system reaches with the maximum number of possible microstates (a hot object in a cold room will eventually reach thermal equilibrium)
This tendency defines the , indicating the direction of time's flow in physical processes
Probability of macrostates
A describes the overall state of a system (temperature, pressure, and volume)
Each macrostate can have multiple microstates associated with it
The probability of a particular macrostate is proportional to the number of microstates associated with it
with more microstates are more probable than those with fewer microstates (a fair coin has a 50% probability of landing on heads or tails)
For a simple system with N particles and M possible states for each particle, the total number of microstates is MN
The probability of a specific macrostate with n1 particles in state 1, n2 particles in state 2, etc., is given by the :
P(n1,n2,...,nM)=n1!n2!...nM!N!(M1)N
Example: for a system with 4 particles and 2 possible states, the probability of having 2 particles in each state is 2!2!4!(21)4=166=0.375
The suggests that, over long periods, the time spent by a system in a particular is proportional to the probability of that microstate
Entropy and microstate quantity
Entropy directly relates to the number of possible microstates in a system
The relates entropy (S) to the number of microstates (Ω):
S=kBlnΩ
kB is the Boltzmann constant, which has a value of 1.38×10−23 J/K
This equation, developed by , forms the foundation of statistical mechanics
A system with more microstates has higher entropy, while a system with fewer microstates has lower entropy (a shuffled deck of cards has higher entropy than a sorted deck)
As a system evolves towards equilibrium, it moves towards the macrostate with the largest number of microstates, which corresponds to the highest entropy (a drop of ink in water will diffuse until it reaches a uniform concentration)
The can be interpreted as the natural tendency of a system to move towards the most probable macrostate with the highest entropy (a room will become more disordered over time if not cleaned)
Entropy and Information
provides a complementary perspective on entropy
Entropy can be viewed as a measure of the information content or uncertainty in a system
The concept of is closely tied to information loss in thermodynamic processes
Irreversible processes lead to an increase in entropy and a loss of information about the system's initial state