5.4 Exercises
These are homework exercises to accompany Libl's "Differential Equations for Engineering " Textmap. This is a textbook targeted for a one semester first course on differential equations, aimed at engineering students. Prerequisite for the course is the basic calculus sequence.
Your Turn
Find eigenvalues and eigenfunctions of
y
″
+
λ
y
=
0
,
y
(
0
)
−
y
′
(
0
)
=
0
,
y
(
1
)
=
0
.
Your Turn
Expand the function f ( x ) = x on 0 ≤ x ≤ 1 using the eigenfunctions of the system
y
″
+
λ
y
=
0
,
y
′
(
0
)
=
0
,
y
(
1
)
=
0
.
Your Turn
Suppose that you had a Sturm-Liouville problem on the interval [ 0 , 1 ] and came up with y n ( x ) = sin ( γ n x ) , where γ > 0 is some constant. Decompose f ( x ) = x , 0 < x < 1 , in terms of these eigenfunctions.
Your Turn
Find eigenvalues and eigenfunctions of
y
′
(
4
)
+
λ
y
=
0
,
y
(
0
)
=
0
,
y
′
(
0
)
=
0
,
y
(
1
)
=
0
y
′
(
1
)
=
0
.
This problem is not a Sturm-Liouville problem, but the idea is the same.
Your Turn
(more challenging)
Find eigenvalues and eigenfunctions for
d
d
x
(
e
x
y
′
)
+
λ
e
x
y
=
0
,
y
(
0
)
=
0
,
y
(
1
)
=
0
.
Hint: First write the system as a constant coefficient system to find general solutions. Do note that Theorem 5.1.1 guarantees λ ≥ 0 .
Your Turn
Find eigenvalues and eigenfunctions of
y
″
+
λ
y
=
0
,
y
(
−
1
)
=
0
,
y
(
1
)
=
0
.
Answer
λ n = ( 2 n − 1 ) π 2 , n = 1 , 2 , 3 , ⋯ , y n = cos ( ( 2 n − 1 ) π 2 x )
Your Turn
Put the following problems into the standard form for Sturm-Liouville problems, that is, find p ( x ) , q ( x ) , r ( x ) , α 1 , α , β 1 , β 1 , , and decide if the problems are regular or not.
x y ″ + λ y = 0 for 0 < x < 1 , y ( 0 ) = 0 , y ( 1 ) = 0 , ( 1 + x 2 ) y ″ + 2 x y ′ + ( λ − x 2 ) y = 0 for − 1 < x < 1 , y ( − 1 ) = 0 , y ( 1 ) + y ′ ( 1 ) = 0
Answer
p ( x ) = 1 , q ( x ) = 0 , r ( x ) = 1 x , α 1 = 1 , α 2 = 0 , β 1 = 1 , β 2 = 0 . The problem is not regular.p ( x ) = 1 + x 2 , q ( x ) = x 2 , r ( x ) = 1 , α 1 = 1 , α 2 = 0 , β 1 = 1 , β 2 = 1 . The problem is regular.
Your Turn
Suppose you have a beam of length 5 with free ends. Let y be the transverse deviation of the beam at position x on the beam ( 0 < x < 5 ) . You know that the constants are such that this satisfies the equation y t t + 4 y x x x x = 0 . Suppose you know that the initial shape of the beam is the graph of x ( 5 − x ) , and the initial velocity is uniformly equal to 2 (same for each x ) in the positive y direction. Set up the equation together with the boundary and initial conditions. Just set up, do not solve.
Your Turn
Suppose you have a beam of length 5 with one end free and one end fixed (the fixed end is at x = 5 ). Let u be the longitudinal deviation of the beam at position x on the beam ( 0 < x < 5 ) . You know that the constants are such that this satisfies the equation u t t = 4 u x x . Suppose you know that the initial displacement of the beam is x − 5 50 , and the initial velocity is − ( x − 5 ) 100 in the positive u direction. Set up the equation together with the boundary and initial conditions. Just set up, do not solve.
Your Turn
Suppose the beam is L units long, everything else kept the same as in (5.2.2). What is the equation and the series solution?
Your Turn
Suppose you have
a
4
y
x
x
x
x
+
y
t
t
=
0
(
0
<
x
<
1
,
t
>
0
)
,
y
(
0
,
t
)
=
y
x
x
(
0
,
t
)
=
0
,
y
(
1
,
t
)
=
y
x
x
(
1
,
t
)
=
0
,
y
(
x
,
0
)
=
f
(
x
)
,
y
t
(
x
,
0
)
=
g
(
x
)
.
That is, you have also an initial velocity. Find a series solution. Hint: Use the same idea as we did for the wave equation.
Your Turn
Suppose you have a beam of length 1 with hinged ends. Let y be the transverse deviation of the beam at position x on the beam (0 < x < 1 ). You know that the constants are such that this satisfies the equation y t t + 4 y x x x x = 0 . Suppose you know that the initial shape of the beam is the graph of sin ( π x ) , and the initial velocity is 0 . Solve for y .
Answer
y
(
x
,
t
)
=
sin
(
π
x
)
cos
(
2
π
2
t
)
Your Turn
Suppose you have a beam of length 10 with two fixed ends. Let y be the transverse deviation of the beam at position x on the beam (0 < x < 10 ). You know that the constants are such that this satisfies the equation y t t + 9 y x x x x = 0 . Suppose you know that the initial shape of the beam is the graph of sin ( π x ) , and the initial velocity is uniformly equal to x ( 10 − x ) . Set up the equation together with the boundary and initial conditions. Just set up, do not solve.
Answer
9 y x x x x + y t t = 0 ( 0 < x < 10 , t > 0 ) , y ( 0 , t ) = y x ( 0 , t ) = 0 , y ( 10 , t ) = y x ( 10 , t ) = 0 , y ( x , 0 ) = sin ( π x ) , y t ( x , 0 ) = x ( 10 − x ) .
Your Turn
Suppose that the forcing function for the vibrating string is F 0 sin ( ω t ) . Derive the particular solution y p .
Your Turn
Take the forced vibrating string. Suppose that L = 1 , a = 1 . Suppose that the forcing function is the square wave that is 1 on the interval 0 < x < 1 and − 1 on the interval − 1 < x < 0 . Find the particular solution. Hint: You may want to use result of Exercise 5.3 .1 .
Your Turn
The units are cgs (centimeters-grams-seconds). For k = 0.005 , ω = 1.991 × 10 − 7 , A 0 = 20 . Find the depth at which the temperature variation is half (± 10 degrees) of what it is on the surface.
Your Turn
Take the forced vibrating string. Suppose that L = 1 , a = 1 . Suppose that the forcing function is a sawtooth, that is | x | − 1 2 on − 1 < x < 1 extended periodically. Find the particular solution.
Answer
y
p
(
x
,
t
)
=
∑
n
odd
n
=
1
∞
−
4
n
4
π
4
(
cos
(
n
π
x
)
−
cos
(
n
π
)
−
1
sin
(
n
π
)
sin
(
n
π
x
)
−
1
)
cos
(
n
π
t
)
.
Your Turn
The units are cgs (centimeters-grams-seconds). For k = 0.01 , ω = 1.991 × 10 − 7 , A 0 = 25 . Find the depth at which the summer is again the hottest point.
Answer
Approximately 1991 centimeters
Adapted from Differential Equations for Engineers by Jiří Lebl (Oklahoma State University), hosted on LibreTexts (math.libretexts.org) and licensed under CC BY-SA 4.0. Changes were made. License: CC-BY-SA-4.0 .