Ericsson cycle- question concerning entropy

In summary: But in either case, the change in entropy of the working fluid will be zero, since it returns to its original state.
  • #1
trelek2
88
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?
 
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  • #2
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.
 

1. What is the Ericsson cycle?

The Ericsson cycle is a thermodynamic cycle that is used in the operation of heat engines. It was proposed by Swedish inventor John Ericsson in the 19th century and is an alternative to the more commonly known Carnot cycle.

2. How does the Ericsson cycle differ from the Carnot cycle?

The Ericsson cycle differs from the Carnot cycle in a few key ways. Firstly, the Ericsson cycle is an open cycle, meaning that the working fluid is constantly replenished. Secondly, the Ericsson cycle uses a regenerator, which is a device that stores and releases heat to improve the efficiency of the cycle. Lastly, the Ericsson cycle has a higher efficiency than the Carnot cycle due to these differences.

3. What is the role of entropy in the Ericsson cycle?

Entropy plays a crucial role in the Ericsson cycle as it is a measure of the disorder or randomness in a system. In the Ericsson cycle, the working fluid goes through a series of processes that involve changes in temperature and pressure, which in turn affect the entropy of the system. The goal of the cycle is to minimize the increase in entropy to maximize the efficiency of the engine.

4. How is the efficiency of the Ericsson cycle calculated?

The efficiency of the Ericsson cycle is calculated using the equation: Efficiency = (T1-T2)/(T1-T3), where T1 is the maximum temperature of the cycle, T2 is the minimum temperature of the cycle, and T3 is the temperature of the working fluid after it passes through the regenerator. This equation takes into account the effects of entropy and the regenerator on the efficiency of the cycle.

5. What are some real-world applications of the Ericsson cycle?

The Ericsson cycle has been used in various applications such as the Stirling engine, which is often used in solar power systems. It has also been used in refrigeration and air conditioning systems and some types of gas turbines. Additionally, the Ericsson cycle has potential applications in renewable energy systems as it can use various fuels and has a high efficiency compared to other cycles.

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