Thermodynamics - Heat Engine Cycle

In summary, the heat increase from 2 to 3 is 8.32T1, the increase from 3 to 1 is 8.32T2, and the change in heat from 1 to 2 is 350T3.
  • #1
azukibean
18
0

Homework Statement


n = 5 moles, monatomic, ideal gas
p1 = 7280 Pa; v1 = 2 m3
p2 = 7280; v2 = 6
p3 = 6500; v3 = 6

What is the change in heat, from 2 to 3, and from 3 to 1?

Homework Equations


PV = nRT
U = (3/2)nRT
Q = du + dw

The Attempt at a Solution



PV = nRT
(7280)(2) = (5)(8.32)T1

T1 = 350 (correct)
T2= 1050 (correct)
T3 = 937.5 (correct)

U = (3/2)nRT
U1 = (3/2)(5)(8.32)(350) = 21840
U2 = 65520
U3 = 57796.88

W1 = 29120
W2 = 0
W3 = -27560
(all correct)

Q = du + dw
ΔQ1 to 2 = (65520-21840) + 29120 = 72800 (correct)
ΔQ2 to 3 = (57796.88-65520) + 0 = -7723.12 (correct: -7020)
ΔQ3 to 1 (21840-57796.88) - 27560 = -63516.88 (correct: -64220)

This is driving me nuts. I can get the first heat quantity right, but not the next two. I've triple checked my work (though that doesn't totally eliminate the possibility of an arithmetic mistake). Where am I going wrong?
 
Last edited:
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  • #2
Is Q = du + dw or is dQ = du + dw ?

How come I get T3 = 312.5 from pV = nRT ? Any chance p3 = 19500 ?
Any (other) typos or omissions (adiabatic, isothermal?) in the problem statement ?

You say W1, do you mean W##_{1\rightarrow2}## ? There I get 29120 for the work pΔV the gas is doing.
If so, why is W##_{2\rightarrow3}## = 0 ?
If so, why is W##_{3\rightarrow1}## = -27560 ? The volume does not change ?!
 
Last edited:
  • #3
BvU said:
Is Q = du + dw or is dQ = du + dw ?
The first one is correct. The heat added or subtracted is equal to the change in internal energy and work.
I'm unsure how to work the problem to find dQ; in ΔQ1→2 I equated it to Q1→2 because I assumed at "step 0" there was no heat energy.

BvU said:
How come I get T3 = 312.5 from pV = nRT ? Any chance p3 = 19500 ?
Any (other) typos or omissions (adiabatic, isothermal?) in the problem statement ?
There are no omissions. V3 should actual be 6 instead of 2. I fixed it. Sorry about that.

BvU said:
You say W1, do you mean W##_{1\rightarrow2}## ? There I get 29120 for the work pΔV the gas is doing.
If so, why is W##_{2\rightarrow3}## = 0 ?
If so, why is W##_{3\rightarrow1}## = -27560 ? The volume does not change ?!
Right.
W##_{2\rightarrow3}## = 0 because the volume does not change.
W##_{3\rightarrow1}## = -27560 because I made a mistake in the original post; V3 should be 6 instead of 2.
 
  • #4
What happened to the units in your calculations?
 
  • #5
SteamKing said:
What happened to the units in your calculations?
I added the units to the original problem. There was no unit conversion involved, so I didn't want to clutter my work.
 
  • #6
Your calculation of U3 is a bit low. I get 58500 J.

You can use ΔU = 3nRΔT/2

ΔU from 2-3 is (3)(5)(8.32)(112.5)/(2) = 7020.

AM
 
  • #7
Andrew Mason said:
Your calculation of U3 is a bit low. I get 58500 J.

You can use ΔU = 3nRΔT/2

ΔU from 2-3 is (3)(5)(8.32)(112.5)/(2) = 7020.

AM

Ah, that's it. Thank you so much.
 

What is the definition of a heat engine cycle?

A heat engine cycle is a series of thermodynamic processes that take place in a closed system in order to convert heat energy into mechanical work. This cycle typically involves the transfer of energy between a heat source and a heat sink, with the end goal being to produce useful work.

What are the four main processes involved in a heat engine cycle?

The four main processes involved in a heat engine cycle are: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression. These processes follow the laws of thermodynamics and work together to convert heat energy into mechanical work.

What is the difference between a Carnot cycle and a Rankine cycle?

A Carnot cycle is a theoretical heat engine cycle that is considered to be the most efficient possible. It consists of two isothermal processes and two adiabatic processes. A Rankine cycle, on the other hand, is a practical heat engine cycle commonly used in power plants. It involves a mixture of isobaric and isentropic processes and is less efficient than a Carnot cycle.

How does a heat engine cycle relate to the second law of thermodynamics?

The second law of thermodynamics states that the total entropy of a closed system will always increase over time. In a heat engine cycle, the conversion of heat energy into mechanical work results in an increase in entropy, as some of the energy is lost to the surroundings as heat. This demonstrates the irreversible nature of thermodynamic processes.

What are some real-world examples of heat engine cycles?

Some common examples of heat engine cycles include car engines, jet engines, and steam turbines in power plants. These all involve the conversion of heat energy into mechanical work to power various forms of transportation or generate electricity.

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