0387986995Basic TheoryC
.pdf148 VI. BOUNDARY-VALUE PROBLEMS
where b = t. Note that t = 0 is a regular singular point of (VI.1.8) and the indicial equation is 4s2 + 2s + A = 0 whose roots are s = - 2 f 4 - A. These roots are real if and only if A < 4 This verifies the claim. 0
Note that J |
+00 |
dx |
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1 + x2 |
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0 |
2* |
The following theorem shows some structure of solutions in the case when
+00
ig(x)ldx < +oo.
0
Theorem VI-1-8. Let g(x) be a real-valued and continuous function on the inter-
f+C0
valA. If 1 jg(x)ldx < +oo, then there exist unbounded solutions of differential
0
equation (VI. 1. 1) on Ia.
Proof.
The assumption of this theorem and (VI.1.1) imply that |
lim dq(x) |
= -Y exists |
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:-+oo dx |
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for any bounded solution n(x) of (VI.1.1). If 7 0, then i(x) is unbounded. Hence,
lim odd) = 0. Therefore, calculating the Wronskian of two bounded solutions
z
of (VI.1.1), we find that those bounded solutions are linearly dependent on each other. This implies that there must be unbounded solutions. 0
Remark VI-1-9. Theorems VI-1-1 and VI-1-2 are also explained in ]CL, §1 of
Chapter 8, pp. 208-211] and [Hart, Chapter XI, pp. 322-403]. For details concern- ing other results in this section, see also [Cop2, Chapter 1, pp. 4-33] and [Be12,
Chapter 6, pp. 107-142].
VI-2. Sturm-Liouville problems
A Sturm-Liouville problem is a boundary-value problem
dd-x (p(x) Ly) + u(x)y = f (.T),
(BP) |
y(a) cos a |
-Ip(a)y'(a)sin or = 0, |
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y(b) cos Q - P(b)y(b) sin )3 = 0,
under the assumptions:
(i)the quantities a, b, a, and $ are real numbers such that a < b,
(ii)two functions u(x) and f (x) are real-valued and continuous on the interval
Z(a,b) = {x: a < x < b},
(iii)the function p(x) is real-valued and continuously differentiable, and p(x) > 0
on 1(a, b).
In this section, we explain some basic results concerning problem (BP).
2. STRUM-LIOUVILLE PROBLEMS |
149 |
Let 4(x) and O(z) be two solutions of the homogeneous linear differential equation
(VI-2.1) |
(p(x)A) + u()y = 0 |
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-dx |
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such that |
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(VI.2.2) |
m(a) = sins, p(a)d'(a) = cosa, |
,p(b) = sin f3, p(b)t'(b) = cosfi, |
respectively. Then, these two solutions satisfy the boundary conditions |
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(VI.2.3) |
¢(a) cos a - p(a)4,'(a) sin a = 0, |
i (b) cos /3 - p(b)0'(b) sin /3 = 0. |
The two solutions 4(x) and /;(x) are linearly independent if and only if |
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(VI.2.4) |
4(b) cos Q - p(b)©'(b) sin /3 # 0 or |
'(a) cos a - p(a)rb'(a) sin a # 0. |
The first basic result of this section is the following theorem, which concerns the existence and uniqueness of solution of (BP).
Theorem VI-2-1. If the two solutions 4(x) and ip(x) of (VI.2.1) are linearly independent, then problem (BP) has one and only one solutwn on the interval
I(a, b).
Proof
Using the method of variation of parameters (cf. Remark IV-7-2), write the general solution y(x) of the differential equation of (BP) and its derivative y'(x)
respectively in the following form:
(VI.2.5)
6 |
'j'(_)f (_) |
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VW = CIOW + C20 W + 4(x) J P(f)WW |
4 + |
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Y' (X) = Clo'(x) + C21k'(x) + 0'(x) I |
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4 |
s |
P(A)W |
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i,&(x)1= o(f)f
a
(x) J |
A, |
JJJu P(A)W V) |
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where cl and c2 are arbitrary constants and W (x) denotes the Wronskian of
Now, using (VI.2.3) and (VI.2.4), it can be shown that solution
(VI.2.5) satisfies the boundary conditions of (BP) if and only if cl = 0 and c2 =
0. 0
Observation VI-2-2. It can be shown easily that p(x)W(x) is independent of x.
