How to Calculate Steam Engine Efficiency and Water Usage in a Power Plant

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The discussion revolves around calculating the efficiency and water usage of a steam power plant using two steam engines. The first engine operates between 718°C and 427°C, while the second operates between 419°C and 270°C, with a combined efficiency derived from their individual Carnot efficiencies. The participants clarify that the power output of 950 MW is the total output from both engines, and the heat rejected by the first engine is crucial for determining the heat input for the second. For water cooling, the correct approach involves calculating the heat that must be removed based on the output power and the temperature increase allowed. Overall, the conversation emphasizes the importance of correctly applying thermodynamic principles and understanding the relationship between the engines' efficiencies.
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Homework Statement


At a steam power plant, steam engines work in pairs, the heat output of the first one being the approximate heat input of the second. The operating temperatures of the first are 718∘C and 427∘C, and of the second 419∘C and 270∘C.
A) If the heat of combustion of coal is 2.8×107J/kg, at what rate must coal be burned if the plant is to put out 950 MW of power? Assume the efficiency of the engines is 65 % of the ideal (Carnot) efficiency.
B)Water is used to cool the power plant. If the water temperature is allowed to increase by no more than 5.5 C∘ , estimate how much water must pass through the plant per hour.

Homework Equations


e = 1-QL/QH
eideal = 1-TL/TH
e = W/QH

The Attempt at a Solution


for part A
second engine
e2 = W/(QH2) = (950000000J/s)/(QH2)

e2ideal =1-(TL2/TH2) = 1-(427+273)/(718+273) = 1 - 543/692 = .215
e2 = .65(e2ideal) = .65(.215) = .140

.140 =(950000000J/s)/(QH2)
QH2 = (950000000J/s)/(.140) = 6785714286 J/s

QH2 = QL1

e1ideal = 1 - 700/991 = .294
e1 = .65(.294) = .191
.191 = 1 - (QL1)/(QH1)
(QL1)/(QH1) = 1 - .191 = .809
QL1 = (.809)(QH1)

so QH2 = .809(QH1)
QH2 = 6785714286 J/s
.809(QH1) = 6785714286 J/s
QH1 = 8387780329 J/s - heat input of first engine

(8387780329 J/s) (kg/(2.8x10^2 J))
= 299.6 kg/s
but it came up wrong. I can't figure out what I did wrong
 
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The given power output is the sum of the outputs of the two engines, not the output of the second engine alone.
You seem to have used the first engine's temperatures in your calculation for the second engine.
Haven't checked past there.
 
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ahh ok thanks I got it right now
 
im a little confused about the set up for part B
would it work if i used
q = mc(deltaT) where q = 950000000 J/s
c is the specific heat of water and deltaT is 5.5 and solve for m?
 
toothpaste666 said:
im a little confused about the set up for part B
would it work if i used
q = mc(deltaT) where q = 950000000 J/s
c is the specific heat of water and deltaT is 5.5 and solve for m?
The 950MW is the output power. It is not heat. What is the heat that must be removed?
 
the sum of QL for each engine?
 
toothpaste666 said:
the sum of QL for each engine?
No. Some of the QL from the first engine was turned into useful work by the second.
 
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so only the QL for the second?
 
yeah i got it. thanks!
 
  • #10
toothpaste666 said:
so only the QL for the second?
Yes.
 
  • #11
You have written, toothpaste666, in your calcs above:

e2ideal =1-(TL2/TH2) = 1-(427+273)/(718+273) = 1 - 543/692 = .215

And that's wrong. It should be:

e2ideal =1-(TL2/TH2) = 1-(427+273)/(718+273) = 1 - 700/991 = .2936

There may be other mistakes (or not). I've spotted just this one...
 
  • #12
I would prefer a global approach to solve the problem, haruspex permitting... The power plant can be considered as a 'black box' that ingests coal at a given rate, produces a given power of electricity and rejects some quantity of heat per unit of time. We are told that the the efficiencies of the engines are 65% of the Carnot efficiency. Well, the efficiency of the first engine, working between 718 ºC and 427 ºC is 0,29360. That of the second, working between 419 ºC and 270 ºC is 0,21532. Their compounded efficiency is thus 0,29360 + 0,21532 = 0,50892. As we are told that we are left with 65% of that, then we have a global, real efficiency of 0,33080.

Now that we know the efficiency of that 'black box', we can reckon that, from 100 units of coal energy input, 33,08 units become electric energy, and 66,92 units go to heat a mass of water by 5,5ºC .

Little is left, but doing a few sums. I believe that toothpaste666 was doing quite well, but had confused some data in his calculations. I believe that my suggestions are not excessive, in the sense that I'm not violating the rules...
 
  • #13
NTW said:
You have written, toothpaste666, in your calcs above:

e2ideal =1-(TL2/TH2) = 1-(427+273)/(718+273) = 1 - 543/692 = .215

And that's wrong. It should be:

e2ideal =1-(TL2/TH2) = 1-(427+273)/(718+273) = 1 - 700/991 = .2936

There may be other mistakes (or not). I've spotted just this one...
Looks like a typo in copying into PF. The 543 and 692 are right, it's the 427 and 718 that are wrong.
 
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  • #14
NTW said:
the efficiency of the first engine, working between 718 ºC and 427 ºC is 0,29360. That of the second, working between 419 ºC and 270 ºC is 0,21532. Their compounded efficiency is thus 0,29360 + 0,21532 = 0,50892.
Is that valid? Maybe 0,29360 + (1-0,29360)*0,21532?
 
  • #15
haruspex said:
Is that valid? Maybe 0,29360 + (1-0,29360)*0,21532?

You are right, I believe...

The efficiency along the all the fall from 718 ºC to 270 ºC would be 1- (543/991) = 0.45207. You calculate a lower one, 0,4457, that is somewhat lower than the 'extreme' 718 ºC/270 ºC efficiency because of the eight degrees lost in the 'transfer'...
 
  • #16
haruspex said:
Is that valid? Maybe 0,29360 + (1-0,29360)*0,21532?

Which is quite logic, because -in order to obtain total, 'chained' efficiency, you calculate the efficiency of the second machine from the heat rejected from the first machine...
 
  • #17
Accepting, of course, haruspex' correction concerning the chained efficiency, I re-write the global approach to solve the problem. The power plant can be considered as a 'black box' that ingests coal at a given rate, produces a given power of electricity and rejects some quantity of heat per unit of time. We are told that the the efficiencies of the engines are 65% of the Carnot efficiency. Well, the efficiency of the first engine, working between 718 ºC and 427 ºC is 0,29360. That of the second, working between 419 ºC and 270 ºC is 0,21532. Their compounded efficiency is thus 0,29360 + (1-0,29360) * 0,21532 = 0,44570. As we are told that we are left with 65% of that, then we have a global, real efficiency of 0,28971.
Now that we know the efficiency of that 'black box', we can reckon that, from 1000 units of coal energy input, 289,71 units become electric energy, and 710,29 units go to heat a mass of water by 5,5ºC .
 
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  • #18
yeah it looks like i got a little sloppy and confused myself =\. So I can treat this problem as one engine with the combined efficiency instead of two separate engines? thanks for all your help guys
 
  • #19
toothpaste666 said:
yeah it looks like i got a little sloppy and confused myself =\. So I can treat this problem as one engine with the combined efficiency instead of two separate engines? thanks for all your help guys

Yes, but not simply adding the individual efficiencies, as I mistakenly did. Read the posts of haruspex...
 
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