How Efficient Can a Heat Engine Be Between 1200 K and 300 K?

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In summary, a heat engine operating between temperatures of 1200 K and 300 K is used to lift a 30 kg mass at a constant velocity of 4 m/s. The power that the heat engine must supply to lift the mass is 1176 J/s and the maximum possible efficiency is 75%. The rate at which the hot reservoir supplies heat to the engine is 1568 W, and the rate at which heat is exhausted to the cold reservoir is 392 W. This can be found by using the equation for efficiency, work output, and the first law of thermodynamics.
  • #1
science.girl
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Homework Statement



A heat engine is built to operate between temperatures of 1200 K and 300 K. It is used to lift a 30 kg mass at a constant velocity of 4 m/s.

a) Determine the power that the heat engine must supply to lift the mass.

b) Determine the maximum possible efficiency of the heat engine.

c) If the engine were to operate at the maximum possible efficiency, determine the following:
i. The rate at which the hot reservoir supplies heat to the engine.
ii. The rate at which heat is exhausted to the cold reservoir.


Homework Equations



P = W/t
e = 1 - T1/T2


The Attempt at a Solution



I figured out that (b) is 1 - (300/1200) = 75%.

For (a), there is no distance stated to figure out work (W = Fd), and there is no time to determine power (P = W/t). What am I missing?
 
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  • #2
Power= rate of doing work. = Fd/t = fv.
 
  • #3
rl.bhat said:
Power= rate of doing work. = Fd/t = fv.

Oh! So, P = Fv = (30 kg)(9.8 m/s^2)(4 m/s) = 1176 J/s.

So, if the power supplied to lift the mass is 1176 J/s, and the maximum possible efficiency is 75%, then the rate heat is removed from the hot reservoir... Wouldn't that depend on the first law of thermodynamics?
[delta]U = Q + W

But how would you apply the equation exactly, and what would it signify?
 
  • #4
science.girl said:
Oh! So, P = Fv = (30 kg)(9.8 m/s^2)(4 m/s) = 1176 J/s.

So, if the power supplied to lift the mass is 1176 J/s, and the maximum possible efficiency is 75%, then the rate heat is removed from the hot reservoir... Wouldn't that depend on the first law of thermodynamics?
[delta]U = Q + W

But how would you apply the equation exactly, and what would it signify?
You do not need to apply the first law here. You just have to apply the efficiency. The work output is 1176 watts (J/s) at 75% efficiency (efficiency = work out/energy in) so the energy (heat flow) input must be...?

AM
 
  • #5
Andrew Mason said:
You do not need to apply the first law here. You just have to apply the efficiency. The work output is 1176 watts (J/s) at 75% efficiency (efficiency = work out/energy in) so the energy (heat flow) input must be...?

AM

So, given the equation e = W/QH...

.75 = (1176W)/QH

QH = 1568 WAnd, for the rate at which heat is exhausted to the cold reservoir, does this also depend on an efficiency equation?
 
Last edited:
  • #6
75% = 75/100 = 0.75

for rate at which heat is exhausted note that W = QH-QC. So dW/dt = dQH/dt - dQC/dt
 
  • #7
djeitnstine said:
75% = 75/100 = 0.75

for rate at which heat is exhausted note that W = QH-QC. So dW/dt = dQH/dt - dQC/dt

Hmm... Unfortunately, this is a non-calc based course, so would you know of another approach?
 
  • #8
dW/dt = Power

dQh/dt = rate of energy output from the hot resevior

or perhaps delta Qh/ delta t which is average energy over a period of time

similar argument for Qc
 
  • #9
djeitnstine said:
dW/dt = Power

dQh/dt = rate of energy output from the hot resevior

or perhaps delta Qh/ delta t which is average energy over a period of time

similar argument for Qc

Yes, but unfortunately, this is an algebra-based course. Is there another method for finding the rate at which heat is exhausted to the cold reservoir?
 
  • #10
science.girl said:
Yes, but unfortunately, this is an algebra-based course. Is there another method for finding the rate at which heat is exhausted to the cold reservoir?
W = Qh-Qc

P = W/t = Qh/t - Qc/t

You know two of those terms. So find Qc/t

AM
 
  • #11
Andrew Mason said:
W = Qh-Qc

P = W/t = Qh/t - Qc/t

You know two of those terms. So find Qc/t

AM

W = QH - QC

392 W = 980 W - QC/t

QC/t = 588 W

Correct?
 
  • #12
science.girl said:
W = QH - QC

392 W = 980 W - QC/t

QC/t = 588 W

Correct?
I am not sure what you are doing here.

W/t = 1176 w
Qh/t = W/e = 1568 w

AM
 
  • #13
Andrew Mason said:
I am not sure what you are doing here.

W/t = 1176 w
Qh/t = W/e = 1568 w

AM

My apologies. I was working on two similar problems... that's why the values were different.

Thank you very much for your help! I appreciate it.

-Science.girl
 

What is a heat engine?

A heat engine is a device that converts heat energy into mechanical work. It follows the principles of thermodynamics and typically involves the transfer of heat from a hot source to a colder sink, resulting in the production of work.

What are the laws of thermodynamics?

The laws of thermodynamics are fundamental principles that govern the behavior of energy in a system. There are four laws, but the first and second laws are the most commonly referenced. The first law states that energy cannot be created or destroyed, only converted from one form to another. The second law states that the total entropy of a closed system will never decrease over time.

What is the Carnot cycle?

The Carnot cycle is a theoretical thermodynamic cycle that is used as a model for the most efficient heat engine possible. It consists of four stages: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression. The Carnot cycle is important because it sets the upper limit for the efficiency of any heat engine.

What is the difference between a heat engine and a heat pump?

A heat engine converts heat energy into mechanical work, while a heat pump moves heat from a colder source to a hotter one. Heat engines typically have a lower efficiency than heat pumps because they produce work, while heat pumps require energy to operate.

How does the efficiency of a heat engine change with temperature?

The efficiency of a heat engine is directly related to the temperature difference between the hot source and the cold sink. As the temperature difference increases, so does the efficiency of the heat engine. However, the efficiency will never reach 100% due to the limitations of the second law of thermodynamics.

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