Post

Created by @nathanedwards
 at November 3rd 2023, 10:33:47 am.

AP Physics 2 Exam Question

A heat engine operates between two reservoirs at temperatures of 400 K and 800 K. During each cycle, 100 J of heat is absorbed from the high-temperature reservoir and 80 J of heat is exhausted to the low-temperature reservoir. Determine:

(a) The efficiency of this heat engine.

(b) The entropy change for the entire cycle.

Answer

(a) The efficiency of a heat engine can be calculated using the equation:

Efficiency=Work done by the engineHeat absorbed from the high-temperature reservoir\text{{Efficiency}} = \frac{{\text{{Work done by the engine}}}}{{\text{{Heat absorbed from the high-temperature reservoir}}}}

In this case, the work done by the engine is given by:

Work=Heat absorbed−Heat rejected\text{{Work}} = \text{{Heat absorbed}} - \text{{Heat rejected}}

Therefore, the efficiency is:

Efficiency=Heat absorbed−Heat rejectedHeat absorbed\text{{Efficiency}} = \frac{{\text{{Heat absorbed}} - \text{{Heat rejected}}}}{{\text{{Heat absorbed}}}}

Substituting the given values:

Efficiency=100 J−80 J100 J=20 J100 J=0.2 (20%)\text{{Efficiency}} = \frac{{100 \, \text{J} - 80 \, \text{J}}}{{100 \, \text{J}}} = \frac{{20 \, \text{J}}}{{100 \, \text{J}}} = 0.2 \, (20\%)

So, the efficiency of this heat engine is 20%.

(b) The entropy change for the entire cycle can be determined using the equation:

ΔS=QrevT\Delta S = \frac{{Q_{\text{{rev}}}}}{{T}}

where ΔS\Delta S is the entropy change, QrevQ_{\text{{rev}}} is the heat absorbed or rejected in a reversible process, and TT is the temperature of the reservoir.

For the heat absorbed from the high-temperature reservoir, Qrev=100 JQ_{\text{{rev}}} = 100 \, \text{J}. The temperature of the high-temperature reservoir is T=400 KT = 400 \, \text{K}.

Therefore, the entropy change for the heat absorbed is:

ΔSabsorbed=QrevT=100 J400 K\Delta S_{\text{{absorbed}}} = \frac{{Q_{\text{{rev}}}}}{{T}} = \frac{{100 \, \text{J}}}{{400 \, \text{K}}}

For the heat rejected to the low-temperature reservoir, Qrev=80 JQ_{\text{{rev}}} = 80 \, \text{J}. The temperature of the low-temperature reservoir is T=800 KT = 800 \, \text{K}.

Therefore, the entropy change for the heat rejected is:

ΔSrejected=QrevT=80 J800 K\Delta S_{\text{{rejected}}} = \frac{{Q_{\text{{rev}}}}}{{T}} = \frac{{80 \, \text{J}}}{{800 \, \text{K}}}

Now, to calculate the total entropy change for the entire cycle, we add the entropy changes for the heat absorbed and rejected:

ΔStotal=ΔSabsorbed+ΔSrejected\Delta S_{\text{{total}}} = \Delta S_{\text{{absorbed}}} + \Delta S_{\text{{rejected}}}

ΔStotal=100 J400 K+80 J800 K=1 J4 K+1 J10 K=5+220=720\Delta S_{\text{{total}}} = \frac{{100 \, \text{J}}}{{400 \, \text{K}}} + \frac{{80 \, \text{J}}}{{800 \, \text{K}}} = \frac{{1 \, \text{J}}}{{4 \, \text{K}}} + \frac{{1 \, \text{J}}}{{10 \, \text{K}}} = \frac{{5 + 2}}{20} = \frac{{7}}{20}

Therefore, the entropy change for the entire cycle is 720 J/K\frac{7}{20} \, \text{J/K}.

Thus, the answers to the given questions are:

(a) The efficiency of this heat engine is 20%.

(b) The entropy change for the entire cycle is 720 J/K\frac{7}{20} \, \text{J/K}.