B.C.Solve. Completely to the final form of the 200Solution as a Fourier Series the heat.equation boundary value problem.IC.(homogeneous PDĚ, mixed, homogeneous B.C.)S sul sulodxe to, L7 L: 2, k=4 t2012u - R 2²u = 032tu(0₁t) = 0u(Lt) = Ode all st 3.3u(x,0) = \JA:2x² 10 t poodopso rot jand on :/ 10 i dia9-109 + 1 - 2 +9-15(4) mei + (as) 223-1)0) + ((s) ora 1 - (0) 205-1) ₁Fi-Cost

B.C. IC Solve. Completely to the final form of the 200 Solution as a Fourier Series the heat equation boundary value problem. (homogeneous PDĚ, mixed, X = [0,L] L= 2, k= 4 +₁ zon R 2²u 2u 24, u(o₁t) = 0 u(L₁Z) = 0 u(x, 0) = 1 A homogeneous BC.) - = 0 2x² nut Lond op So not sand of A 10 M dia (start 9-10 N TAS

B.C. IC Solve. Completely to the final form of the 200 Solution as a Fourier Series the heat equation boundary value problem. (homogeneous PDĚ, mixed, X = [0,L] L= 2, k= 4 +₁ zon R 2²u 2u 24, u(o₁t) = 0 u(L₁Z) = 0 u(x, 0) = 1 A homogeneous BC.) - = 0 2x² nut Lond op So not sand of A 10 M dia (start 9-10 N TAS

Advanced Engineering Mathematics

10th Edition

ISBN:9780470458365

Author:Erwin Kreyszig

Publisher:Erwin Kreyszig

Chapter2: Second-order Linear Odes

Section: Chapter Questions

Problem 1RQ

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Setup is from image 1. Use the Green's function (see image 2) to derive the expression for 1d Born's approximation.
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