How Much Energy Does a Carnot Cycle Heat Engine Expel Per Cycle?

AI Thread Summary
The discussion centers on a Carnot cycle heat engine operating between temperatures of 354.05K and 711.15K, absorbing 22415J from the hot reservoir. The mechanical power output was calculated at 11.49kW, derived from the work done (W) being the difference between heat absorbed (Qh) and heat expelled (Qc). The correct method to find Qc is confirmed as Qc = Qh - W, resulting in 11159.43J or 11.16kJ, which matches the calculated Qc. The relationship between Qc and Qh is also explained through the Carnot efficiency formula, emphasizing the constant temperature heat flow and zero entropy change.
S_fabris
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Hey i have a heat engine that operates in a Carnot cycle between 354.05K and 711.15K, it absorbs 22415J of energy per cycle from hot resevoir. The duration of each cycle is 0.98s.
First question was to find the mechanical power output...i calculated this and got W = Qh - Qc = 22415 - 11159.43 = 11255.57 J/0.98s = 11,49kW

the next question asks how much energy does it expel in each cycle by heat in units of kJ..

everywhere I look it says to use Qc = Qh - W which gives me 11 159.43J is this right?? 11.16kJ?

this seems odd as an answer because it is the same answer as Qc.

Can anybody confirm this or steer me in right direction? thank you
 
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S_fabris said:
Hey i have a heat engine that operates in a Carnot cycle between 354.05K and 711.15K, it absorbs 22415J of energy per cycle from hot resevoir. The duration of each cycle is 0.98s.
First question was to find the mechanical power output...i calculated this and got W = Qh - Qc = 22415 - 11159.43 = 11255.57 J/0.98s = 11,49kW

the next question asks how much energy does it expel in each cycle by heat in units of kJ..

everywhere I look it says to use Qc = Qh - W which gives me 11 159.43J is this right?? 11.16kJ?

this seems odd as an answer because it is the same answer as Qc.

Can anybody confirm this or steer me in right direction? thank you
! Qc IS the heat energy expelled in each cycle (ie the heat flowing to the cold reservoir.

For the Carnot cycle heat flows into and out of the reservoirs at constant temperature and there is 0 change in entropy. ie \Delta S = Q_h/T_h - Q_c/T_c = 0, so Q_c/Q_h = T_c/T_h[/tex]<br /> <br /> From the first law: W = Qh - Qc, so<br /> <br /> \eta = \frac{W}{Q_h} = \frac{Q_h - Q_c}{Q_h} = 1 - \frac{Q_c}{Q_h} = 1 - \frac{T_c}{T_h}<br /> <br /> Q_c = Q_h\frac{T_c}{T_h}<br /> <br /> AM
 
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