Troubleshooting Nuclear Reactions: Decay, Gamma Rays & More

In summary: Correction:The way to find out how much ##^{116m}##In was formed in 10 minutes is to measure how many decays to Sn took place in 120 minutes.sorry about that. So the path is1 flux ##\rightarrow## parents ##^{116m}##In2 parents ##^{116m}_{\ \ 49}##In ##\rightarrow## ##\beta, \gamma## decay product ##^{116}_{\ \ 50}##SnThe daughter does not capture a neutron from the parent. The daughter undergoes beta decay (i.e. one neutron emits an electron and becomes a proton) yielding an excited state of the ##^{116}_{\ \ 50}##Sn
  • #1
Graham87
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Homework Statement
See pictures
Relevant Equations
See pictures
The problem comes with solutions. However, I dont get the 3 steps in the solutions. Why do they calculate decay for 120min in step 3? And why is only the daughter nuclide relevant and no granddaughter? There might be something lacking in my knowledge about nuclear reactions.
Also, I don't know what to use with the information "most likely gamma ray" in the question. I know it is gamma37, but what should I derive from knowing that?

Thanks!
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  • #2
Graham87 said:
1 Why do they calculate decay for 120min in step 3?
2 And why is only the daughter nuclide relevant and no granddaughter?
3 Also, I don't know what to use with the information "most likely gamma ray" in the question. I know it is gamma37, but what should I derive from knowing that?
1. It says so in the problem statement : they measure from 5 to 125 min
2. that last one does not decay
3. Its probability (yield) is used to divide by

And you'll learn about decay processes by doing exercises like this.. :smile:

##\ ##
 
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  • #3
BvU said:
1. It says so in the problem statement : they measure from 5 to 125 min
2. that last one does not decay
3. Its probability (yield) is used to divide by

And you'll learn about decay processes by doing exercises like this.. :smile:

##\ ##
Regarding to calculate the fluence rate of the neutrons: how does the process of the neutrons in the reaction work? Are there neutrons decaying from the daughter particle? I cant see it. According to the reaction table the neutrons are coming from the parent particle 115(In) + n ? The daughter 116m(In) is an excited state but has no neutron decay?

So if we want to calculate the fluence rate of neutrons, why does the solution calculate the decay of the daughter, if it includes no neutrons?
Or does the daughter decay actually contribute neutrons? In that case I think I'm getting it :)
 
  • #4
Neutrons don't play a role in the decay process that is described, only in the formation of the ##^{115}##In .
The flux of incoming neutrons is determined from the amount of ##^{115}##In that is found and the cross section.

##\ ##
 
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  • #5
Oh, ok. I don't get step 3 - calculate the decay of the daughter for t3. What do we need that for to find the flux if the flux is from the incoming neutrons in the parent?

Thanks for the replies!
 
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  • #6
Graham87 said:
Oh, ok. I don't get step 3 - calculate the decay of the daughter for t3. What do we need that for to find the flux if the flux is from the incoming neutrons in the parent?
The way to find out how much ##^{115}##In was formed in 10 minutes is to measure how many decays to Sn took place in 120 minutes.
Thanks for the replies!
You are welcome; that's what PF is for...
 
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  • #7
BvU said:
The way to find out how much ##^{115}##In was formed in 10 minutes is to measure how many decays to Sn took place in 120 minutes.
You are welcome; that's what PF is for...
Aha, that clears it. But how is that so? So this is because the radioactive decay is proportional to the number of daughter isotopes, which in turn is proportional to the neutron flux rate since the daughter captures neutrons from the parent?
I think I got most of it now!
Big thanks! Really appreciate it.
 
