| 4A-3 : | Quasi-Equilibrium Compression of Ammonia | 4 pts |
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| Ammonia vapor is compressed inside a cylinder by an external force acting on the piston. The ammonia is initially at 30°C and 500 kPa. The final pressure is 1400 kPa. | |||||||||
| a.) | Determine the work done by the ammonia in the process. | ||||||||
| b.) | What is the final temperature of the ammonia ? | ||||||||
| The following data have been measured for the process. | |||||||||
| P (kPa) | 500 |
653 |
802 |
945 |
1100 |
1248 |
1400 |
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| V (L) | 1.25 |
1.08 |
0.96 |
0.84 |
0.72 |
0.60 |
0.50 |
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| Read : | The key concept here is that boundary or PV work is represented by the area under the process path curve on a PV Diagram. So, once we plot the given data on a PV Diagram, all we need to do is numerically integrate to determine the area under the curve and we will have know the work ! | ||||||||
| We can use the Ammonia Tables on the NIST WebBook to determine the final temperature because we know both Pfinal and Vfinal. But we don't know the number of moles in the system. Fortunately, we can use the initial state P1, V1, and T1 to determine the number of moles in this closed system. | |||||||||
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| Given: | P (kPa) |
V (L) |
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500 |
1.25 |
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653 |
1.08 |
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802 |
0.96 |
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945 |
0.84 |
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1100 |
0.72 |
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1248 |
0.60 |
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1400 |
0.50 |
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| T1 = | 30 |
oC | |||||||
| Find: | T2 = | ??? |
oC | ||||||
| Assumptions: | - Each state in the data table is an equilibrium state. | ||||||||
| - The process is a quasi-equilibrium process. | |||||||||
| - The system is a closed system. | |||||||||
| - The trapezoidal rule gives an acceptable estimate of the area under the process path in the PV Diagram | |||||||||
| Part a.) | The area of each trapezoid under the process path in the PV Diagram is the product of the average pressure for that trapezoid and the change in volume across the trapezoid. | ||||||||
Trapezoid |
Pavg (kPa) |
ΔV (L) |
W (J) |
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A |
1324 |
0.10 |
132 |
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B |
1174 |
0.12 |
141 |
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C |
1023 |
0.12 |
123 |
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D |
874 |
0.12 |
105 |
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E |
728 |
0.12 |
87 |
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F |
577 |
0.17 |
98 |
Wtotal = | 686 |
J | |||
| Part b.) | If we knew the specific volume of the ammonia in the final state, we could use the ammonia tables to determine the temperature. But, at this point all we know is the total volume in the final state. Therefore, we need to determine the mass of ammonia in the system is the same in the initial and final state. So, we can use the information we have for the initial state to determine the mass of ammonia in the system. | ||||||||
| First, look up the specific volume of ammonia in the initial state in the isothermal thermodynamic tables: | |||||||||
| V1 = | 0.28099 |
m3/kg | |||||||
| Then, to calculate mNH3, use: | ![]() |
Eqn 1 |
mNH3 = | 0.00445 | kg | ||||
| Finally, calculate V2,hat using: | Eqn 2 |
V2,hat = | 0.112396 | m3/kg | |||||
| Now, use the isobaric thermodynamic tables at a pressure of 1400 kPa. Specify a temperature range that you are sure brackets V2. Here is a table that I cut-and-pasted from the NIST WebBook. | |||||||||
T (C) |
P (MPa) |
V (m3/kg) |
Phase |
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70 |
1.4 |
0.10881 |
vapor |
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72 |
1.4 |
0.1097 |
vapor |
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74 |
1.4 |
0.11059 |
vapor |
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76 |
1.4 |
0.11148 |
vapor |
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78 |
1.4 |
0.11236 |
vapor |
V2 falls between 78oC and 80oC | |||||
80 |
1.4 |
0.11323 |
vapor |
So, now, we must interpolate. | |||||
Answer: |
T2 = | 78.1 | oC | ||||||

