Second Law of Thermodynamics - Entropy

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SUMMARY

The discussion focuses on calculating the change in entropy associated with a car engine's operation, specifically when using premium gasoline that produces 1.23×108 J of heat per gallon. The engine operates at 25% efficiency, expelling three-fourths of the heat into the air at 20.0 ºC. The calculations reveal that the total change in entropy when driving 1 mile is 850 J/K, indicating an increase in the world's entropy, consistent with the Second Law of Thermodynamics.

PREREQUISITES
  • Understanding of the Second Law of Thermodynamics
  • Familiarity with entropy calculations using the formula ΔS = Q/T
  • Knowledge of thermodynamic systems and reservoirs
  • Basic principles of heat transfer and efficiency in engines
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  • Study the implications of the Second Law of Thermodynamics in real-world applications
  • Learn about heat engines and their efficiency calculations
  • Explore the concept of thermodynamic reservoirs and their role in entropy changes
  • Investigate advanced entropy calculations involving multiple temperature reservoirs
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Students studying thermodynamics, engineers working on automotive efficiency, and anyone interested in the principles of energy transfer and entropy in physical systems.

Tynged
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Homework Statement



Premium gasoline produces 1.23×108 J of heat per gallon when it is burned at a temperature of approximately 400 ºC (although the amount can vary with the fuel mixture). If the car's engine is 25.0 % efficient, three-fourths of that heat is expelled into the air, typically at 20.0 ºC.

Part A: If your car gets 38.0 miles per gallon of gas, by how much does the car's engine change the entropy of the world when you drive 1.00 mile?

Part B: Does it decrease or increase the entropy of the world?


Homework Equations



\Delta S = S_2 - S_1 = \frac{Q}{T}

Where \Delta S is the change in entropy of the system, S_2 is the entropy of the system at its final state, S_1 is the entropy of the system at its initial state, Q is the heat added to or removed from the system, and T is the absolute temperature at which the process is occurring.


The Attempt at a Solution



\Delta S = S_2 - S_1 = \frac{Q}{T} = \frac{(0.750)(1.23\times10^{8}\ J/gal)(1.00\ mi\times\frac{1\ gal}{38.0\ mi})}{673\ K} = 3610\ J/K

I believe I went wrong when I used the temperature of the burning fuel mixture as the absolute temperature. I am sure the temperature of the surrounding air is also important somehow. Writing the equation for entropy differently, I tried to incorporate that second temperature.

\Delta S = S_2 - S_1 = \frac{Q_2}{T_2} - \frac{Q_1}{T_1} = \left(\frac{(0.750)(1.23\times10^{8}\ J/gal)(1.00\ mi\times\frac{1\ gal}{38.0\ mi})}{673\ K}\right) - \left(\frac{(0.250)(1.23\times10^{8}\ J/gal)(1.00\ mi\times\frac{1\ gal}{38.0\ mi})}{293\ K}\right)

= 3610\ J/K - 2760\ J/K = 850\ J/K

Although this seemed to be a step in the wrong direction because my first solution was closer to the correct answer according to the automatic response.

For Part B, I assume that driving the car will increase the entropy of the world since most processes I have seen naturally tend toward increasing disorder. I am sure the correct answer to Part A will be a positive change in entropy and support my assumption.

I would definitely appreciate any help you could offer. Thanks in advance!
 
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Tynged said:

The Attempt at a Solution



\Delta S = S_2 - S_1 = \frac{Q}{T} = \frac{(0.750)(1.23\times10^{8}\ J/gal)(1.00\ mi\times\frac{1\ gal}{38.0\ mi})}{673\ K} = 3610\ J/K

I believe I went wrong when I used the temperature of the burning fuel mixture as the absolute temperature. I am sure the temperature of the surrounding air is also important somehow. Writing the equation for entropy differently, I tried to incorporate that second temperature.
The total change in entropy is the change in entropy of the system + the change in entropy of the surroundings. The system keeps returning to its original state, so there is no change in the system entropy. The surroundings consist of the hot reservoir and the cold reservoir. This process can be viewed as the engine drawing heat from the hot reservoir at 400C and delivering 75% of that heat to the cold reservoir at 20C

Because heat is leaving the hot reservoir, the change in entropy of the hot reservoir is negative (dQ < 0 means dQ/T < 0). Heat is entering the cold reservoir (the air) so the entropy change of the air is positive.

\Delta S = \Delta S_{sys} + \Delta S_{surr} = 0 + \left(\frac{Q_h}{T_h} + \frac{Q_c}{T_c}\right) =

Work that out and you will have your answer.

AM
 

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