Time for which RTG will supply the required energy output?

In summary: PU 238 to Pu 239. Both the Cassini and Galileo missions used Pu 238 RTGs. However, in summary, the NASA Galileo space probe to Jupiter 'contained 49 lb of plutonium to provide 285 watts of electricity through its radioactive thermonuclear generator (RTG)'. Assuming that the plutonium is 239Pu, which is built into a small nuclear reactor and that the efficiency of the RTG is 10 %, what is the maximum time for which the RTG will supply the required energy output?
  • #1
moenste
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12

Homework Statement


A newspaper article stated that the NASA Galileo space probe to Jupiter 'contained 49 lb of plutonium to provide 285 watts of electricity through its radioactive thermonuclear generator (RTG)'.

(Note: An RTG is a device for converting thermal energy produced by fission into electrical energy.)

Assuming that the plutonium is 239Pu, which is built into a small nuclear reactor and that the efficiency of the RTG is 10 %, what is the maximum time for which the RTG will supply the required energy output?

(Take the energy emitted for each nuclear disintegration of the 239Pu to be 32 pJ, NA = 6.0 * 1023 mol-1, 1 lb = 0.45 kg.)

Answer: 6.2 * 1011 s.

2. The attempt at a solution
We have the mass m = 22.05 kg, power P = 285 W, element 239Pu, energy emitted per disintegration E = 32 * 10-12 J and the Avogadro number with the fact that the RTG is 10 % efficient.

Power P = Work done W / Time t where, as I understand, t is what we need to find.

We know the energy emitted, but how many disintegrations are there? It says "for each disintegration", but how to find how many of them are there are what kind of disintegration a nuclear disintegration is?

So, I think it is required to find the number of disintegrations, then calculate the total work done and then calculate time. Though I'm not sure about the 10 % efficiency. Efficiency = Power output / Power input. So for the final calculation it should be used 285 * 10 % = 28.5 W (like 28.5 W = 32 * 10-12 J * X number disintegrations / Y maximum time for which the RTG will supply the required energy output).

Is this logic correct? How to find the number of disintegrations?
 
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  • #2
To find the disintegration rate, you need the half life of 239Pu. If it's not supplied in the question, you need to look it up.

10% efficiency means that only 10% of the energy output is converted to electricity. If the requirement is for 285W of electricity, then the total energy output is obviously much higher.
 
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  • #3
Jonathan Scott said:
To find the disintegration rate, you need the half life of 239Pu. If it's not supplied in the question, you need to look it up.
OK, so we have T1 / 2 = 2.4 * 104 years or * 365 days * 24 hours * 3600 minutes and seconds = 7.56864 * 1011 seconds.

Jonathan Scott said:
10% efficiency means that only 10% of the energy output is converted to electricity. If the requirement is for 285W of electricity, then the total energy output is obviously much higher.
You mean 10 % of the energy INput is converted into electricity (OUTput)?

So the requirement is to have 285 W as output, so input should be 2850 W.
 
  • #4
moenste said:
You mean 10 % of the energy INput is converted into electricity (OUTput)?
So the requirement is to have 285 W as output, so input should be 2850 W.
That's close enough. By my way of thinking, the plutonium is producing a total thermal energy output of 2850W and the RTG converts 285W of that to electric power.

Now you need to use the usual equation to determine the disintegration rate from the half life.
 
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  • #5
Something tells be that at some point the original problem was "updated", changing the isotope from PU 238 to Pu 239. Both the Cassini and Galileo missions used Pu 238 RTGs.

That said, I have my doubts that the original spec of 49 lb of plutonium would produce enough energy to harvest 285 W if it were Pu 239 and the RTG only 10% efficient. Even initially, never mind over time.

Specific activity of Pu 239 is only 0.06133 Ci/gm (that's curies* per gram) compared to Pu 238's 17.13 Ci/gm. See:
LLNL-TR-490356: Plutonium 239 Equivalency Calculations, J. Wen, July 2011.* A curie is a unit of activity. 1 Ci = 3.7 x 1010 decays per second.
 
