6.6 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 the Laplace transform of a + b t + c t 2 for some constants a , b , and c .
Your Turn
Find the Laplace transform of t i f t ≥ 1 , 0 i f t < 1 . .
Your Turn
Find the inverse Laplace transform of 8 s 3 ( s + 2 ) .
Answer
2
t
2
−
2
t
+
1
−
e
−
2
t
Your Turn
Verify Table 6.2.1.
Your Turn
Using the Heaviside function write down the piecewise function that is 0 for t < 0 , t 2 for t in [ 0 , 1 ] and t for t > 1 .
Your Turn
Using the Laplace transform solve
m
x
″
+
c
x
′
+
k
x
=
0
,
x
(
0
)
=
a
,
x
′
(
0
)
=
b
.
where m > 0 , c > 0 , k > 0 , and c 2 − 4 k m > 0 (system is overdamped).
Your Turn
Using the Laplace transform solve
m
x
″
+
c
x
′
+
k
x
=
0
,
x
(
0
)
=
a
,
x
′
(
0
)
=
b
.
where m > 0 , c > 0 , k > 0 , and c 2 − 4 k m < 0 (system is underdamped).
Your Turn
Using the Laplace transform solve
m
x
″
+
c
x
′
+
k
x
=
0
,
x
(
0
)
=
a
,
x
′
(
0
)
=
b
.
where m > 0 , c > 0 , k > 0 , and c 2 = 4 k m (system is critically damped).
Your Turn
Show the differentiation of the transform property. Suppose ℒ { f ( t ) } = F ( s ) , then show
ℒ
{
−
t
f
(
t
)
}
=
F
′
(
s
)
.
Hint: Differentiate under the integral sign.
Your Turn
Solve x ‴ + x = t 3 u ( t − 1 ) for initial conditions x ( 0 ) = 1 and x ′ ( 0 ) = 0 , x ″ ( 0 ) = 0 .
Your Turn
Let us think of the mass-spring system with a rocket from Example 6.2.2. We noticed that the solution kept oscillating after the rocket stopped running. The amplitude of the oscillation depends on the time that the rocket was fired (for 4 seconds in the example).
Find a formula for the amplitude of the resulting oscillation in terms of the amount of time the rocket is fired. Is there a nonzero time (if so what is it?) for which the rocket fires and the resulting oscillation has amplitude 0 (the mass is not moving)?
Your Turn
Define
(
t
−
1
)
2
i
f
1
≤
t
<
2
,
3
−
t
i
f
2
≤
t
<
3
,
0
o
t
h
e
r
w
i
s
e
.
Sketch the graph of f ( t ) . Write down f ( t ) using the Heaviside function. Solve x ″ + x = f ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 using Laplace transform.
Your Turn
Using the Heaviside function u ( t ) , write down the function
0
i
f
t
<
1
,
t
−
1
i
f
1
≤
t
<
2
,
i
f
2
≤
t
.
Answer
f
(
t
)
=
(
t
−
1
)
(
u
(
t
−
1
)
−
u
(
t
−
2
)
)
+
u
(
t
−
2
)
Your Turn
Solve x ″ − x = ( t 2 − 1 ) u ( t − 1 ) for initial conditions x ( 0 ) = 1 , x ′ ( 0 ) = 2 using the Laplace transform.
Answer
x
(
t
)
=
(
2
e
t
−
1
−
t
2
−
1
)
u
(
t
−
1
)
−
1
2
e
−
t
+
3
2
e
t
Your Turn
Let f ( t ) = t 2 for t ≥ 0 , and g ( t ) = u ( t − 1 ) . Compute f * g .
Your Turn
Let f ( t ) = t for t ≥ 0 , and g ( t ) = sin t for t ≥ 0 . Compute f * g .
Your Turn
Find the solution to
m
x
″
+
c
x
′
+
k
x
=
f
(
t
)
,
x
(
0
)
=
0
,
x
′
(
0
)
=
0
,
for an arbitrary function f ( t ) , where m > 0 , c > 0 , k > 0 , and c 2 − 4 k m > 0 (system is overdamped). Write the solution as a definite integral.
Your Turn
Find the solution to
m
x
″
+
c
x
′
+
k
x
=
f
(
t
)
,
x
(
0
)
=
0
,
x
′
(
0
)
=
0
,
for an arbitrary function f ( t ) , where m > 0 , c > 0 , k > 0 , and c 2 − 4 k m < 0 (system is underdamped). Write the solution as a definite integral.
Your Turn
Find the solution to
m
x
″
+
c
x
′
+
k
x
=
f
(
t
)
,
x
(
0
)
=
0
,
x
′
(
0
)
=
0
,
for an arbitrary function f ( t ) , where m > 0 , c > 0 , k > 0 , and c 2 = 4 k m (system is critically damped). Write the solution as a definite integral.
Your Turn
Write down the solution to x ″ − 2 x = e − t 2 , x ( 0 ) = 0 , x ′ ( 0 ) = 0 as a definite integral. Hint: Do not try to compute the Laplace transform of e − t 2 .
Your Turn
Let f ( t ) = cos t for t ≥ 0 , and g ( t ) = e − t . Compute f * g .
Answer
1
2
(
cos
t
+
sin
t
−
e
−
t
)
Your Turn
Solve x ″ + x = sin t , x ( 0 ) = 0 , x ′ ( 0 ) = 0 using convolution.
Answer
1
2
(
sin
t
−
t
cos
t
)
Your Turn
Solve x ‴ + x ′ = f ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 , x ″ ( 0 ) = 0 using convolution. Write the result as a definite integral.
