Heat engines and finding efficiency

AI Thread Summary
Engine A receives four times more input heat than engine B, produces six times more work, and rejects three times more heat. The efficiency of both engines can be expressed using the equations e = |W|/|QH| and e = 1 - |Qc|/|QH|. By setting up relationships between the efficiencies of the two engines, it was determined that the efficiency of engine A is 1/2 and that of engine B is 1/3. The discussion highlighted the importance of understanding the cyclic nature of thermal engines and the relevance of the First Law of Thermodynamics in deriving these efficiencies. Overall, the problem was simplified through the application of these principles and relationships.
BOAS
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Hello,

Homework Statement



Engine A receives four times more input heat, produces six times more work, and
rejects three times more heat than engine B. Find the efficiency of (a) engine A and
(b) engine B.

Homework Equations



e = |W|/|QH|

e = 1 - |Qc|/|QH|

The Attempt at a Solution



I can't really see how I'm supposed to find any numerical answer to this question. It seems overly simple just to state the efficiency of A in terms of B and vice versa.

What relationship am I not seeing that will help me solve this problem?

Thanks for any help you can give.
 
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Express the efficiency of A in terms of B via the two different equations for efficiency. That will give you two equations for two unknowns.
 
BOAS said:
Hello,

Homework Statement



Engine A receives four times more input heat, produces six times more work, and
rejects three times more heat than engine B. Find the efficiency of (a) engine A and
(b) engine B.

Homework Equations



e = |W|/|QH|

e = 1 - |Qc|/|QH|

The Attempt at a Solution



I can't really see how I'm supposed to find any numerical answer to this question. It seems overly simple just to state the efficiency of A in terms of B and vice versa.

What relationship am I not seeing that will help me solve this problem?

Thanks for any help you can give.

What is the change of internal energy during the whole circle? Write up the First Law with QH, QC and W for both systems and use the relations given between the input heat, rejected heat and work.

ehild
 
voko said:
Express the efficiency of A in terms of B via the two different equations for efficiency. That will give you two equations for two unknowns.

Thanks for the response,

e_{a} = \frac{6|W_{b}|}{4|Q_{Hb}|} = 1 - \frac{3|Q_{Cb}|}{4|Q_{Hb}|}

\frac{6|W_{b}|}{4|Q_{Hb}|} = 1 - \frac{3|Q_{Cb}|}{4|Q_{Hb}|}

\frac{6|W_{b}|}{4|Q_{Hb}|} + \frac{3|Q_{Cb}|}{4|Q_{Hb}|} = 1

\frac{6|W_{b}| + 3|Q_{Cb}|}{4|Q_{Hb}|} = 1

6|W_{b}| + 3|Q_{Cb}| = 4|Q_{Hb}|

6|W_{b}| = 4|Q_{Hb}| - 3|Q_{Cb}|

The above is the same as a cons. energy statement, but I'm not sure if I'm getting any closer to an actual answer.
 
Last edited:
You do not want to deal with the heats and work. You want to relate ##e_A## and ##e_B## in two different ways.
 
e_{a} = \frac{6|W_{b}|}{4|Q_{Hb}|}

e_{a} = 1 - \frac{3|Q_{Cb}|}{4|Q_{Hb}|}

e_{b} = \frac{4|Q_{Ha}|}{6|W_{a}|}

e_{b} = 1 - \frac{4|Q_{Ha}|}{3|Q_{Ca}|}

I don't understand what to do with this info.
 
Since ## e_B = \dfrac {|W_B|} {|Q_{HB}|} ## by definition, you have ##e_A = \dfrac 6 4 e_B##.
 
voko said:
Since ## e_B = \dfrac {|W_B|} {|Q_{HB}|} ## by definition, you have ##e_A = \dfrac 6 4 e_B##.

So I was unnecessarily confusing matters by talking about b in fractions of a(which was in turn multiples of b...)?

This has turned out a lot simpler than I was making it, but I am concerned that there are 5 marks available here.
 
Have you been able to form another equation for ##e_A## and ##e_B##? Have you solved the system?
 
  • #10
e_{a} = 1 - \frac{3|Q_{Cb}|}{4|Q_{Hb}|}

e_{b} = 1 - \frac{|Q_{Cb}|}{|Q_{Hb}|}

e_{a} = \frac{3}{4}e_{b} + \frac{1}{4}

I have a feeling that my equation for the efficiency of a is wrong...

Then doing simultaneous equations I obtain that ea = 1/2

so eb = 1/3
 
  • #11
All correct.
 
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  • #12
Thank you Voko,

for being so patient and leading me through it.

BOAS.
 
  • #13
A bit different approach: During a cyclic process, the change of internal energy is zero: Qh(A)-Qc(A)-W(A)=0, Qh(B)-Qc(B)-W(B)=0. With the given relation between engines A and B: 4Qh(B)-3Qc(B)-6W(B)=0. Eliminate Qc(B): Qh(B)-3W(B)=0. The efficiency is defined as η=W/Qh, so it is 1/3 for engine B. You know already the ratio of the efficiencies...

ehild
 
  • #14
ehild said:
A bit different approach: During a cyclic process, the change of internal energy is zero: Qh(A)-Qc(A)-W(A)=0, Qh(B)-Qc(B)-W(B)=0. With the given relation between engines A and B: 4Qh(B)-3Qc(B)-6W(B)=0. Eliminate Qc(B): Qh(B)-3W(B)=0. The efficiency is defined as η=W/Qh, so it is 1/3 for engine B. You know already the ratio of the efficiencies...

ehild

Hi,

I don't know what you mean by cyclic process, or how I can know my question describes one. It is always a good idea to know different ways of solving a problem, so I would be interested in understanding your method.

BOAS.
 
  • #15
BOAS said:
Hi,

I don't know what you mean by cyclic process, or how I can know my question describes one. It is always a good idea to know different ways of solving a problem, so I would be interested in understanding your method.

BOAS.

How does a thermal engine work? Is it not repeating itself, and going back to its initial state after performing the process?

How do you define QH, QC and W? They are not meaningless letters. Your two equations of efficiency were derived from the condition that the net change of the internal energy during the process is zero.

Eliminate e from the two equations for efficiency

e = |W|/|QH|, e = 1 - |Qc|/|QH| ,

You get that QH-QC-W=0. *

The definition of efficiency refers to a process where heat is taken in one stage, heat is rejected in other stage, (the net heat transferred to the system is Q= QH-QC) work W is done.

The change of the internal energy in a process is ΔU=Q-W, according to the First Law of Thermodynamics. Eguation * means that the internal energy does not change.

ehild
 
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