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A collection of practice problems related to laplace transform and linear systems. It includes finding the laplace transform of various functions, finding the inverse laplace transform, determining the solution of differential equations, and solving initial value problems for linear systems.
Typology: Exercises
1 / 6
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PRACTICE PROBLEMS CHAPTER 6 AND 7 I. Laplace Transform
1, if 0 ≤ t 2, t 2 − 4 t 4, if t ≥ 2
t , if 0 ≤ t 3, 5, if t ≥ 3 (h) f^ t^ = { 0, if t , t − , if ≤ t 2 0 , if t ≥ 2
cos t , if t 4, 0, if t ≥ 4 (j) f t =
t , if 0 ≤ t 1, e t , if t ≥ 1
1
2 t e t
1
2 − 1
x e t
1
− 2 − 6
x Two solutions of the system are x 1 = e t
− 2
and x 2 = e − 2 t
1
(a) Use the Wronskian to verify that the two solutions are linearly independent. (b) Write the general solution of the system.
ANSWERS TO PRACTICE PROBLEMS CHAPTER 6 AND 7 I. Laplace Transform
1 s s s 2
(c) Using the property L { t f t }=− F ' s with F^ ^ s =L^ { e 2 t sin 3 t }= 3 s − 2 2 9 yields L { t e 2 t sin 3 t }= 6 s − 2
2
2 (d) f^ t^ =[ t −^7 ^10 ] u 7 t^ .^ Thus L^ {^ f^ t^ }= e − 7 s L { t 10 }= e − 7 s
1 s 2 ^ 10
(e) L^ {^ f^ t^ }= e − 3 s L { t 3 2 }= e − 3 s L { t 2 6t 9 }= e − 3 s
2 s 3 ^ 6 s 2 ^ 9
(f) f t = 1 u 2 t t 2
2
Thus L^ {^ f^ t^ }=^ 1 s e − 2 s L { t 2 − 1 }= 1 s e − 2 s
2 s 3 −^ 1
(g) f^ t^ = t^ − u 3 t^ t^ −^5 = t − u 3 t^ [ t −^3 −^2 ].^ Thus L { f t }= 1 s 2 − e − 3 s L{ t − 2 }= 1 s 2 − e −3s
1 s 2 −^ 2
(h) f^ t^ = u t^ t −− u 2 t^ t −= u t^ t^ −− u 2 t^ t^ −^2 Thus L^ {^ f^ t^ }= e − s L{ t }− e − 2 s L { t }= e − s s 2 − e − 2 s
1 s 2 ^
(i) f^ t^ =cos^ t^ − u 4 t^ cos^ ^ t^ =cos t^ − u 4 t^ cos^ t −^4 ^ Thus L { f t }= s 2 s 2 − e − 4 s L{cos t }= s 2 s 2 − e − 4 s s 2 s 2 (j) f t = t u 1 t [ e t − t ]= t u 1 t [ e t − 1 1 − t − 1 − 1 ] Thus L { f t }= 1 s 2 e − s L { e t 1 − t − 1 }= 1 s 2 e − s
e s − 1 − 1 s 2 −^ 1
(a) Using PFD, F^ ^ s =−^ 1 4 1 s 1 − 1 2 1 s 1 2 ^ 1 4 1 s − 1
. (^) Thus f t =− 1 4 e − t − 1 2 t e − t 1 4 e t (b) F ( s ) can be rewritten as F^ ^ s =^ 2 s 3 s 2 2 9 = 2 s 2 − 1 s 2 2 9 = 2 s 2 s 2 2 9 − 1 3 3 s 2 2 9 .
Thus f^ t^ = e − 2 t
1 3
(c) The inverse Laplace is u 3 t^ ^ f^ t −^3 ^ where f^ t^ =L − 1
1
= e 2 t . Thus L − 1
e − 3 s
= u 3 t e 2 t − 3 (d) F^ ^ s =^ 1
s 2 6 e − 2 s
s 2 6 thus L − 1 { F s }= 1
1
1 s − s s 2
. (^) (b) y t = 1 2 sin 2 t u 5 t [ 1 −cos 2 t − 10 ]
1
2 e t 2 t e t
1
3 e t 2 t e t 2 e t 2 t e
Substituting x into the right hand side of the DE yields:
2 − 1
e t 2 t e t 2 t e
t
1
2 e t 4 t e t − 2 t e t 3 e t 6 t e t − 4 t e
e t − e
3 e t 2 t e t 2 e t 2 t e
x y
P t =
t − 1 e t 2 t 2 − 1 0 3 t t
f t =
0 0 e
u'
0 1
u
0
u 0
2