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I was overlooking page 47 of "The Physics of the Manhattan Project" 2.2 Critical Mass: Diffusion Theory, and author Bruce Cameron Reed reported that:
Can anyone explain how Bruce Cameron Reed got from (2.18) to (2.19)
I tried plugging ## N(r,t) = N(r) N(t) ## into (2.18) to get (2.19), but it just does not make any sense to me on how there is a fraction of ## \frac{1}{N_r} ## multiplied to the second term after the equals sign
Assuming ## N ## in the first term after the equals sign is ## N(r,t) ## I cannot see how using algebra would allow a person to arrive to (2.19)
I have also tried to take advantage of the relationship
## \Big (\frac{\partial N(r,t)}{\partial t} \Big)_t = N'(t) N(r) ## but even taking advantage of this I still could not figure out how Reed transformed (2.18) to (2.19)
## \Big (\frac{\partial N}{\partial t} \Big)_t = \frac{v}{\lambda_f} \big( \nu-1 \big) N + \frac{v \lambda_t}{3} \big( \nabla^2 N_r \big)_r ## \hfill (2.18)
can be modified. Basically, since ## N(r,t) = N(t)_tN(r)_r ## we can use separation of variables to modify (2.18) to get ##\frac{1}{N_t} \Big (\frac{\partial N_t}{\partial t} \Big)_t = \frac{v}{\lambda_f} \big( \nu-1 \big) + \frac{v \lambda_t}{3 N_r} \Bigg( \frac{1}{r^2} \frac{\partial}{\partial r} \Bigg( r^2 \frac{\partial N_r}{\partial r} \Bigg) \Bigg) ## \hfill (2.19)
Can anyone explain how Bruce Cameron Reed got from (2.18) to (2.19)
I tried plugging ## N(r,t) = N(r) N(t) ## into (2.18) to get (2.19), but it just does not make any sense to me on how there is a fraction of ## \frac{1}{N_r} ## multiplied to the second term after the equals sign
Assuming ## N ## in the first term after the equals sign is ## N(r,t) ## I cannot see how using algebra would allow a person to arrive to (2.19)
I have also tried to take advantage of the relationship
## \Big (\frac{\partial N(r,t)}{\partial t} \Big)_t = N'(t) N(r) ## but even taking advantage of this I still could not figure out how Reed transformed (2.18) to (2.19)
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