Finding work, heat, and entropy in a heat engine

In summary: I think the issue was the significant digits in T, as you mentioned. I was not using enough significant digits in my calculations. Thank you for your help! In summary, the engine operates with 1.94 moles of a monatomic ideal gas, starting at a volume of 21.4 L and pressure of 2.77 atm. The cycle consists of an isobaric expansion until the volume reaches 50.1 L, followed by an isochoric process that lowers the pressure to 1.184 atm, and finally an isothermal process that returns the gas to its original pressure and volume. The absolute temperature of the isothermal process is 372 K, the work done on the gas is 5214.
  • #1
rubenhero
42
2

Homework Statement


An engine operates with n = 1.94 moles of a monatomic ideal gas as its working substance, starting at volume VA = 21.4 L and pressure PA = 2.77 atm. The cycle consists of:

- A to B: an isobaric expansion until its volume is VB = 50.1 L
- B to C: an isochoric (constant volume) process that lowers the pressure to PC = 1.184 atm
- C to A: an isothermal (constant temperature) process that returns the gas to its original pressure and volume

HINT: Draw a P-V diagram of this process.

a) Find TT, the absolute temperature of the isothermal process.
b) Find WT, the work done on the gas during the isothermal process.
c) Find ΔST, the change in entropy of the gas during the isothermal process.
d) Find Wtot, the work done in the entire cycle.
e) Find Qtot, the heat that is exchanged (in or out) during the entire cycle.


Homework Equations


PV=nRT, Wdone on a gas = nRTln(Vo/Vf),
ΔS = Qrev/T, Qp = CpT, Cp = 5/2nR,
Qv = CvΔT, Cv = 3/2nR


The Attempt at a Solution


necessary conversions:
1 atm = 1.013e5 Pa
2.77 atm = 280601 Pa
1.184 atm = 119939.2 Pa

1L = 1/1000 m^3
21.4 L = .0214 m^3
50.1 L = .051 m^3

2 a) Find TT, the absolute temperature of the isothermal process.
PV = nRT
PV/nR = T
(280601Pa * .0214m^3)/ (1.94 moles * 8.314 J/mol-K) = T
372.2984582K = T
372 K = T [webassign marked as correct] 3 significant digits

b) Find WT, the work done on the gas during the isothermal process.

Won the gas = nRT ln(Vo/Vf)
= 1.94 moles * 8.314 J/mol-K * 372 K ln(.051m^3/.0214m^3)
= 5214.830072 J
Won the gas = 5.21e3 J [webassign marked as correct] 3 significant digits

c) Find ΔST, the change in entropy of the gas during the isothermal process.
change in IE is 0 since it is an isothermal process, work is positive because the gas was compressed and work was done on the gas
change IE = Q + W
0 = Q + 5214.830072 J
-5214.830072 J = Q
dS = dQrev/T
= -5214.830072 J/ 372.2984582 K
= -14.0071224 J/K
dS = -14.0 J/K [webassign marked as wrong] 3 significant digits

d) Find Wtot, the work done in the entire cycle.
plan : find work done in all parts of the cycle and get sum

A-B is an isobaric process so W = -PdV
= -280601 Pa * (.051m^3 - .0214m^3)
= -8365.7896 J
B-C is an isochoric process so W = 0
C-A is an isothermal process (taken from part 2b) W = 5214.830072 J

Wtot = WA-B + WB-C + WC-A = -8365.7896 J + 0J + 5214.830072 J
Wtot = -3090.959528 J
Wtot = -3.09e3 J [ webassign marked as wrong] 3 significant digits

e) Find Qtot, the heat that is exchanged (in or out) during the entire cycle.

plan : find heat in all parts of the cycle and get sum

A-B is an isobaric process so Q = CpdT
= 5/2 n R dT

we need the different temperature at points A and B to get dT:
@ A : PV/nR = T
= (280601Pa * .0214m^3)/ (1.94 moles * 8.314 J/mol-K) = T
= 372 K
@B : PV/nR = T
= (280601Pa * .051m^3)/ (1.94 moles * 8.314 J/mol-K) = T
= 887.253335 K
dT = TB - TA = 887.253335 K - 372.2984582 K = 515 K

so now QA-B = 5/2 n R dT
= 5/2 * 1.94 moles * 8.314 J/mol-K * 515 K
= 20764.474 J positive because heat was added to the system

B-C is an isochoric process so Qv = CvdT
= 3/2 n R dT
we need the different temperature at points B and C to get dT:
@B : PV/nR = T
= (280601Pa * .051m^3)/ (1.94 moles * 8.314 J/mol-K) = T
= 887.253335 K
@C : PV/nR = T
= (119939.2Pa * .051m^3) / (1.94 moles * 8.314 J/mol-K) = T
= 379.2447468 K
dT = TB - Tc = 887.253335 K - 379.2447468 K
= 508.0085882 K
= 508 K
so Q = 3/2 n R dT
= 3/2 1.94 moles * 8.314 J/mol-K * 508 K
= -12290.6277 J negative because heat was removed
C-A is an isothermal process and we already figured out Q is -5214.830072 J from part 2b

so finally Qtot = QA-B + QB-C + QC-A

= 20764.474 J + -12290.6277 J + -5214.830072 J
= 3259.016228 J
= 3.25e3 J [webassign marked as wrong] 3 significant figures

thank you in advance for any input as to why my work might be wrong.
 
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  • #2
rubenhero said:

The Attempt at a Solution


necessary conversions:


1L = 1/1000 m^3
21.4 L = .0214 m^3
50.1 L = .051 m^3

VB=0.0501 m^3.
Recalculate the isotherm work with the correct volume. Also try to use more significant digits in T.

ehild
 
  • #3
Thank you ehild, I redid all the work and got the correct answers.
 

1. What is a heat engine?

A heat engine is a device that converts heat energy into mechanical work. It operates by taking in heat from a high temperature source, using that energy to perform work, and then releasing the remaining heat to a low temperature sink.

2. How does a heat engine work?

A heat engine works by taking in heat from a high temperature source and using that energy to expand a gas or liquid, which then drives a piston or turbine to perform work. The remaining heat is released to a low temperature sink, completing the cycle.

3. What is the relationship between work, heat, and entropy in a heat engine?

In a heat engine, work is performed by converting heat energy into mechanical energy. This process also results in an increase in entropy, which is a measure of the disorder or randomness in a system. The greater the amount of work performed, the greater the increase in entropy.

4. How is the efficiency of a heat engine calculated?

The efficiency of a heat engine is calculated by dividing the amount of work done by the input heat energy. In other words, it is the ratio of the output work to the input heat.

5. What are some practical applications of heat engines?

Heat engines are used in a variety of practical applications, such as power plants, car engines, and refrigerators. They are also used in industrial processes, such as in manufacturing and chemical reactions.

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