Observation VI-2-3. Under the assumption that the two solutions 40(x) and tfi(x) of (VI.2.1) are linearly independent, the unique solution of (BP) is given by
rb
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y(x) = d(x) |
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10(x) I (- ))- W(f ) |
(VI.2.6) |
Jx P(A)W (O |
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i |
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Y 'W = O(x) |
rb owfwdC + V,'(x) r= 4(W W 4. |
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1r |
W |
Ja P(OW (O |
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150 VI. BOUNDARY-VALUE PROBLEMS
Setting
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4(x)1() |
if |
x |
< C <b, |
(VI.2.7) |
G(x, ) = |
p(OW (c) |
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O WOW |
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a |
< t < x, |
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if |
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p(f)W(c) |
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we can write (VI.2.6) in the form |
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b |
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J |
b aG |
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y(x) = J G(x, )f |
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8x (x, Of (Ode. |
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y '(x) = |
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The function G(x,l;) is called Green's function of problem (BP). The following theorem gives the characterization of Green's function.
Theorem VI-2-4. The function G(x, C) given by (VI. 2.7) satisfies the following conditions:
(i) G(x, l:) is continuous with respect to (x, e) on the region D = {(x,) a < x < b, a< £<b},
(ii) 8 (x, l:) is continuous with respect to (x, C) on the region D - |
a < |
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C < b}, |
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(iii) at ({, l;), we have |
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8 (tr + 0. 0 - |
for a < < b, |
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( - 0, 0 = p(0 |
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(iv)as a function of x, G(x, l:) satisfies homogeneous linear differential equation
(VI. 2. 1) if x 0 4,
(v)as a function of x, G(x, 4) satisfies the boundary conditions of (BP), i. e.,
G(b,Z:)cosf3-p(b)8G(b,{)sinf3=0
for a:5 < b.
Furthermore, the function G(x, f) is uniquely determined by these five conditions.
Proof.
It is evident that the function G(x, l;) satisfies these five conditions. Suppose H(x,t) satisfies the five conditions. Conditions (iv) and (v) imply that
Cl(l;)4(x) for
{ C2(t;)V(x) |
for |
a < x < l;,
{ < x < b
for (x,l;') E D, where Ci(1;) and C2(C) must be determined by conditions (i), (ii),
and (iii). This means that C,({) and |
must be determined by |
0 and
-PW
2. STRUM-LIOUVILLE PROBLEMS |
151 |
OW |
4(f) |
Since {(x,e) : a < x < } |
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This yields Cl(a;) = p(OW(O and C2({) = |
p(OW(O |
- |
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x<t<b}and {(x,t): 1;<x< b}{(x,£): a<t<x}for
(x, ) E V, we obtain H(x,1;) = G(x, l;). 0
The second basic result co//ncerns self-adjointness of problem (BP). Define a dif-
ferential operator L[y] _ |
(p(x) |
I + u(z)y and a vector space V(a, b) over the |
real number field 1R by |
\ |
/ |
V(a, b) _ { f r C2(a, b) : f (a) cos a - p(a) f'(a)sin a = 0, f(b)cos5 - p(b)f'(b) sin,3 = 01,
where C2(a, b) denotes the set of all real-valued functions which are twice contin- uously differentiable on the interval I(a, b) = {x : a < x < b). Define also an inner product (f, g) for two real-valued continuous functions f and g on I(a, b) by
(f,9) = f |
Since |
a |
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(()) |
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(f, 4191) = |
J6f() [ |
+ |
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= p(b)f (b)9 (b) - p(a)f (a)9'(a) + fb |
dl; |
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a |
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for f E V(a, b) and g E V(a, b), we obtain
(f,L[g) - (L(f1,9)
={p(b)f(b)9'(b) - p(b)g(b)f'(b)} - {p(a)f(a)9 (a) - p(a)9(a)f'(a)}.
Also, since
( |
f (a) cos a - p(a)f'(a) sin a = 0, |
f (b) cos Q - p(b) f'(b) sin O= 0, |
t |
9(a) cos a - p(a)9'(a) sin a = 0, |
g(b) cos, - p(6)9'(b) sin /3 = 0 |
for f E V(a. b) and g E V(a, b), we obtain |
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p(a)f(a)9'(a) - p(a)g(a)f(a) = 0, |
p(b)f(b)9'(b) - p(b)g(b)f(b) = 0. |
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Thus, we proved the following theorem.
Theorem VI-2-5 (self-adjointness). The operator L has the following property:
(f, 0191) = (L(f], 9) |
for |
f E V (a, b) and g E V(a, b). |
154 |
VI. BOUNDARY-VALUE PROBLEMS |
Observation VI-3-2. All roots of (VI.3.5) are simple, since, if A is a root of
(VI.3.5), we can prove
80(b, A) |
cos j3 - P(b) |
8¢'(b, A)sun f # 0 |
8A |
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8A |
in the following way. Let A be a root of (VI.3.5). Then, notice that z = 84(x, A)
8A
is a solution of the differential equation
CP(x)L1 + u(x)z = Az + ¢(x,A).
