Elementary Real Analysis - Test 1 Problems | MATH 444, Exams of Mathematical Methods for Numerical Analysis and Optimization

Material Type: Exam; Class: Elementary Real Analysis; Subject: Mathematics; University: University of Illinois - Urbana-Champaign; Term: Spring 2001;

Typology: Exams

Pre 2010

Uploaded on 03/11/2009

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Math 444 Spring 2001 Test
Total points: 100. Do all questions.
Instructions: Show ALL your working and make your explanations as full as possible,
unless the question says otherwise. Calculators are not allowed on this exam; neither
are books or notes.
If you apply a theorem from class, you need not state the theorem but you must
demonstrate that its hypotheses are satisfied.
Green’s Formulas:
Z
[vu+v· u]dx =Z
v∂u
∂ν dS
Z
[vuuv]dx =Z·v∂u
∂ν uv
∂ν ¸dS
1: (25 points) Assume Gis a smooth function and u(x, y) is a weak solution of the
conservation law
G(u)x+uy= 0.
(a) Show that if uis in fact a smooth solution except for a jump across the C1-curve
x=ξ(y), then the direction of the curve is related to the jump by
ξ0(y) = G(u`)G(ur)
u`ur
.
(b) State the entropy condition, say what it means physically, and illustrate with a
diagram. (If you like, you can assume in part (b) that G(z) = 1
2z2,i.e. Burgers’
equation.)
2: (25 points) Let f(x, t) be smooth.
(a) State Duhamel’s Principle for solving the nonhomogeneous wave equation ztt
c2z=fin Rn(with zero initial conditions) in terms of the solutions to certain
homogeneous problems. (You are not required to solve these homogeneous problems.)
(b) Prove Duhamel’s Principle. That is, show that your formula for z(x, t) really
does solve ztt c2z=f.
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Math 444 — Spring 2001 — Test

Total points: 100. Do all questions.

Instructions: Show ALL your working and make your explanations as full as possible, unless the question says otherwise. Calculators are not allowed on this exam; neither are books or notes. If you apply a theorem from class, you need not state the theorem but you must demonstrate that its hypotheses are satisfied.

Green’s Formulas: ∫

Ω

[v∆u + ∇v · ∇u] dx =

∂Ω

v ∂u ∂ν dS ∫

Ω

[v∆u − u∆v] dx =

∂Ω

[

v ∂u ∂ν

− u ∂v ∂ν

]

dS

1: (25 points) Assume G is a smooth function and u(x, y) is a weak solution of the conservation law G(u)x + uy = 0. (a) Show that if u is in fact a smooth solution except for a jump across the C^1 -curve x = ξ(y), then the direction of the curve is related to the jump by

ξ′(y) = G(u) − G(ur) u − ur

(b) State the entropy condition, say what it means physically, and illustrate with a diagram. (If you like, you can assume in part (b) that G(z) = 12 z^2 , i.e. Burgers’ equation.)

2: (25 points) Let f (x, t) be smooth. (a) State Duhamel’s Principle for solving the nonhomogeneous wave equation ztt − c^2 ∆z = f in Rn^ (with zero initial conditions) in terms of the solutions to certain homogeneous problems. (You are not required to solve these homogeneous problems.) (b) Prove Duhamel’s Principle. That is, show that your formula for z(x, t) really does solve ztt − c^2 ∆z = f.

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3: (25 points) For x ∈ R^2 , let

u(x) =

|x|^2 − 1 if |x| ≤ 1, ln(|x|^2 ) if |x| > 1, f^ (x) =

4 if |x| ≤ 1, 0 if |x| > 1. Show ∆u = f weakly in R^2. (Note: here x = (x 1 , x 2 ) and |x| =

x^21 + x^22 .)

4: (25 points) Consider the nonhomogeneous wave equation utt − c^2 ∆u = f. Write

E(t) =

u^2 t + c^2 |∇u|^2

dx.

(Here the integral is over Rn. We assume u and f are smooth and have compact support, at each t). (a) Show E′(t) =

utf dx. (b) Explain why this formula is physically plausible. [For part (b) you can work in one dimension, so that f represents an external force on the string.]

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