Math 401, Sec 501: Homework 7 Solutions for Wave Equation and Heat Equation - Prof. Stephe, Assignments of Mathematics

Solutions for various problems related to the wave equation and heat equation, including classifying equations as linear homogeneous, linear nonhomogeneous, or nonlinear, finding steady-state temperatures in a bar, and understanding the impact of boundary conditions on the heat equation.

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Pre 2010

Uploaded on 02/10/2009

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Math. 401, Sec. 500 Spring, 2005
Homework 7, due March 9
1. Classify these equations as linear homogeneous, linear nonhomogeneous, or nonlinear.
(Here ut∂u/∂t,etc.)
(a) utt uxx =cos(xt)
(b) ut+u2ux=0
(c) ut+3t
2
u=0
(d) utt uxx =m2u
2. Why do we not make a distinction between “homogeneous” and “nonhomogeneous”
for nonlinear equations? Hint: Try to classify the equation y00 +(cosy)
2=1.
3. [Schaum’s, p. 46, Ex. 2.52] Find the steady-state temperature in a bar whose ends
are located at x=0andx= 10, if these ends are kept at 150C and 100C respectively.
4. Suppose that the boundary conditions (“BC:”) on p. 64 of the notes (and corresponding
lecture on the heat equation with fixed end temperatures) are replaced by
∂u
∂x(t, 0) = F1,∂u
∂x(t, 1) = F2.
(That is, the heat flux through each end of the bars is held constant.) What happens
when you attempt to find a steady-state solution as on p. 66? Distinguish between the
two cases F1=F2and F16=F2. Can you give a physical explanation for your results?

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Math. 401, Sec. 500 Spring, 2005

Homework 7, due March 9

  1. Classify these equations as linear homogeneous, linear nonhomogeneous, or nonlinear. (Here ut ≡ ∂u/∂t, etc.)

(a) utt − uxx = cos(x − t) (b) ut + u^2 ux = 0 (c) ut + 3t^2 u = 0 (d) utt − uxx = −m^2 u

  1. Why do we not make a distinction between “homogeneous” and “nonhomogeneous” for nonlinear equations? Hint: Try to classify the equation y′′^ + (cos y)^2 = 1.
  2. [Schaum’s, p. 46, Ex. 2.52] Find the steady-state temperature in a bar whose ends are located at x = 0 and x = 10, if these ends are kept at 150◦C and 100◦C respectively.
  3. Suppose that the boundary conditions (“BC:”) on p. 64 of the notes (and corresponding lecture on the heat equation with fixed end temperatures) are replaced by

∂u ∂x

(t, 0) = F 1 ,

∂u ∂x

(t, 1) = F 2.

(That is, the heat flux through each end of the bars is held constant.) What happens when you attempt to find a steady-state solution as on p. 66? Distinguish between the two cases F 1 = F 2 and F 1 6 = F 2. Can you give a physical explanation for your results?