Answer to Question #214216 in Differential Equations for Manoranjan Kumar

Question #214216
A bar 100 cm long, with insulated sides, has its ends kept at 0
1
Expert's answer
2021-07-08T11:50:51-0400

A bar 100 cm long, with insulated sides, has its ends kept at 0° Celsius and 100° Celsius until

steady state condition prevails. The two ends are then suddenly insulated and kept so. Find

the temperature distribution.​

Solution

The heat flow flow equation is

"\\nabla ^2u(x,t)={1\\over \\alpha ^2}{\\partial u\\over \\partial t}...................(i)"

where "u(x, t)" is the temperature. Because the sides of the bar are insulated, the heat flows only in the "x" direction; the same happens for a slab of finite thickness but infinitely large. The initial condition is "u(x, 0) = 100" and the boundary condition for "t > 0" is "u(0, t) = u(100, t) = 0" . We search for a solution of the form "u(x, t) = F(x)T(t)" ; the differential equation "(i)" gives

"{\u2202 ^2F\\over \u2202x^2} + k ^2F = 0 , \\implies F = A cos kx + B sin kx.............(ii)"

"{\u2202T\\over \u2202t} = \u2212k^2\u03b1^2T , \\implies T = e^{\u2212k^2\u03b1^2t}....................(iii)"

Because of the boundary condition in "x = 0" , we have "A = 0" . To satisfy "u(100, t) = 0" , we find discrete values of "k:"

"sin 100k = 0 ,\\implies k_n ={n\u03c0\\over100}," ".........(iv)" ,for "n = 1, 2, 3, . . ."

Finally, we must satisfy the initial condition

"u(x, 0) =\\displaystyle\\sum_{n=1}^\u221eb_n sin{n\u03c0x\\over 100}= 100 ...............(v)" ,for "0 \u2264 x \u2264 10."

Now,solving for "b_n" we have

"b_n ={2\\over 100} \\int_0^{100 }sin{n\u03c0x\\over 100}dx = \u2212{200\\over n\u03c0}cos{n\u03c0x\\over 100}\\mid_0^{100}"

"={200\\over n\u03c0}[1 \u2212 (\u22121)^n]"

"= \\begin{cases}\n {400\\over \\pi n}&\\text{for }{odd} {n} \\\\\n 0 &\\text{for } {even} n\n\\end{cases}" "..............(vii)"

after using "cos (n\u03c0 )= (\u22121)^n" for integer "n" . The solution to the differential equation "(i)" with the given boundary conditions is then


"u (x,t)={400\\over \u03c0}\\sum_ {oddn}{1\\over n}e^{\u2212({n\u03c0\u03b1\\over 100})^2t }sin {n\u03c0x\\over 100}"


where “odd n” means a sum over n = 1, 3, 5, . . ..


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