- #1
Grinkle
Gold Member
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- 234
If I open a new deck of cards the sequence is known.
If I shuffle them, the sequence is unknown. If I then memorize the sequence, it is again known.
State 1: New deck
State 2: Shuffled deck
State 3: Shuffled deck after I have memorized the sequence
State 4: Re-shuffled deck
I have computed the entropy difference of the deck sequence between state 1 and state 2. Many of us will have done the same as an introductory exercise in the second law of thermodynamics.
If I skip step 3 then it seems to me I must say that state 2 has equivalent entropy to state 4, but if I don't skip step 3 then it seems that delta entropy (1->2) must equal the delta entropy (2->4). Entropy really is a thermodynamic property - it is not just a mind game. Is there any way to conceptually relate the entropy of the sequence of a deck of cards to the entropy in a container of gas so they both have the same 'amount' of physical significance? One seems to be a state of mind and the other seems to be a thermodynamic property, but both share a common mathematical model.
If I shuffle them, the sequence is unknown. If I then memorize the sequence, it is again known.
State 1: New deck
State 2: Shuffled deck
State 3: Shuffled deck after I have memorized the sequence
State 4: Re-shuffled deck
I have computed the entropy difference of the deck sequence between state 1 and state 2. Many of us will have done the same as an introductory exercise in the second law of thermodynamics.
If I skip step 3 then it seems to me I must say that state 2 has equivalent entropy to state 4, but if I don't skip step 3 then it seems that delta entropy (1->2) must equal the delta entropy (2->4). Entropy really is a thermodynamic property - it is not just a mind game. Is there any way to conceptually relate the entropy of the sequence of a deck of cards to the entropy in a container of gas so they both have the same 'amount' of physical significance? One seems to be a state of mind and the other seems to be a thermodynamic property, but both share a common mathematical model.