Problem 3. Consider the classical solution to the initial boundary-value problem for the heat equation: (t, x) E (0, 0) x (0,1), te (0, 0), л€ [0, 1]. dru – Kôrau = 0, - u(t,0) = u(t, 1) = 0, (1.6)...


Problem 3. Consider the classical solution to the initial boundary-value problem for the heat equation:<br>(t, x) E (0, 0) x (0,1),<br>te (0, 0),<br>л€ [0, 1].<br>dru – Kôrau = 0,<br>-<br>u(t,0) = u(t, 1) = 0,<br>(1.6)<br>u(0, x) = 4x(1 – x),<br>(1) Show that 0 < u(t, x) < 1 for all (t, x) E (0, ∞) × [0, 1].<br>(2) Show that u(t, x) = u(t, 1 – x) for all (t, x) E [0, c) × [0, 1].<br>(3) Use the energy method to show that<br>E(t) = | lu(t, x)|²dæ<br>(1.7)<br>is a decreasing function of time.<br>1<br>

Extracted text: Problem 3. Consider the classical solution to the initial boundary-value problem for the heat equation: (t, x) E (0, 0) x (0,1), te (0, 0), л€ [0, 1]. dru – Kôrau = 0, - u(t,0) = u(t, 1) = 0, (1.6) u(0, x) = 4x(1 – x), (1) Show that 0 < u(t,="" x)="">< 1="" for="" all="" (t,="" x)="" e="" (0,="" ∞)="" ×="" [0,="" 1].="" (2)="" show="" that="" u(t,="" x)="u(t," 1="" –="" x)="" for="" all="" (t,="" x)="" e="" [0,="" c)="" ×="" [0,="" 1].="" (3)="" use="" the="" energy="" method="" to="" show="" that="" e(t)="|" lu(t,="" x)|²dæ="" (1.7)="" is="" a="" decreasing="" function="" of="" time.="">

Jun 05, 2022
SOLUTION.PDF

Get Answer To This Question

Related Questions & Answers

More Questions »

Submit New Assignment

Copy and Paste Your Assignment Here