Carnot Cycle: Analysis of Energy Exchange

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SUMMARY

The discussion focuses on the Carnot cycle as it applies to refrigerators and heat engines. A refrigerator absorbs 120 J of energy at temperature Tc and does 300 J of work, resulting in 420 J of energy exhausted as heat. The principles of cyclic processes are emphasized, particularly that the work done equals the heat expelled plus any heat added. Additionally, a heat engine operating on a Carnot cycle absorbs 420 J from a hot reservoir and does 300 J of work, necessitating the expulsion of 120 J as heat.

PREREQUISITES
  • Understanding of the Carnot cycle principles
  • Familiarity with thermodynamic concepts such as work, heat, and internal energy
  • Basic knowledge of heat engines and refrigerators
  • Ability to interpret thermodynamic diagrams
NEXT STEPS
  • Study the first and second laws of thermodynamics
  • Learn about the efficiency of Carnot engines and refrigerators
  • Explore real-world applications of the Carnot cycle in engineering
  • Investigate the implications of temperature differences in energy exchange
USEFUL FOR

Students of thermodynamics, mechanical engineers, and anyone interested in the principles of energy exchange in heat engines and refrigerators.

physics123
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A refrigerator operates on a Carnot cycle. In this cycles, it absorbs 120 J of energy at a temperature Tc while 300 J of work is done on the gas undergoing the cycle.

How much energy is exhausted as heat during this process?

The answer is 420 J.

I am unsure of where to start for this question as we are not given temperatures.
 
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Recall that, in any cyclic process, the gas must return to its original state. So, in one cycle,

$$\Delta U=Q-W=0$$

Therefore, work done (300 J) must equal heat expelled. And any heat added (120 J) must also be expelled.
 
zenmaster99 said:
Recall that, in any cyclic process, the gas must return to its original state. So, in one cycle,

$$\Delta U=Q-W=0$$

Therefore, work done (300 J) must equal heat expelled. And any heat added (120 J) must also be expelled.

so to find energy exhausted as heat, it is as simple as adding the work plus any heat added?
 
physics123 said:
so to find energy exhausted as heat, it is as simple as adding the work plus any heat added?

Could you then explain this question?
A heat engine operates on a Carnot cycle. In this cycles, it absorbs 420J of energy while it expands in contact with a reservoir of temperature Th. The heat engine does a net 300J during the full cycle.

The answer is 120J, so why isn't the energy added? What is the difference between absorbing energy at Th and Tc?
 
In this case, the engine takes in 420 J from the hot reservoir. This must be expelled as either heat or work. 300 J is returned as work, therefore 120 J must be heat.

Hang on, let me look for the diagram I'm thinking of...

Here it is: https://en.wikipedia.org/wiki/Heat_engine#/media/File:Heat_engine.png

Notice that what goes in must come out as either work or heat. Although this diagram tries to be all-encompassing by including a little loss mechanism, you needn't worry about that at this level.
 
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