Temprature-Entropy cyclic process

Click For Summary
SUMMARY

The discussion centers on calculating heat input and efficiency for a temperature-entropy (T-S) cyclic process. The efficiency η is expressed as η=(Q1/Q2)-1=(T1/T2)-1. The heat extracted during the linear process II-III is calculated as Q_{II-III} = -\frac{1}{2\alpha} (T_1^2 - T_2^2), indicating heat extraction. Additionally, the process III-I is identified as adiabatic with Q_{III-I}=0, while the isothermal process I-II requires further analysis of entropy change.

PREREQUISITES
  • Understanding of thermodynamic cycles
  • Familiarity with temperature-entropy (T-S) diagrams
  • Knowledge of heat transfer equations
  • Basic calculus for integration and differentiation
NEXT STEPS
  • Study the derivation of heat transfer in isothermal processes
  • Explore the implications of adiabatic processes in thermodynamics
  • Learn about the Carnot cycle and its efficiency calculations
  • Investigate the relationship between entropy and heat in cyclic processes
USEFUL FOR

Students and professionals in thermodynamics, mechanical engineers, and anyone involved in energy systems analysis will benefit from this discussion.

astrozilla
Messages
28
Reaction score
0

Homework Statement


There is a temperature-Entropy graph (T-S) (attachment),which illustrates a hypothetical cyclic process.
a) Calculate the heat input or output along each of the paths.

b) Find an expression for the efficiency η of the complete cycle in terms of T1 and T2 only.

Homework Equations



for b ,η=(Q1/Q2)-1=(T1/T2 )-1,HEAT INPUT: DH=DQ (ONLY in case of isobaric change)

The Attempt at a Solution

 

Attachments

  • temperature-entropy gragh.jpg
    temperature-entropy gragh.jpg
    5 KB · Views: 442
Physics news on Phys.org
[PLAIN]http://img202.imageshack.us/img202/3227/temperatureentropygragh.jpg
I suppose the most complicated path is the linear process II-III (see attached image) in which both T and S change:
[tex]T(S)= \alpha S + T_0[/tex]
where [tex]\alpha, T_0 >0[/tex] are some constants.
So, in this process we have
[tex]\frac{dS}{dT} = \frac{1}{\alpha}[/tex]
and hence
[tex]\delta Q_{II-III} = TdS = \frac{1}{\alpha} T dT[/tex]

When T changes from [tex]T_1[/tex] to [tex]T_2[/tex] you have
[tex]Q_{II-III} = \frac{1}{\alpha}\int_{T_1}^{T_2} TdT = -\frac{1}{2\alpha} \left(T_1^2 - T_2^2 \right)[/tex]
That is, the heat is extracted in this process.
Now for the process III-I where the entropy is constant it is trivial that [tex]Q_{III-I}=0[/tex]. It is in fact an adiabatic process.

Try to find the heat for isothermal process I-II. Note that the change of the entropy
[tex]S_{II} - S_{I}[/tex]
you can express in terms of [tex]T_2[/tex], [tex]T_1[/tex] and [tex]\alpha[/tex] just from the following equations for III and II points on the graph:
[tex]T_2 = \alpha S_{I} +T_0[/tex]

[tex]T_1 = \alpha S_{II} + T_0[/tex]
Note also that [tex]S_{I}=S_{III}[/tex]
 
Last edited by a moderator:
That's amazing.Thank you very much for both answers !
 

Similar threads

  • · Replies 14 ·
Replies
14
Views
9K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
1K
Replies
3
Views
4K
  • · Replies 8 ·
Replies
8
Views
4K
  • · Replies 12 ·
Replies
12
Views
6K
Replies
5
Views
5K
  • · Replies 3 ·
Replies
3
Views
12K
  • · Replies 2 ·
Replies
2
Views
2K