Heat Engine and Entropy Change

In summary, the proposed engine violates the first law of thermodynamics because the work output does not match the difference between the heat input and output. It also violates the second law because its efficiency is greater than the Carnot efficiency for an engine operating between 400K and 300K. The entropy calculation does not accurately reflect the violation of the second law in this case.
  • #1
Aztral-
3
0

Homework Statement


An inventor claims to have invented an engine which operates between constant-temperature reservoirs at 400K and 300K. Data on the engine, per cycle of operation:
Qh = 200J
Qc -175J
W = 40J
Th = 400K
Tc = 300K
Of the first and second laws of thermodynamics, which (if either) does the engine violate?

Homework Equations


dE = Q - W (first law of thermodynamics, Q is heat, W is work, dE is internal energy change)
dS = Q/T (entropy change when T is constant, Q is heat, T is temperature)


The Attempt at a Solution


I understand how to do these problems in terms of the first law, using either dE = Q - W or the equivalent (since an engine is a cycle), by setting dE to zero and using W = abs(Qh) - abs(Qc)

The problem stated above thus violates the first law, because
dE = 0 = abs(Qh) - (Qc) = 200 - 175 = 25J /= 40J

but I get confused determining whether or not it violates the second law. Since entropy is a state function, the net entropy change over the course of a full cycle should be zero, correct?

I use the equation for entropy change with a constant T because the hot and cold reservoirs are at constant temperature.

The heat transfer from the hot reservoir to the engine results in an entropy change of -Qh/Th in the environment (negative because the entropy in the environment in this case is decreasing). The heat transfer from the engine to the cold reservoir after the engine does work results in an entropy change of Qc/Tc in the environment (positive because heat is being put back into the environment, thus the entropy increases).

So the net entropy change for the environment should be dS = -Qh/Th + Qc/Tc


This is where I get confused, plugging in numbers to this equation results in
-200/400 + 175/300 = 0.083J/K

Is that all there is to determining whether or not it violates the second law of thermodynamics? Whether or not the resulting dS is >= 0? My question here then is what happened to dS = 0, where did that go? Is the Work done responsible for this difference? The work done on some external thing would raise the entropy of that thing to account for the 0.083J/K increase in entropy? I'm not clear on how the work done factors into the equation for entropy change.

Thanks, I hope my question is somewhat clear.
 
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  • #2
Carnot's theorem is equivalent to the second law. It states that all heat engines will have an efficiency that is less than or equal to the Carnot efficiency.

So what is the Carnot efficiency and what is the efficiency of this proposed engine?

AM
 
  • #3
Carnot efficiency is E = 1 - Tc/Th

Which means that not all of the heat put into the system produces work.

So the efficiency of the proposed engine is

1 - (300K / 400K) = 0.25, which means that 25% of the heat put into the engine (taken from the environment) becomes work.

With that efficiency, work should be 0.25 * abs(Qc) = 43.75 which is not the correct amount as provided by the problem.

So is calculating the efficiency of the engine and verifying that the ratio of Qc to Qh is correct effectively checking whether or not it violates the second law?
 
  • #4
If the efficiency does not exceed the Carnot efficiency for an engine operating between those two temperatures, then you do not have a second law violation.

The problem with the entropy calculation as you have done it (and it is done correctly) is that it does not take into account the work that is claimed to be done. If the designer had claimed to produce 60 J of work, by taking in 200 J at 400K and expelling 175 J at 300K, this would violate the Carnot theorem and therefore violate the second law (as well as the first law of course) since the Carnot theorem follows from the second law.

AM
 
  • #5
Makes sense, though I am still not clear on where dS = 0 comes into play.
 
  • #6
Aztral- said:
Makes sense, though I am still not clear on where dS = 0 comes into play.
I am not sure what you mean by your question. dS = 0 applies to reversible processes. However, this is not a real engine so the entropy calculation is not valid.

If the proposed engine would violate the first law, the entropy calculation does not tell you whether it also would violate the second law. You cannot tell by calculating entropy whether the second law is violated. In my example where 60J of work is claimed, the entropy calculation shows positive entropy. But it would violate both the first and second laws.

AM
 

1. What is a heat engine?

A heat engine is a device that converts heat energy into mechanical work. It follows the laws of thermodynamics and operates by taking in heat from a high temperature source, converting some of it into work, and releasing the remaining heat to a lower temperature sink.

2. How does a heat engine work?

A heat engine works by using the temperature difference between a hot source and a cold sink to drive a cyclic process. This process usually involves a working fluid, such as steam or gas, which expands and contracts to produce work. The work is then used to power a machine or perform other tasks.

3. What is entropy change in a heat engine?

Entropy change in a heat engine refers to the change in the amount of disorder or randomness in the system as it operates. Entropy is a measure of the system's energy that is unavailable for work. In a heat engine, the entropy increases as heat is transferred from the hot source to the cold sink, reducing the efficiency of the engine.

4. How is efficiency related to entropy change in a heat engine?

The efficiency of a heat engine is directly related to the entropy change. The higher the entropy change, the lower the efficiency of the engine. This is because as the engine operates and transfers heat, some of the energy is lost to the surroundings due to the increase in entropy. Therefore, minimizing entropy change is essential for maximizing the efficiency of a heat engine.

5. What are some real-life examples of heat engines?

Some common examples of heat engines include car engines, steam turbines, and refrigerators. Car engines use the combustion of fuel to produce mechanical work, while steam turbines use the expansion and contraction of steam to generate electricity. Refrigerators use a heat engine cycle to transfer heat from the inside of the refrigerator to the outside, keeping the inside cool.

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