Answer
∫
0
t
f
(
τ
)
(
1
−
cos
(
t
−
τ
)
)
d
τ
Your Turn
Solve (find the impulse response) x ″ + x ′ + x = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 .
Your Turn
Solve (find the impulse response) x ″ + 2 x ′ + x = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 .
Your Turn
A pulse can come later and can be bigger. Solve x ″ + 4 x = 4 δ ( t − 1 ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 .
Your Turn
Suppose that f ( t ) and g ( t ) are differentiable functions and suppose that f ( t ) = g ( t ) = 0 for all t ≤ 0 . Show that
( f * g ) ′ ( t ) = ( f ′ * g ) ( t ) = ( f * g ′ ) ( t ) .
Your Turn
Suppose that L x = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 , has the solution x = e − t for t > 0 . Find the solution to L x = t 2 , x ( 0 ) = 0 , x ′ ( 0 ) = 0 for t > 0 .
Your Turn
Compute ℒ − 1 { s 2 + s + 1 s 2 } .
Your Turn
Suppose we have a beam of length 1 simply supported at the ends and suppose that force F = 1 is applied at x = 3 4 in the downward direction. Suppose that E I = 1 for simplicity. Find the beam deflection y ( x ) .
Your Turn
Solve (find the impulse response) x ″ = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 .
Answer
x
(
t
)
=
t
Your Turn
Solve (find the impulse response) x ′ + a x = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 .
Answer
x
(
t
)
=
e
−
a
t
Your Turn
Suppose that L x = δ ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 , has the solution x ( t ) = cos ( t ) for t > 0 . Find (in closed form) the solution to L x = sin ( t ) , x ( 0 ) = 0 , x ′ ( 0 ) = 0 f o r t > 0 .
Answer
x
(
t
)
=
(
cos
*
sin
)
(
t
)
=
1
2
t
sin
(
t
)
Your Turn
Compute ℒ − 1 { s 2 s 2 + 1 } .
Answer
δ
(
t
)
−
sin
(
t
)
Your Turn
Compute ℒ − 1 { 3 s 2 e − s + 2 s 2 } .
Answer
3
δ
(
t
−
1
)
+
2
t
Your Turn
Solve
y t + y x = 1 , 0 < x < ∞ , t > 0 , y ( 0 , t ) = 1 , y ( x , 0 ) = 0 .
Your Turn
Solve
y t + α y x = 0 , 0 < x < ∞ , t > 0 , y ( 0 , t ) = t , y ( x , 0 ) = 0 .
Your Turn
Solve
y t + 2 y x = x + t , 0 < x < ∞ , t > 0 , y ( 0 , t ) = 0 , y ( x , 0 ) = 0 .
Your Turn
For an α > 0 , solve
y t + α y x + y = 0 , 0 < x < ∞ , t > 0 , y ( 0 , t ) = sin ( t ) , y ( x , 0 ) = 0 .
Your Turn
Find the corresponding ODE problem for Y ( x ) , after transforming the t variable
y t t + 3 y x x + y x t + 3 y x + y = sin ( x ) + t , 0 < x < 1 , t > 0 , y ( 0 , t ) = 1 , y ( 1 , t ) = t , y ( x , 0 ) = 1 − x , y t ( x , 0 ) = 1 .
Do not solve the problem.
Your Turn
Write down a solution to
y t = y x x , 0 < x < ∞ , t > 0 , y x ( 0 , t ) = e − t , y ( x , 0 ) = 0 ,
as an definite integral (convolution).
Your Turn
Use the Laplace transform in t to solve
y t t = y x x , − ∞ < x < ∞ , t > 0 , y t ( x , 0 ) = sin ( x ) , y ( x , 0 ) = 0 .
Hint: Note that e s x does not go to zero as s → ∞ for positive x , and e − s x does not go to zero as s → ∞ for negative x .
Your Turn
Solve
y t + y x = 1 , 0 < x < ∞ , t > 0 , y ( 0 , t ) = 0 , y ( x , 0 ) = 0 .
Answer
y
=
(
x
−
t
)
u
(
t
−
x
)
+
t
Your Turn
For a c > 0 , solve
y t + y x + c y = 0 , 0 < x < ∞ , t > 0 , y ( 0 , t ) = sin ( t ) , y ( x , 0 ) = 0 .
Answer
y
=
e
−
c
x
sin
(
t
−
x
)
u
(
t
−
x
)
Your Turn
Find the corresponding ODE problem for Y ( x ) , after transforming the t variable
y t t + 3 y x x + y = x + t , − 1 < x < 1 , t > 0 , y ( − 1 , t ) = 0 , y ( 1 , t ) = 0 , y ( x , 0 ) = ( 1 − x 2 ) , y t ( x , 0 ) = 0 .
Do not solve the problem.
Answer
s
2
Y
(
x
)
−
s
(
1
+
x
2
)
+
3
Y
″
(
x
)
+
Y
(
x
)
=
x
s
+
1
s
2
,
Y
(
−
1
)
=
0
,
Y
(
1
)
=
0
.
Your Turn
Use the Laplace transform in t to solve
y t t = y x x , − ∞ < x < ∞ , t > 0 , y t ( x , 0 ) = x 2 , y ( x , 0 ) = 0 .
Hint: Note that e s x does not go to zero as s → ∞ for positive x , and e − s x does not go to zero as s → ∞ for negative x .
Answer
y
=
t
x
2
+
t
3
3
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 .