M.I.T. Mathematics Homework 6: Integral Equations and Eigenfunctions, Exercises of Calculus

Solutions to selected problems from the mit 18.307: integral equations course, focusing on eigenvalues and eigenfunctions of integral kernels. Topics include finding eigenvalues and eigenfunctions of non-square integrable kernels, symmetric kernels, and integrodifferential operators. Students are expected to understand concepts of integral equations, eigenfunctions, and eigenvalues.

Typology: Exercises

2019/2020

Uploaded on 04/30/2020

amritay
amritay 🇺🇸

4.7

(14)

256 documents

1 / 2

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
18.307: Integral Equations M.I.T. Department of Mathematics
Spring 2006
Homework 6 Due: Wednesday, 04/12/06
ixy u18. (Prob. 4.7 in text by M. Masujima.) Consider the equation u(x) = −� dy e (y), −� <
x < , i.e., with a kernel that is not square integrable. Note that solutions to this equation
are essentially “Fourier transforms of themselves.”
(a) Show that there are only 4 eigenvalues of the kernel eixy . What are they?
(b) Show by an explicit calculation that the functions un(x) = ex2 /2 Hn(x), where Hn(x) =
2
(1)n ex2 dn exare Hermite polynomials, are eigenfunctions with corresponding eigenvalues
dxn
(i)n/2 (n= 0, 1, 2, ...). Hence, the eigenvalues of part (a) are infinitely degenerate, i.e.,
there is a infinite number of independent eigenfunctions for each of them.
(c) Using the result in (b) and the fact that un are known to form a complete set, in some
sense, show that any square integrable solution is of the form u(x) = f(x) + C f
˜(x), where f(x)
is an (arbitrary) odd or even, square integrable function with Fourier transform f
˜(k), and C is
a suitable constant. Evaluate C and relate its value(s) to the eigenvalues found in part (a).
(d) From (c), construct a solution to the original integral equation by taking f(x) = eax2 /2
(Gaussian, a > 0).
19. (Prob. 5.11 in text by M. Masujima.) Consider the kernel K of a 2nd-kind Fredholm equation,
which is given by
K(x, y) = 3, 0 y < x 1,
2, 0 x < y 1.
(a) Find the kernel eigenfunctions un and corresponding eigenvalues n.
(b) Is K symmetric? Determine the transpose kernel KT , and find its eigenfunctions vn with
corresponding eigenvalues n.
(c) Show by an explicit calculation that any un is orthogonal to any vm if m= n.
(d) Derive the spectral representation of K(x, y) in terms of un and vn
20. (Probs. 5.3 & 5.4, Chap. 6 in text by I. Stakgold.) The energy levels E of an atom that expe-
riences non-local interactions with other atoms in a dilute gas are described by the eigenvalue
problem Au = E u, where A is the integrodifferential operator defined by
1
d2u
Au = + dy xy u(y), 0 <x<1,
2
dx 0
and u(x) is any function that has a second derivative continuous for 0 < x < 1 and satisfies
the boundary conditions u(0) = 0 and u(1) = 0. We denote the space of such functions as DA.
Beware: The constant E above multiplies the u outside the integral.
(a) Show that all eigenvalues En of this problem are real and positive, and that eigenfunctions
corresponding to different eigenvalues are orthogonal. Justify your answer. Why is it
sufficient to restrict ourselves to real eigenfunctions?
OVER
pf2

Partial preview of the text

Download M.I.T. Mathematics Homework 6: Integral Equations and Eigenfunctions and more Exercises Calculus in PDF only on Docsity!

18.307: Integral Equations M.I.T. Department of Mathematics

Spring 2006

Homework 6 Due: Wednesday, 04/12/

� (^) −ixy

  1. (Prob. 4.7 in text by M. Masujima.) Consider the equation u(x) = � u −�

dy e (y), −� <

x < �, i.e., with a kernel that is not square integrable. Note that solutions to this equation

are essentially “Fourier transforms of themselves.”