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  • #6
Jonathan Scott said:
That's close enough. By my way of thinking, the plutonium is producing a total thermal energy output of 2850W and the RTG converts 285W of that to electric power.

Now you need to use the usual equation to determine the disintegration rate from the half life.
dN / dt = - ln 2 / T1 / 2 * N

But how to find N?

We have 239 gram of plutonium which have 6 * 1023 atoms. But we also have like 22.05 kg, which cannot contain so much atoms, right?

Update
I used N = m NA / Ar, where m is in grams = 22 050 * 6 * 1023 / 239 = 5.5 * 1025 atoms.

dN / dt = - ln 2 / (7.6 * 1011) * 5.5 * 1025 = 5.1 * 1013 Bq.

t = 32 * 10-12 * 5.1 * 1013 / 2850 = 0.563 s.

gneill said:
Something tells be that at some point the original problem was "updated", changing the isotope from PU 238 to Pu 239. Both the Cassini and Galileo missions used Pu 238 RTGs.

That said, I have my doubts that the original spec of 49 lb of plutonium would produce enough energy to harvest 285 W if it were Pu 239 and the RTG only 10% efficient. Even initially, never mind over time.

Specific activity of Pu 239 is only 0.06133 Ci/gm (that's curies* per gram) compared to Pu 238's 17.13 Ci/gm. See:
LLNL-TR-490356: Plutonium 239 Equivalency Calculations, J. Wen, July 2011.* A curie is a unit of activity. 1 Ci = 3.7 x 1010 decays per second.
In the original post I only changed "plutiniom" (or something close to it) to "plutonium". The numbers are all correct, checked them with the book. I think it's just a made-up problem, the only quote from the article they are giving is in
moenste said:
'contained 49 lb of plutonium to provide 285 watts of electricity through its radioactive thermonuclear generator (RTG)'
 
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  • #7
Calculate the initial power output of your 49 pounds of Pu 239. You've determined that it has an activity of 5.1 x 1013 Bq, and you're told that each decay delivers 32 pJ of energy. So, what does that give you?
 
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  • #8
gneill said:
Calculate the initial power output of your 49 pounds of Pu 239. You've determined that it has an activity of 5.1 x 1013 Bq, and you're told that each decay delivers 32 pJ of energy. So, what does that give you?
Yes, and I calculated 32 pJ * 5.1 * 1013 Bq.
moenste said:
t = 32 * 10-12 * 5.1 * 1013 / 2850 = 0.563 s.
Since Bq is disintegration per second, so if we multiply these two numbers we'll get total Work done W.
 
  • #9
No, I asked for the power output. You've gone and divided by 2850 for some reason. If that 2850 is a power in watts, then your calculation would yield a unitless number, not a time.

In fact, if 2850 W is the necessary minimum power output of the Plutonium, what you've shown is that the RTG will only produce about 56 % of the required minimum amount.
 
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  • #10
gneill said:
No, I asked for the power output. You've gone and divided by 2850 for some reason. If that 2850 is a power in watts, then your calculation would yield a unitless number, not a time.

In fact, if 2850 W is the necessary minimum power output of the Plutonium, what you've shown is that the RTG will only produce about 56 % of the required minimum amount.
What shall I do then? I still don't understand what do you suggest, sorry.
 
  • #11
moenste said:
What shall I do then? I still don't understand what do you suggest, sorry.
I'm saying that the problem is not solvable as it is given. The author of the problem may have changed some values and not properly checked the result to see that the problem scenario was valid.

If you can prove that the problem is not workable then that is a valid answer.

The problem author may have misinterpreted a result when he made checked it. I think he ignored a sign when he solved for the time and interpreted a negative time value as a positive one. Allow me to demonstrate.

Suppose that when brand new the RTG produces a power output ##P_o##. The RTG's isotope has a decay constant ##λ##, so that the power output will decay over time according to:

##P(t) = P_o e^{-λt}##

If the minimum usable power output is ##P_{min}## then solve for t in:

##P_{min} = P_o e^{-λt}##

##t = \frac{-ln\left( \frac{P_{min}}{P_o} \right)}{λ}##

Now, if ##P_{min}## is less than ##P_o## then all is well: the ln function will return a negative value, cancelling the negative sign in front of it. But if ##P_{min}## happens to be greater than ##P_o##, the result of the ln is a positive value and the overall result will be negative.

