Efficiency of a combustion motor

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SUMMARY

The efficiency of a combustion motor can be expressed using the formula E = (Q2 - Q1) / Q2, where Q2 represents the heat from the explosion and Q1 is the heat lost through the exhaust. This efficiency can also be derived from the volume ratio V1/V2, leading to the equation E = 1 - (1 / (V1/V2)^(γ-1)). The discussion highlights the relationship between temperature, volume, and heat transfer, emphasizing that maximum efficiency is achieved only under reversible processes where entropy is conserved. The connection between temperature changes and heat transfer is crucial for understanding these concepts.

PREREQUISITES
  • Understanding of thermodynamics principles, specifically the second law of thermodynamics.
  • Familiarity with adiabatic processes and the concept of entropy.
  • Knowledge of the Carnot efficiency and its relation to temperature.
  • Basic grasp of heat transfer equations, including Q = mCPΔT and Q = mCVΔT.
NEXT STEPS
  • Research the Carnot efficiency and its implications for thermal machines.
  • Study adiabatic expansion and its mathematical derivations in thermodynamics.
  • Explore the relationship between temperature, volume, and heat transfer in combustion engines.
  • Learn about reversible processes and their significance in maximizing efficiency.
USEFUL FOR

Students of thermodynamics, mechanical engineers, and anyone interested in the efficiency of combustion engines and heat machines.

Karol
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Homework Statement


The efficiency of a heat machine is ##E=\frac{Q_2-Q_1}{Q_2}## where Q2 is the heat inserted because of the explosion and Q1 is the heat that leaves through the exhaust.
It says in the book that E can be derived from the volumes ratio V1/V2:
$$E=1-\frac{1}{\left(V_1/V_2 \right)^{\gamma-1}}$$ why?

Homework Equations


Adiabatic expansion: ##T_1V_1^{\gamma-1}=T_2V_2^{\gamma-1}##

The Attempt at a Solution


$$E=1-\frac{1}{\left(V_1/V_2 \right)^{\gamma-1}}=\frac{T_2-T_1}{T_2}$$
But V2 and T2 have nothing to do with Q2, the heat from the explosion. also i don't know what's the connection between V1 or T1 and the heat lost through the exhaust.
I have just started studying the second law, maybe the book is excluding some explanations, it's an old book for high school but the level is quite high
 
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Not my field but perhaps look up Carnot Efficiency. That relates efficiency and temperature.
 
Note that E is the maximum efficiency, achievable only if all process steps are carried out reversibly, i.e. entropy is conserved. Then Q2 = T2dS2 and idem 1 (with a - sign). Over all ##\Delta S = Q_2/T_2 - Q_1/T_1## and only ##Q_2 - Q_1## can be drawn off as work.
 
BvU said:
Note that E is the maximum efficiency, achievable only if all process steps are carried out reversibly, i.e. entropy is conserved.
You're right. But mostly actual cycles aren't considered till you study the subject in depth. And I think there is an easier way for this proof.

Karol said:
But V2 and T2 have nothing to do with Q2, the heat from the explosion. also i don't know what's the connection between V1 or T1 and the heat lost through the exhaust.
If you know the the changes in temperatures (ΔT), you can use the equations-
Q = mCPΔT (constant pressure) or Q = mCVΔT (constant volume)
Knowing the relation between temperature and volume, you can introduce 'V' into the equation.

I must say though, it isn't really too easy for a starter.
 
Thanks i solved but it's long development so i won't write it here
 
No problemo!
 

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