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  • #8
One more small detail:

Looking at your solution step 1 I am puzzled by step 1. I think
1682692129807.png
is wrong:
$$\begin{align*}
{{\rm d} N_D\over {\rm d} t}&= \dot\Phi\sigma N_P - \lambda N_D \\ \ \\
{{\rm d} (e^{\lambda t} N_D )\over {\rm d} t}&= \lambda e^{\lambda t} N_D + e^{\lambda t} {{\rm d} N_D\over {\rm d} t} \\ \ \\
& = \lambda e^{\lambda t} N_D + e^{\lambda t} \dot\Phi\sigma N_P - e^{\lambda t} \lambda N_D \\ \ \\
& = e^{\lambda t} \dot\Phi\sigma N_P \tag 1
\end{align*}
$$and not ##\left (\dot\Phi\sigma N_P - \lambda N_D\right ) e^{\lambda t} ## as the solution states...

And then the next line in the solution follows from integrating left and right of ##(1)## from ##t=0## to ##t=t_1## :
we get $$\begin{align*}
e^{\lambda t_1} N_D(t_1) &= {\dot\Phi\sigma N_P\over \lambda} \ \left (e^{\lambda t_1} - 1\right ) \Leftrightarrow \\ \ \\
N_D(t_1) &= {\dot\Phi\sigma N_P\over \lambda} \ \left (1-e^{-\lambda t_1} \right )
\end{align*}
$$
 
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  • #9
Graham87 said:
Aha, that clears it. But how is that so? So this is because the radioactive decay is proportional to the number of daughter isotopes, which in turn is proportional to the neutron flux rate since the daughter captures neutrons from the parent?

Correction:
BvU said:
The way to find out how much ##^{116m}##In was formed in 10 minutes is to measure how many decays to Sn took place in 120 minutes.
sorry about that. So the path is
1 flux ##\rightarrow## parents ##^{116m}##In
2 parents ##^{116m}_{\ \ 49}##In ##\rightarrow## ##\beta, \gamma## decay product ##^{116}_{\ \ 50}##Sn

The daughter does not capture a neutron from the parent. The daughter undergoes beta decay (i.e. one neutron emits an electron and becomes a proton) yielding an excited state of the ##^{116}_{\ \ 50}##Sn
This nucleus loses energy by emitting a gamma (photon)

##\ ##
 
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FAQ: Troubleshooting Nuclear Reactions: Decay, Gamma Rays & More

What are the common causes of unexpected results in nuclear decay experiments?

Unexpected results in nuclear decay experiments can often be attributed to factors such as contamination of the sample, inaccurate calibration of detection equipment, or external environmental influences like temperature and pressure variations. Ensuring proper experimental controls and calibration can help mitigate these issues.

How can I differentiate between gamma rays and other types of radiation in my measurements?

Gamma rays can be differentiated from other types of radiation (like alpha and beta particles) by their high energy and penetrating power. Using a scintillation detector or a Geiger-Müller counter with appropriate shielding can help identify gamma rays. Additionally, the energy spectrum of gamma rays is distinct and can be analyzed using a spectrometer.

What steps should I take if my nuclear reaction does not produce the expected isotopes?

If the expected isotopes are not produced, first verify the purity of your reactants and the accuracy of your target material. Check the experimental setup for any misalignments or errors in the reaction conditions, such as temperature, pressure, or neutron flux. Re-evaluating the theoretical calculations and cross-sections for the reactions involved may also provide insights.

How do I ensure the accuracy of my gamma ray spectroscopy readings?

To ensure accuracy in gamma ray spectroscopy, regularly calibrate your equipment using known standard sources. Maintain a stable environment to minimize background radiation and temperature fluctuations. Use proper shielding to reduce noise and ensure that the detector is properly aligned with the sample. Regular maintenance and software updates can also help maintain accuracy.

What are the safety precautions I should follow when working with radioactive materials?

When working with radioactive materials, always follow established safety protocols such as wearing appropriate personal protective equipment (PPE), using shielding to minimize exposure, and working in a well-ventilated area. Use tools like tongs or remote handling devices to maintain distance from the source, and always monitor radiation levels with appropriate detection devices. Proper storage and disposal of radioactive materials are also crucial to ensure safety.

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