Using Separation of Variables to Modify Neutron Density Diff

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SUMMARY

This discussion focuses on the mathematical transformation of neutron density diffusion equations as presented by Bruce Cameron Reed in "The Physics of the Manhattan Project." Specifically, the transition from equation (2.18) to (2.19) is analyzed, where the separation of variables technique is applied to express the neutron density as a product of spatial and temporal functions. The confusion arises around the presence of the term ##\frac{1}{N_r}## in the modified equation, which requires a deeper understanding of the algebraic manipulation involved in the separation process.

PREREQUISITES
  • Understanding of diffusion theory in nuclear physics
  • Familiarity with separation of variables in differential equations
  • Knowledge of neutron density functions and their mathematical representations
  • Basic algebraic manipulation skills in the context of calculus
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  • Study the derivation of the separation of variables technique in partial differential equations
  • Review the concepts of critical mass and neutron diffusion in nuclear physics
  • Examine the mathematical properties of the Laplacian operator in spherical coordinates
  • Explore advanced algebraic techniques for manipulating differential equations
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tasm
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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:

## \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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tasm said:
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)

BY THE WAY, I FORGOT TO GIVE A LINK TO THE PDF OF THE BOOK. HERE IT IS:

http://download.springer.com/static/pdf/164/bok%253A978-3-642-14709-8.pdf?originUrl=http%3A%2F%2Flink.springer.com%2Fbook%2F10.1007%2F978-3-642-14709-8&token2=exp=1477589641~acl=%2Fstatic%2Fpdf%2F164%2Fbok%25253A978-3-642-14709-8.pdf%3ForiginUrl%3Dhttp%253A%252F%252Flink.springer.com%252Fbook%252F10.1007%252F978-3-642-14709-8*~hmac=43061743582b27e324f2238b065b3a347a0078d2a4cc041f0781d563e9739e2a
 

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