University of British Columbia Mathematics 401 Examination - April 2008, Exams of Mathematics

A past examination from the university of british columbia's mathematics 401 course, held in april 2008. The examination covers various topics in mathematical analysis, including partial differential equations, green's functions, and variational principles. Five problems that require the application of these concepts to solve for functions u(x,y) and φ(x,y) in different regions, as well as finding eigenvalues and eigenfunctions. Students are expected to use analytical methods to find solutions and represent functions in terms of green's functions or other appropriate functions.

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2012/2013

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The University of British Columbia
Final Examinations - April 2008
Mathematics 401
M. Ward
Closed book examination Time: 2 1
2hours
Special Instructions: A two-sided single page of notes is allowed.
Marks
[20] 1. Consider the following problem for u(x, y ) in a square:
uxx +uyy + 4u=f(x, y) in 0 xπ , 0yπ ,
ux(0, y) = ux(π , y) = 0 , u(x, 0) = u(x, π) = 0 .
(i) Is there a condition on f(x, y) that is required in order for there to be a solution
to this problem? If so, find this condition.
(ii) Show how to represent u(x, y) in terms of either a Green’s function or a modified
Green’s function, which ever is appropriate. (You do not need to calculate this
Green’s function analytically).
[20] 2. Consider the following problem for u(x, y ) in the unit disk:
uxx +uyy u=f(x, y) in x2+y21 ; u=h(x, y) on x2+y2= 1 .
(i) Show how to represent uin terms of an appropriate Green’s function G. Is there
a simple analytical formula for Gby the method of images?
(ii) In terms of the usual modified Bessel functions, derive the following identity:
K0(R) =
X
n=−∞
ein(φθ)In(r<)Kn(r>),
where r<= min(r, ρ), r>= max(r, ρ), and R=pr2+ρ22 cos(θφ).
(Hint: you will need the Wronskian relation I0
n(x)Kn(x)In(x)K0
n(x) = 1/x.
(iii) By using the identity in (ii), give an infinite series representation for the Green’s
function that is required in part (i).
Continued on page 2
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The University of British Columbia Final Examinations - April 2008

Mathematics 401

M. Ward

Closed book examination Time: 2 12 hours

Special Instructions: A two-sided single page of notes is allowed.

Marks

[20] 1. Consider the following problem for u(x, y) in a square: uxx + uyy + 4u = f (x, y) in 0 ≤ x ≤ π , 0 ≤ y ≤ π , ux(0, y) = ux(π, y) = 0 , u(x, 0) = u(x, π) = 0.

(i) Is there a condition on f (x, y) that is required in order for there to be a solution to this problem? If so, find this condition. (ii) Show how to represent u(x, y) in terms of either a Green’s function or a modified Green’s function, which ever is appropriate. (You do not need to calculate this Green’s function analytically).

[20] 2. Consider the following problem for u(x, y) in the unit disk: uxx + uyy − u = f (x, y) in x^2 + y^2 ≤ 1 ; u = h(x, y) on x^2 + y^2 = 1.

(i) Show how to represent u in terms of an appropriate Green’s function G. Is there a simple analytical formula for G by the method of images? (ii) In terms of the usual modified Bessel functions, derive the following identity:

K 0 (R) =

∑^ ∞

n=−∞

ein(φ−θ)In(r<)Kn(r>) ,

where r< = min(r, ρ), r> = max(r, ρ), and R =

r^2 + ρ^2 − 2 rρ cos(θ − φ). (Hint: you will need the Wronskian relation I n′(x)Kn(x) − In(x)K

′ n(x) = 1/x. (iii) By using the identity in (ii), give an infinite series representation for the Green’s function that is required in part (i).

Continued on page 2

April 2008 Mathematics 401 Page 2 of 3 pages

[20] 3. Let u = u(x) and consider the functional

I(u) =

∫ L

0

F (x, u, u

′ , u

′′ ) dx ,

over all four times continuously differentiable functions, u(x), satisfying the boundary conditions u(0) = u(L) = 0.

(i) Show that the Euler-Lagrange equation associated with I(u) is

∂F ∂u

d dx

∂F

∂u′

d^2 dx^2

∂F

∂u′′

What are the natural boundary conditions for u at x = 0, L?

(ii) Suppose that F (x, u, u′, u′′) =

[u′′] 2

[u′] 2 −

σ (1 + u)

where σ is a positive constant. Write the associated Euler-Lagrange equation and boundary conditions for u explicitly. (This problem models the deflection of a beam in a micro-electrical-mechanical system). (ii) Next, consider the eigenvalue problem

(p(x)u′′) ′′ = λu , 0 ≤ x ≤ L; u(0) = u(L) = u′(0) = u′(L) = 0 ,

with p(x) > 0 in 0 ≤ x ≤ L. Find a variational principle, together with a simple trial function, that can be used to give an upper bound on the first eigenvalue λ 1 (Do not calculate this bound analytically).

Continued on page 3