This implies that
(VI.3.6) |
r_ |
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Z(X) = c16(x, A) + c2p(x) - O(x, A) |
A) dC + p(x) f = |
' , A)2 de, |
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Ja P(O1't'(O |
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1 n |
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z'(x) = clOx, A) + C21L (x) - 4'(x, A) f pW¢(f, A)dC + |
p '(x) j |
= w(), A)2 |
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PwW (f) |
P(O-N) dd, |
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where p(x) is a solution of homogeneous linear differential equation (VI.3.1) such that 4(x, A) and p(x) are linearly independent, two quantities ct and c2 are constants, and W(x) denotes the Wronskian of {¢(x,A),p(x)}. Note that p(x)W(x) is independent of x and that
(VI.3.7) p(a) cos a - p(a)p'(a) sin a 0, p(b) cos,3 - p(b)1 (b) sin Q # 0.
Formulas (VI.3.6) imply that
(VI.3.8)
z(a) = clo(a,A) + c2p(a), z'(a) = ci4'(a,A) + c2,u (a),
z(b) = cj¢(b, A) + c2p(b) - 4(b, A) |
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fb |
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p(b) |
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Jn |
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Pwww |
z'(b) = c1 ¢'(b, A) + c2p'(b) - 0'(b.,\) j |
w |
+ p'(b)rP(u)W |
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o P(4)W (0 |
Since (VI.3.3) is true for all values of A, it follows that z(a) cos a - p(a)z(a) sin a
0. Hence, from (VI.3.7) and (VI.3.8), we conclude that c2 = 0. Therefore,
z(b) cos |
cos$ |
- P(b) |
(b) sin 0) ° 0(Td |
# 0. |
0 |
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- P(b) z'(b) sin,3 = (,u(b) |
Ia a P(A)W w |
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Remark VI-3-3. If A = 0 is not an eigenvalue of (EP), we can define Green's function G(x,t) of problem (BP of §V-2 so that (EP) is changed equivalently to
the integral equation y(x) = A |
G(x, |
To prove that all eigenvalues of (EP) are real, it is convenient to extend Theorem VI-2-5 (self-adjointness) to complex-valued functions f and g. Define a differential
156 |
VI. BOUNDARY-VALUE PROBLEMS |
Theorem VI-3-5. All eigenvalues of (EP) are meal.
Proof.
Let A be an eigenvalue of (EP) and let y(x) be an eigenfunction corresponding to A. We may assume that (y, y) = 1. Then,
(y,Cjy]) = (y, Ay) = X(y,y) = X,
(hjyl,y) = (Ay,y) = A(yy) = A,
and Theorem VI-3-4 imply that J = A. 0
In order to explain distribution of eigenvalues on the real line IR, look at the basic comparison theorem (Theorem VI-1-1) more closely. Let us rewrite the differential equation
(VI.3.9) |
(P(X) dy) + g(x)y = 0 |
in the form
p(x) = (1 - p(x)g(x))rsin(O)cos(9)
and
(VI.3.10) p(x)dO = I + (p(x)g(x) - 1) sin2(a)
by setting
y = r sin(O), p(x) Li = r cos(B).
The right-hand side of (VI.3.10) is independent of r. Therefore, (VI.3.10) is a first- order nonlinear differential equation on 0. Our main concern is the behavior of solutions of (VI.3.10).
Remark VI-3-6. Set w = ! ((x) L) . Then, differential equation (VI.3.9) be-
comes p(x) dx + w2 + p(x)g(x) = 0. This equation is further changed to (VI.3.10)
by the transformation w = cot(8).
Remark VI-3-7. If the function g(x) is continuous on the interval 2(a, b), then every solution 0(x) of (VI.3.10) exists on T(a,b).
Now, we prove the following basic lemma.
Lemma VI-3-8. Assume that
(1) four functions gl(x), g2(x), pi (x), and p2(x) are continuous on the interval
2(a, b),
(2) 92(x) ? gi(x) and pi(x) ? P2(x) > 0 on T(a,b),
(3) 01(x) (j = 1,2) are solutions of the differential equations
Pi (x) ! |
= 1 + [pi (x)gg (x) - 1J sin2(01) |
(j = 1, 2), |
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