harjyot said:
I know carnot's cycle is an example. but what is it exactly? a cycle in which ever part of process has a 'counter-process' please elaborate.
There are only two things that can be done to entropy. It can be moved and it can be created. "Reversal" refers only to reversal of the motion of entropy.
In a reversible cyclic process, entropy is not created. However, a reversible cyclic process can move entropy from one spatial point to another.
The reverse cycle moves the entropy in the opposite direction of the original cycle. The reversal refers to motion of entropy. Since no entropy is created anyway in the original cycle, the reverse cycle doesn’t create entropy either.
In an irreversible cyclic process, entropy is created as well as moved. An irreversible cyclic process both moves some entropy from one point to another and creates extra entropy.
It should be note that irreversible engines also have a counter cycle in irreversible refrigerators. If you run the irreversible engine backwards, the direction of motion of the entropy is reversed.
The irreversible engine does work on the surroundings. However, the irreversible engine can be run backwards as a refrigerator. Then, the surroundings do work on the irreversible refrigerator. The important difference is that entropy is created in both directions. Although the motion of the entropy can be reversed, the creation of the entropy can not be reversed.
When entropy moves from a high temperature point to a low temperature point, it releases energy in the form of work. A good analogy would be in electricity. Moving an electric charge from high potential to low potential releases energy in the form of work.
The energy can be stored by any method. If no entropy is created, then moving the entropy in the opposite direction requires only the same amount of work. However, if entropy is created then more entropy has entered the low temperature point then was taken from the high temperature point. Then, more work is required to move all the entropy from low to high temperature. The energy stored is not enough to reverse the process.
A Carnot cycle is one example of a reversible cyclic process. The Carnot cycle moves entropy from one spatial point to another without making any entropy. When a scientist calculates the change of entropy per cycle in a Carnot engine, he is talking about the entropy moved from one heat reservoir to another.
Entropy can spontaneously move a certain quantity of entropy through the Carnot engine from the high temperature reservoir to the low temperature reservoir. The Carnot engine does a certain amount of work TO the surroundings in the mode. If the surroundings do the same amount of work ON the Carnot engine, the same amount of entropy will move from the low temperature reservoir to the high temperature reservoir.
The “counter cycle” to a Carnot engine cycle is a Carnot refrigerator cycle. No entropy is created. It is important to emphasize that the Carnot engine does not create any entropy at any time. The Carnot cycle moves entropy from one reservoir to the other. If the Carnot cycle spontaneously moves entropy from hot to cold, the cycle acts as an engine by doing work on the surroundings. If work is done by the surroundings to move entropy from cold reservoir to a hot reservoir, it is working as a refrigerator.
Real engines are irreversible. They both move entropy and make entropy.
“Spontaneous” means to happen without work being done on the cycle. Entropy can spontaneously move from a region of high temperature to a region of low temperature. Entropy can not spontaneously move from a region of low temperature to a region of high temperature.
Here is a link and quotation stating that a reversible engine does not make entropy.
http://web.chem.ucsb.edu/~genchem/Chem1BW03/moreinfo/ch.10-entropy.pdf
“In a reversible, cyclic “process both the system and the surroundings are returned exactly to their original conditions. In an irreversible process, even if the process is cyclic (state 1 —> state 2 —> state 1), the surroundings are changed in a permanent way. Work is converted to heat in the surroundings. All real processes are irreversible. A reversible process gives us the maximum work obtainable from the gas.
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1) In a reversible process the total entropy of a system plus its surroundings is unchanged, Suniv = 0.
2) In an irreversible process the total entropy of a system plus its surroundings must increase, Suniv > 0.
3) A process for which Stot < 0 is impossible. (The process is spontaneous in the opposite direction.)”