AZINGLY, for the Joule cycle there is no heat flow at all, so it is 1-0 = 1.

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    Diesel Joule Otto
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The discussion focuses on calculating the efficiency of Diesel, Otto, and Joule cycles, emphasizing that for the Joule cycle, there is no heat flow, resulting in an efficiency of 1. The efficiency equations for Diesel and Otto cycles are derived from their respective heat flow processes, with Diesel utilizing adiabatic compression and expansion, while Otto relies on constant volume heat flow. The key equations presented are Efficiency = W/Qh for the cycles, with specific formulas for Diesel and Otto cycles based on temperature changes.

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  • Understanding of thermodynamic cycles: Diesel, Otto, and Joule processes
  • Familiarity with the concepts of heat flow and efficiency in thermodynamics
  • Knowledge of adiabatic processes and their implications in cycle efficiency
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Abigale
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Diesel, Otto , Joule TRICK?

Hi Guys,
I try to callculate the efficiency for a cycle Process.
For Diesel, Otto and Joule Processes you can write the efficiency as a really small equation.

I have seen that for example sometimes the adiabatic equation is used,
but i don't understand in which case, or better, how I have to connect the procceses?

Is there a trick or do I have to learn it by memorization?

THX
 
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Abigale said:
Hi Guys,
I try to callculate the efficiency for a cycle Process.
For Diesel, Otto and Joule Processes you can write the efficiency as a really small equation.

I have seen that for example sometimes the adiabatic equation is used,
but i don't understand in which case, or better, how I have to connect the procceses?

Is there a trick or do I have to learn it by memorization?

THX
Efficiency = W/Qh and, since there is no change in U in a complete cycle, W = net heat flow = Qh+Qc = |Qh|-|Qc|.

So all you have to worry about is the heat flow.

Since both the Diesel and Otto cycles involve adiabatic compression and expansion, heat flow only occurs in two of the four parts:

For Diesel the constant pressure expansion part (1 - heat flow in) and constant volume part (3 - heat flow out). So it is just: (Cp|ΔT1|-Cv|ΔT3|)/Cp|ΔT1| = 1 -(1/γ)|ΔT3|/|ΔT1|

For Otto heat flow is in the two constant volume parts, so efficency is (|ΔT1|-|ΔT3|)/|ΔT1| = 1 - |ΔT3|/|ΔT1|

AM
 

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