1540470959-Boundary_Value_Problems_and_Partial_Differential_Equations__Powers

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2.4 Example: Insulated Bar 161


EXERCISES



  1. Using the initial condition


u(x, 0 )=T 1 x
a

, 0 <x<a,

find the solutionu(x,t)of Eqs. (1)–(3). Sketchu(x, 0 ),u(x,t)for some
t>0 (using the first three terms of the series), and the steady-state solu-
tion.


  1. Repeat Exercise 1 using the initial condition


u(x, 0 )=T 0 +T 1

(x
a

) 2

, 0 <x<a.


  1. Same as Exercise 1, but with initial condition


u(x, 0 )=






2 T 0 x
a ,^0 <x<

a
2 ,
2 T 0 (a−x)
a ,

a
2 <x<a.


  1. Solve Eqs. (1)–(3) using the initial conditionu(x, 0 )=f(x),where


f(x)=






T 1 , 0 <x<a 2 ,

T 2 , a
2

<x<a.


  1. Consider this heat problem, which is related to Eqs. (1)–(3):
    ∂^2 u
    ∂x^2 =


1

k

∂u
∂t,^0 <x<a,^0 <t,
∂u
∂x(^0 ,t)=S^0 ,

∂u
∂x(a,t)=S^1 ,^0 <t,
u(x, 0 )=f(x), 0 <x<a.
a.Show that the steady-state problem has a solution if and only ifS 0 =S 1 ,
and give a physical reason why this should be true. (Recall that the heat
fluxqis proportional to the derivative ofuwith respect tox.) Find the
steady-state solution if this condition is met.
b.Ifthesteady-statesolutionv(x) exists, show that the “transient,”
w(x,t)=u(x,t)−v(x), has the boundary conditions
∂w
∂x(^0 ,t)=^0 ,

∂w
∂x(a,t)=^0 ,^0 <t.
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