I plugged in the values associated with this problem and obtained a time of ##t = -6.24 \times 10^{11} s##.

I think that this is pretty good evidence that the author mucked up :smile:
 
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  • #12
gneill said:
I'm saying that the problem is not solvable as it is given. The author of the problem may have changed some values and not properly checked the result to see that the problem scenario was valid.

If you can prove that the problem is not workable then that is a valid answer.

The problem author may have misinterpreted a result when he made checked it. I think he ignored a sign when he solved for the time and interpreted a negative time value as a positive one. Allow me to demonstrate.

Suppose that when brand new the RTG produces a power output ##P_o##. The RTG's isotope has a decay constant ##λ##, so that the power output will decay over time according to:

##P(t) = P_o e^{-λt}##

If the minimum usable power output is ##P_{min}## then solve for t in:

##P_{min} = P_o e^{-λt}##

##t = \frac{-ln\left( \frac{P_{min}}{P_o} \right)}{λ}##

Now, if ##P_{min}## is less than ##P_o## then all is well: the ln function will return a negative value, cancelling the negative sign in front of it. But if ##P_{min}## happens to be greater than ##P_o##, the result of the ln is a positive value and the overall result will be negative.

I plugged in the values associated with this problem and obtained a time of ##t = -6.24 \times 10^{11} s##.

I think that this is pretty good evidence that the author mucked up :smile:
t = - ln (285 / 2850) / (ln 2 / 7.6 * 1011) = 2.52 * 1012 s. What am I missing?
 
  • #13
You've used incorrect power values. The minimum required RTG output power ##P_{min}## is 2850 W (so that the 10% recoverable is 285 W). The initial power output of the RTG, ##P_o##, is the power output you calculated for the given initial mass of isotope. I asked you to calculate it in post #7.
 
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  • #14
gneill said:
Calculate the initial power output of your 49 pounds of Pu 239. You've determined that it has an activity of 5.1 x 1013 Bq, and you're told that each decay delivers 32 pJ of energy. So, what does that give you?
But power has no connection to Bq. At least I can't find any formula on that.

I thought since dN / dt = disintegrations per second I could use that number to multiply on 32 pJ and find total work done W in Joules.
 
  • #15
moenste said:
But power has no connection to Bq. At least I can't find any formula on that.
Bq is decays per second. Each decay produces a bit of energy. Energy per second is power.
I thought since dN / dt = disintegrations per second I could use that number to multiply on 32 pJ and find total work done W in Joules.
Yes, that's right.
 
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  • #16
gneill said:
Bq is decays per second. Each decay produces a bit of energy. Energy per second is power.

Yes, that's right.
Yes, the second P = 1622 W. Now I also get - 6.15 * 1011 s.

Thank you!
 

FAQ: Time for which RTG will supply the required energy output?

How long will an RTG last?

The longevity of an RTG (Radioisotope Thermoelectric Generator) varies depending on the specific design and materials used. However, on average, an RTG can last anywhere from 10-40 years before needing to be replaced.

What factors determine the time for which an RTG can supply energy?

The primary factors that determine the energy output of an RTG are the type and amount of radioactive material used, the efficiency of the thermoelectric conversion process, and the external temperature and conditions of the RTG.

How much energy can an RTG supply?

The amount of energy an RTG can supply depends on the specific design and size of the RTG. On average, an RTG can produce anywhere from a few watts to several hundred watts of power.

Can the energy output of an RTG be increased?

The energy output of an RTG is primarily determined by the amount of radioactive material used, so increasing the amount of material can increase the energy output. However, this also increases the cost and potential safety risks of the RTG.

How does the energy output of an RTG change over time?

The energy output of an RTG will gradually decrease over time as the radioactive material decays. However, this decrease is relatively slow and can be predicted based on the half-life of the material used in the RTG.

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