Deck 14: Integral Transform Method
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Deck 14: Integral Transform Method
1
The solution of the integral equation
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
B
2
In the three previous problems, the solution for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

B
3
Let
. The Fourier integral representation of f is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
C
4
In the previous problem, the solution for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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5
In the previous problem, the integral converges at
to the value
A) 0
B)
C) 1
D) 2
E)

A) 0
B)

C) 1
D) 2
E)

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6
The value of
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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7
The value of
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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8
In the previous two problems, the integral converges for
to the function
A)
B)
C)
D) 1
E) none of the above

A)

B)

C)

D) 1
E) none of the above
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9
In the previous three problems, the solution for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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10
The complementary error function is defined as
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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11
In the previous problem, assume that
. The solution for
is
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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12
Apply a Fourier transform in
in the previous problem. The resulting equation for
is
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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13
The Fourier cosine integral of a function f defined on
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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14
In the previous problem, the integral converges at
to the value
A) 0
B) 1
C) 2
D) 3
E) 4

A) 0
B) 1
C) 2
D) 3
E) 4
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15
In the previous problem, if
is
A)
B)
C)
D)
E) 0

A)

B)

C)

D)

E) 0
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16
Consider the temperature,
, in an infinite rod
, with an initial temperature of
. The mathematical model for this is
A)
B)
C)
D)
E)



A)

B)

C)

D)

E)

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17
In the previous problem, apply the Laplace transform. The resulting equation for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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18
Consider a semi-infinite, elastic, vibrating string, with zero initial position and velocity, driven by a vertical force at
, so that
. Assume that
. The mathematical model for the deflection,
, is
A)
B)
C)
D)
E)




A)

B)

C)

D)

E)

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19
The value of
is
A) 0
B) 1
C)
D)
E)

A) 0
B) 1
C)

D)

E)

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20
The Fourier cosine integral of
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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21
In the previous problem, assume that
. The solution for
is
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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22
The value of
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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23
The error function is defined as
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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24
Consider the problem of finding the temperature in a semi-infinite rod with zero initial temperature and a fixed constant temperature,
, at
. The mathematical model for this problem is
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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25
The value of
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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26
The value of
is
A) 0
B) 1
C)
D)
E)

A) 0
B) 1
C)

D)

E)

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27
The Laplace transform of a function f is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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28
The Fourier integral representation of a function f is given by
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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29
In the three previous problems, the solution for the temperature
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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30
If
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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31
In the previous problem, apply the Laplace transform. The resulting equation for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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32
Suppose
. In the convolution theorem, the formula for the Fourier transform is Select all that apply.
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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33
The complex form of the Fourier integral of a function f is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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34
In the previous problem, the integral representation converges at
to the value
A) 0
B) 1
C)
D) -1
E) none of the above

A) 0
B) 1
C)

D) -1
E) none of the above
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35
In the three previous problems, the solution for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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36
If
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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37
Let
. The Fourier integral representation of f is
, where
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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38
Consider the problem of a vibrating string, tightly-stretched between
and
, with a fixed initial position,
, and zero initial velocity. The mathematical problem for the deflection,
, is 
A)
B)
C)
D)
E)





A)

B)

C)

D)

E)

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39
In the previous problem, apply a Fourier sine transform in x. The new problem for the transform
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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40
In the previous problem, the solution is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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