Ericsson cycle- question concerning entropy

  • Thread starter Thread starter trelek2
  • Start date Start date
  • Tags Tags
    Cycle Entropy
AI Thread Summary
In an Ericsson cycle, if heat is transferred during isobaric processes via direct thermal contact with constant temperature reservoirs, the change in entropy of the working substance is not zero, as entropy is generated and later transferred to the reservoirs. The overall change in entropy for the working substance around a closed cycle is always zero, regardless of whether the processes are reversible or irreversible, because the working fluid returns to its initial thermodynamic state. When calculating the change in entropy of the universe for the cycle, assuming reversible processes results in zero entropy change, while irreversible processes yield a positive change. Thus, the assumptions made about the processes significantly impact the entropy calculations. Understanding these principles is crucial for analyzing thermodynamic cycles accurately.
trelek2
Messages
86
Reaction score
0
Hi!

I have trouble with the following:
1)
Consider an ericsson cycle. It is easy to calculate the change of entropy of the working substance during the isothermal parts. But assuming that all the heat transferred/removed from the working substance during the isobaric processes is done by direct thermal contact with reservoirs at constant temperatures A and B, does this imply the change of entropy of the working substances to be 0?

2)
If we don't make the above assumption, adding all the processes of the ericsson cycle together give a net change of entropy to be 0. Why does the change of entropy of a working substance taken around a closed cycle (even including irreversible processes) is always equal to 0?

3) A corrolary question: When calculating the change of entropy of the universe when the ericsson engine goes around one cycle should I make the assumption as stated in 1)? Otherwise the change of entropy of the universe would be 0, right?
 
Science news on Phys.org
trelek2 said:
Hi!

I have trouble with the following:
1)
Consider an ericsson cycle. It is easy to calculate the change of entropy of the working substance during the isothermal parts. But assuming that all the heat transferred/removed from the working substance during the isobaric processes is done by direct thermal contact with reservoirs at constant temperatures A and B, does this imply the change of entropy of the working substances to be 0?
If the working fluid is in contact with constant temperature reservoirs during the isobaric segments of the process, then entropy will be generated within the working fluid. However, by the ends of these steps, the generated entropy will get transferred to the reservoirs. That is, if the end points at beginning and end of the isobaric segments are independent of whether the steps are reversible or irreversible, the entropy change for the working fluid is the same in both cases. But the entropy changes of the reservoirs will be different.
2)
If we don't make the above assumption, adding all the processes of the ericsson cycle together give a net change of entropy to be 0. Why does the change of entropy of a working substance taken around a closed cycle (even including irreversible processes) is always equal to 0?
Entropy is an inherent physical property of the working fluid, independent of any process. So if, at the end of a cycle, the working fluid is in the same thermodynamic state as at the beginning (which is guaranteed, since we are calling it a cycle), the entropy change over the cycle is zero.
3) A corrolary question: When calculating the change of entropy of the universe when the ericsson engine goes around one cycle should I make the assumption as stated in 1)? Otherwise the change of entropy of the universe would be 0, right?
If the cycle is carried out reversibly, the change in entropy of the universe will be zero. If the cycle is carried out irreversibly, the change in entropy of the universe will be positive.
 
I was watching a Khan Academy video on entropy called: Reconciling thermodynamic and state definitions of entropy. So in the video it says: Let's say I have a container. And in that container, I have gas particles and they're bouncing around like gas particles tend to do, creating some pressure on the container of a certain volume. And let's say I have n particles. Now, each of these particles could be in x different states. Now, if each of them can be in x different states, how many total...
Thread 'Why work is PdV and not (P+dP)dV in an isothermal process?'
Let's say we have a cylinder of volume V1 with a frictionless movable piston and some gas trapped inside with pressure P1 and temperature T1. On top of the piston lay some small pebbles that add weight and essentially create the pressure P1. Also the system is inside a reservoir of water that keeps its temperature constant at T1. The system is in equilibrium at V1, P1, T1. Now let's say i put another very small pebble on top of the piston (0,00001kg) and after some seconds the system...
Back
Top