Max efficiency (thermodynamics)

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The discussion centers on the efficiency of a heat engine and the role of heat extraction between points 3 and 4 on the p-v diagram. The efficiency formula, η = 1 - (Qc/Qh), highlights the losses incurred when heat is not adequately managed. Achieving 100% efficiency is theoretically possible if cooling is eliminated, assuming no friction. The conversation also explores the challenges of implementing isobaric processes in practical applications, questioning how to compress the working fluid without altering pressure or temperature. The complexities of real-world applications of isobaric processes remain a point of inquiry.
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I'm observing the circular process of a heat engine. It's p-v diagram is

heaengcyc.gif


So between points 3 and 4 the heat is extracted. That causes losses since the efficiency if given by
\eta =1- \frac {Q_c} {Q_h}

Where Qh is the heat the heat source has given and Q_c the amount of heat that the "cold" container took.
If we don't cool down the engine in during the process between 3 and 4, the efficiency would grow to 100% (if friction is not consigered).
The process would then look like the picture below, and 3 and 1 we would do an isobaric contraction.

attachment.php?attachmentid=24297&stc=1&d=1268325038.gif


I've encountered isobaric processes through my studies, but only as a theoretical concept. What are the reasons why it couldn't be used here?
 

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How can you do compress the working fluid without changing its pressure or temperature?
 
I don't know, how do you get an isobaric process ever? :)
 
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