Real Analysis 599Returning to the problem, we see that there existsc∈[ 0 ,x]such that
∫x0e−ty′y′′dt=∫c0y′y′′dt=1
2
[
((y′(c))^2 −(y′( 0 ))^2]
.
In conclusion,(y(x))^2 +(y′(c))^2 =(y( 0 ))^2 +(y′( 0 ))^2 , forx> 0 ,showing thatyis bounded asx→∞.
Second solution: Use an integrating factor as in the previous solution to obtainy^2 (x)−y^2 ( 0 )+ 2∫x0e−ty′y′′dt= 0.Then integrate by parts to obtainy^2 (x)+e−x(y′(x))^2 +∫x0e−t(y′(t))^2 dt=y^2 ( 0 )+(y′( 0 ))^2.Because every term on the left is nonnegative, it follows immediately that|y(x)|≤(
y^2 ( 0 )+(y′( 0 ))^2) 1 / 2
is bounded, and we are done.
(27th W.L. Putnam Mathematical Competition, 1966)
567.We havey 1 ′′(t)+y 1 (t)=∫∞
0t^2 e−tx
1 +t^2
dt+∫∞
0e−tx
1 +t^2
dt=∫∞
0e−txdt=1
x.
Also, integrating by parts, we obtain
y 2 (x)=−cost
t+x∣∣
∣∣
∞0−
∫∞
0cost
(t+x)^2
dt=1
x−
sint
(t+x)^2∣∣
∣∣
∞0−
∫∞
02 sint
(t+x)^3
dt=
1
x−y 2 ′′(x).Since the functionsy 1 andy 2 satisfy the same inhomogeneous equation, their difference
y 1 −y 2 satisfies the homogeneous equationy′′+y = 0, and hence is of the form
Acosx+Bsinx. On the other hand,lim
x→∞
(y 1 (x)−y 2 (x))=lim
x→∞
y 1 (x)−lim
x→∞
y 2 (x)= 0 ,