Collision of thermal neutrons and Cobalt

AI Thread Summary
The discussion centers on the calculation of the activity of Cobalt-60 produced from the capture of thermal neutrons by Cobalt-59. The initial calculations suggested an incorrect activity value of 2.4 x 10^16 Bq, while the official result is 6 x 10^11 Bq. The error was identified as omitting a crucial factor of t/τ in the final equation, which reflects the linear increase of activity over time. Correcting this leads to the accurate result consistent with established values. The conversation highlights the importance of careful consideration of decay constants in nuclear reaction calculations.
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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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