There is the boundary value problem
"u_t(x, t) = ku_{xx}(x, t)" , for "t > 0" and "0 < x < L" (1)
"u(0, t) = T_0" and "u(L, t) = T_L" , for "t > 0"
"u(x, 0) = f(x)" , for "0 \\leqslant x \\leqslant L"
A steady-state temperature is one that does not depend on time.
Then ut = 0, so the heat equation (1) simplifies uxx = 0. Hence we are looking for a function us(x) defined for 0 < x < L such that
"\\frac{\u2202^2u_s}{\u2202x^2}(x) = 0" , for "0 < x < L"
"u_s(0, t) = T_0" and "u_s(L,t) = T_L" for "t > 0"
The solution to this boundary value problem is easily found,since the general solution
of the differential equation is us(x) = Ax + B; where A and B are arbitrary constants.
Then the boundary conditions reduce to
us(0) = B = T0 and us(L) = AL + B = TL
We conclude that B = T0 and A = (TL – T0)/L, so the steady-state temperature is
"u_s(x) = (T_L \u2013 T_0)\\frac{x}{L} + T_0"
"u_s(x) = (100 \u2013 200)\\frac{x}{15} + 200 = 200 \u2013 6.66x"
Answer: 200 – 6.66x
Comments
Leave a comment