| 4A-1 : |
Work for a Cycle Carried Out in a Closed System |
6 pts |
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| Air undergoes a three-process cycle. Find the net work done for 2 kg of air if the processes are : |
| Process 1-2: constant pressure expansion |
| Process 2-3: constant volume |
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| Process 3-1: constant temperature compression |
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| Sketch the cycle path on a PV Diagram. |
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| Data : |
T1 |
100 |
oC |
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T2 |
600 |
oC |
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P1 |
200 |
kPa |
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| Given: |
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100 |
oC |
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Find: |
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T2 |
600 |
oC |
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Sketch cycle on a PV Diagram. |
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P1 |
200 |
kPa |
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Wcycle = |
??? |
kJ |
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m |
2.0 |
kg |
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| Assumptions: |
- The gas is a closed system |
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- Boundary work is the only form of work interaction |
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- Changes in kinetic and potential energies are negligible. |
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- Air behaves as an ideal gas.
This must be verified at all three states. |
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| Part a.) |
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| Part b.) |
Since Wcycle = W12 + W23 + W31, we will work our way around the cycle and calculate each work term along the way. |
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Step 1-2 is isobaric, therefore, the definition of boundary work becomes: |
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Eqn 1 |
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We can simplify Eqn 1 using the fact that P2 = P1 and the Ideal Gas EOS : |
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Eqn 2 |
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Eqn 3 |
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We can determine the number of moles of air in the system from the given mass of air and its molecular weight. |
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Eqn 4 |
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MWair |
29 |
g/mole |
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n |
68.97 |
mole |
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Plug values into Eqn 3 : |
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R |
8.314 |
J/mole-K |
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W12 |
286.69 |
kJ |
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Because the volume is constant in step 2-3: |
W23 |
0 |
kJ |
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Step 3-1 is isothermal, therefore, the definition of boundary work becomes: |
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Eqn 5 |
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The problem is that we don't know either P3 or V3. Either one would be useful in evaluating W31 because we know P1 and we can determine V1 from the Ideal Gas EOS, Eqn 2. |
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We can evaluate V3 using the fact that V3 = V2. Apply the the Ideal Gas EOS to state 2. |
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Eqn 6 |
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V3 |
2.503 |
m3/mole |
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Next, we can apply Eqn 6 to state 1 : |
V1 |
1.070 |
m3/mole |
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Now, we can plug values into Eqn 4 to evaluate W13 : |
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W31 |
-181.89 |
kJ |
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Sum the work terms for the three steps to get Wcycle: |
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Wcycle = |
104.8 |
kJ |