Collision of thermal neutrons and Cobalt

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Homework Help Overview

The discussion revolves around the interaction of thermal neutrons with cobalt-59, specifically focusing on the calculation of the activity of cobalt-60 produced from neutron capture. The problem involves concepts from nuclear physics, including cross sections, decay processes, and differential equations related to radioactive decay.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of neutron capture and subsequent decay, questioning the validity of the original poster's approach and the constants used in their equations. There is also a consideration of how the decay of cobalt-60 affects the overall activity calculation.

Discussion Status

The discussion is active, with participants providing feedback on the original poster's calculations and suggesting corrections. Some participants express uncertainty about the "official" results, while others offer clarifications on the mathematical expressions involved.

Contextual Notes

Participants are navigating the complexities of radioactive decay and neutron interactions, with some noting discrepancies between their calculations and established results. There is an acknowledgment of potential errors in the original poster's method, particularly regarding the treatment of constants and the relationship between activity and time.

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Homework Statement


The cross section of ##^{59}Co## for capturing the thermal neutrons is ##2000 fm^2##. A ##10g##, thin paper of ##^{59}Co## is radiated for ##100 hours## in reactor with neutron flux ##2\cdot 10^{18} /m^2s##. Density of ##^{59}Co## is ##8.9g/cm^3##. Half life time of ##^{60}Co## is ##5.2 years##.

Homework Equations


The Attempt at a Solution



So what happens is ##n+##^{59}Co##->^{60}Co## which than decays with ##t_{1/2}=5.2 years##.

Well, the number of successful collisions is ##dN=\frac{NN_{59}\sigma }{S}## and dividing that by ##dt## gives me ##\frac{dN}{dt}=jN_{59}\sigma ##.

Of course, some of the ##^{60}Co## will immediately start to decay, therefore:

##\frac{dN}{dt}=jN_{59}\sigma -\frac{N}{\tau }##

Solving this differential equations using ##N=C+Ae^{-t/\tau }##

Leaves me with ##N=\tau (jN_{59}\sigma -1)(1-e^{-t\tau })## where ##t/\tau <<1## so

##\frac{N}{t}=jN_{59}\sigma -1= 2.4\cdot 10^{16}Bq## instead of ##6\cdot 10^{11}Bq##.

Note that ##N_{59}=\frac{mN_a}{M}##.

Why is this wrong? :(
 
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You're solution seems correct. I'm not sure why you say it's wrong.
 
Basically the only reason why I think this method is wrong is because the "official" result is ##6\cdot 10^{11}Bq##

I also remembered that I could take into account here ##\frac{dN}{dt}=jN_{59}\sigma -\frac{N}{\tau }## that already excited ##^{60}Co## can't get even more exited. Therefore the more exact solution would follow from inserting that ##N_{59}=N_{59}^0-N##

Of course "official" results can be wrong too so if you agree with my solution and if nobody else will complain than I think it is safe to assume that what I did is ok.
 
Your solution is incorrect. If you determine the constants C and A correctly, you will find:
N = \tau j N_{59} \sigma (1-e^{\frac{t}{\tau}})
Then, as you said, t<<τ, so:
N = \tau j N_{59} \sigma {\frac{t}{\tau}} = t j N_{59} \sigma
This makes sense, since at early times the activity increases linearly with time. So the activity N/τ is:
\frac{N}{\tau} = \frac{t}{\tau} j N_{59} \sigma

It is this factor of t/τ that you omitted. When you plug in the numbers, you do in fact get 6E11 Becquerels.
 
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Where one wrote N/t, it should be N/τ (where τ is tau = 1/λ), lambda = decay constant, and tau is the mean lifetime.
 
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Ah, of course!

Thanks to all of you!
 

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