(a) Show that there are only 4 eigenvalues � of the kernel e

−ixy

. What are they?

(b) Show by an explicit calculation that the functions u n

(x) = e

−x

2 / 2 H n

(x), where H n

(x) =

2

n e

x

2 d

n

e

−x are Hermite polynomials, are eigenfunctions with corresponding eigenvalues dx

n

(−i)

n /

2 � (n = 0 , 1 , 2 ,... ). Hence, the eigenvalues of part (a) are infinitely degenerate, i.e.,

there is a infinite number of independent eigenfunctions for each of them.

(c) Using the result in (b) and the fact that u n

are known to form a complete set, in some

sense, show that any square integrable solution is of the form u(x) = f (x) + C f

(x), where f (x)

is an (arbitrary) odd or even, square integrable function with Fourier transform f

(k), and C is

a suitable constant. Evaluate C and relate its value(s) to the eigenvalues found in part (a).

(d) From (c), construct a solution to the original integral equation by taking f (x) = e

−ax

2 / 2

(Gaussian, a > 0).

  1. (Prob. 5.11 in text by M. Masujima.) Consider the kernel K of a 2nd-kind Fredholm equation,

which is given by

K(x, y) =

3 , 0 � y < x � 1 ,

2 , 0 � x < y � 1.

(a) Find the kernel eigenfunctions u n

and corresponding eigenvalues � n

(b) Is K symmetric? Determine the transpose kernel K

T

, and find its eigenfunctions v n

with

corresponding eigenvalues � n

(c) Show by an explicit calculation that any u n

is orthogonal to any v m

if m =≤ n.

(d) Derive the spectral representation of K(x, y) in terms of u n

and v n

  1. (Probs. 5.3 & 5.4, Chap. 6 in text by I. Stakgold.) The energy levels E of an atom that expe

riences non-local interactions with other atoms in a dilute gas are described by the eigenvalue

problem Au = E u, where A is the integrodifferential operator defined by

� 1 d

2 u

Au = + dy xy u(y), 0 < x < 1 ,

2

dx (^0)

and u(x) is any function that has a second derivative continuous for 0 < x < 1 and satisfies

the boundary conditions u(0) = 0 and u

(1) = 0. We denote the space of such functions as D A

Beware: The constant E above multiplies the u outside the integral.

(a) Show that all eigenvalues E n

of this problem are real and positive, and that eigenfunctions

corresponding to different eigenvalues are orthogonal. Justify your answer. Why is it

sufficient to restrict ourselves to real eigenfunctions?

OVER

(b) By using Green’s function, show that the given problem can be reduced

to a homogeneous integral equation (with no derivatives) involving a sym

metric kernel K(x, y), i.e., one needs to find the eigenvalues of a (pure)

integral operator. Hint: Define G(x, x ) such that −G

xx

= �(x − x ) by

considering as ‘source’ �(x ) = Eu(x ) − x

0

1

dy yu. What are the condi

tions on G? After you find G, calculate any undetermined constant in �

for consistency.

(c) [Without using (b) above] By noticing that the given problem Au = E u is

of the form u + Eu = bu, show that the eigenvalues E = μ

2

are obtained

as positive roots of the equation

3

5

tan μ = μ +

5

(d) Sketch the functions tan μ and μ + μ

3

/ 3 − μ. Find an approximate value

for the lowest eigenvalue, E

0

, according to (c) above.

(e) According to a variational principle for the lowest eigenvalue E

0

1

dx [v (x)]

2

1

dx xv(x)

� 2

0

E

0

= min

0

v�D A

1

dx v(x)

2

0

Can you explain this equation? Use the trial function v(x) = x(c − x) to

find an upper bound for E

0

. What is c? Use the “trace inequality” for the

iterated kernel K

2

of the kernel K of part (b) to find a lower bound to E

0

Compare your answer with the answer obtained in part (d).