Reversible Carnot Cycle and Heat Engine

In summary, the powerplant will be able to produce a maximum of 17 watts at a rate of 120 kilowatts per second, but will be most efficient at a temperature of 147 degrees Celsius.
  • #1
mm391
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Homework Statement



A borehole produces 120kg/s of high pressure water at 165°C. A powerplant is to be designed to extract heat from the water, reducing the temp to 147°C. The plant which will initially be assumed to be reversible, will reject heat at 17°C to a river. Take 147°C as the highest temp available and assume the river is so large that there is negligible change in temp. Specific Heat Capacity of high pressure water is 4.2kj/kgK.

Work out:
a) Rate of heat input available to the plant.
b) Rate at which heat is rejected
c) Maximum power out from the plant and its efficiency.

Homework Equations



QL/QH = TL/TH

The Attempt at a Solution



I am not sure where or how to begin. Any help pointing me in the right direction for each question would be much appreciated.
 
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  • #2
I am not sure your question makes sense. What do you mean by "to reject heat?" Are you sure that 17 C is not the temperature of the river? If the process reduces the temperature from 165 C to 147 C, then isn't 165 the highest temperature, and not 147? I would not know where to start either. It does not make sense.
 
  • #3
For part a): Use this equation to calculate the heat lost from the water (the heat input to the plant): Q(rate) = m(rate of mass flow) * specific heat * temperature change

for b): Since the plant is assumed to be reversible, use the equation: Qh(rate)/QL(rate) = Th/TL

for c): The maximum power output results from a reversible cycle (or a process), which is the case here. Now since the efficiency of a reversible cycle is a function of temperature ONLY, use the equation: η(rev) = (Th-TL)/(Th)
After you find the maximum efficiency, use the equation: η = [Wnet,output(rate)]/Qh

I hope that answers your question.
 

1. What is a Reversible Carnot Cycle?

A Reversible Carnot Cycle is a thermodynamic process that describes an ideal heat engine. It consists of four steps: isothermal expansion, adiabatic expansion, isothermal compression, and adiabatic compression. This cycle is reversible, meaning that it can be run in either direction without any energy loss.

2. How does a Reversible Carnot Cycle work?

In a Reversible Carnot Cycle, a working fluid is used to absorb heat at a constant temperature, expand and do work, and then release heat at a lower temperature. This process repeats until the initial state is reached. The cycle relies on the principle that heat flows from hot to cold, and the direction of heat flow can be reversed by changing the temperature difference.

3. What is the efficiency of a Reversible Carnot Cycle?

The efficiency of a Reversible Carnot Cycle is given by the Carnot efficiency formula, which is equal to the temperature difference between the hot and cold reservoirs, divided by the temperature of the hot reservoir. The maximum efficiency that a heat engine can achieve is equal to 1 - (Tcold/Thot).

4. What is the purpose of a Reversible Carnot Cycle?

The purpose of a Reversible Carnot Cycle is to describe the theoretical maximum efficiency that a heat engine can achieve. While no real-world heat engine can operate at 100% efficiency, the Reversible Carnot Cycle serves as a benchmark for comparing the efficiency of real heat engines and improving their design.

5. What are the limitations of a Reversible Carnot Cycle?

The Reversible Carnot Cycle assumes ideal conditions such as a perfect insulation and reversible processes, which do not exist in real-world systems. Additionally, the cycle only works with a perfect gas as the working fluid, and it does not account for any energy losses due to friction or other factors. Therefore, the efficiency of a real heat engine will always be lower than the theoretical efficiency of a Reversible Carnot Cycle.

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