The neutron diffusion equation with a (plane) source at x = 0 is d² f(x) dx² · + w² f(x) = Q(x) where f(x) is the flux of neutrons (|f(x) → 0 as x → ∞), Q8(x) is the plane source at x = 0 (where (x) is the Dirac delta function), and w² is a constant. (a) Fourier transform this equation for f(x) and write the corresponding equation that is satisfied by F(k), the transform of f(x). (b) Solve the equation you found in part (a) for F(k). (c) Find f(x) by using the inverse Fourier transform to obtain the solution for all x = (-∞, ∞).

Linear Algebra: A Modern Introduction
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Author:David Poole
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Chapter4: Eigenvalues And Eigenvectors
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The neutron diffusion equation with a (plane) source at x = 0 is
d² f(x)
dx²
· + w² f(x) = Q(x)
where f(x) is the flux of neutrons (|f(x) → 0 as x → ∞), Q8(x) is the plane source at x = 0
(where (x) is the Dirac delta function), and w² is a constant.
(a) Fourier transform this equation for f(x) and write the corresponding equation that is satisfied
by F(k), the transform of f(x).
(b) Solve the equation you found in part (a) for F(k).
(c) Find f(x) by using the inverse Fourier transform to obtain the solution for all x = (-∞, ∞).
Transcribed Image Text:The neutron diffusion equation with a (plane) source at x = 0 is d² f(x) dx² · + w² f(x) = Q(x) where f(x) is the flux of neutrons (|f(x) → 0 as x → ∞), Q8(x) is the plane source at x = 0 (where (x) is the Dirac delta function), and w² is a constant. (a) Fourier transform this equation for f(x) and write the corresponding equation that is satisfied by F(k), the transform of f(x). (b) Solve the equation you found in part (a) for F(k). (c) Find f(x) by using the inverse Fourier transform to obtain the solution for all x = (-∞, ∞).
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