Deck 13: Boundary-Value Problems in Other Coordinate Systems
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Deck 13: Boundary-Value Problems in Other Coordinate Systems
1
In the previous problem, the solution of the eigenvalue problem is
A)
B)
C)
, where 
D)
, where 
E)
, where 
A)

B)

C)


D)


E)


C
2
Using the separation of the previous problem, the equation for
becomes
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

C
3
The two dimensional wave equation in polar coordinates is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

C
4
Consider the vibrations of a circular membrane of radius 2 clamped along the circumference, with an initial displacement of
and an initial velocity of zero. The mathematical model for this situation is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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5
In the previous four problems, the infinite series solution of the original problem is (for certain values of the constants
and
)
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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6
The equations relating Cartesian and spherical coordinates include Select all that apply.
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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7
In the previous problem, separate variables using
. The resulting problems are
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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8
The solution of
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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9
In the previous four problems, the infinite series solution of the original problem is
where Select all that apply.
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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10
In changing from Cartesian to spherical coordinates,
becomes
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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11
In the three previous problems, the product solutions are
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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12
In the previous three problems, the solution for
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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13
In the previous problem, the solution of the eigenvalue problem is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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14
In separating variables, using,
, in the equation
, the resulting equation for
and is
A)
B)
C)
D)
E)



A)

B)

C)

D)

E)

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15
In the previous problem, if we also require that
be bounded everywhere, the solution of the eigenvalue problem is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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16
In changing from Cartesian to polar coordinates,
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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17
In changing from Cartesian to polar coordinates,
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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18
In the previous problem, after separating variables using
. the resulting problems are
A)
is bounded 
B)
is bounded 
C)
is bounded 
D)
is bounded 
E)
is bounded 

A)


B)


C)


D)


E)


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19
Consider the steady-state temperature distribution in a circular disc of radius
centere at the origin, with temperature given as a function,
on the boundary
and zero on the boundaries
and
The mathematical model of this situation is
A)
B)
C)
D)
E)





A)

B)

C)

D)

E)

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20
In the previous three problems, the product solutions are
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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21
In the previous problem, the solution of the eigenvalue problem is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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Unlock Deck
k this deck
22
In changing from Cartesian to polar coordinates,
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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23
In the previous problem, separate variables using
. The resulting problems are
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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k this deck
24
In changing from Cartesian to polar coordinates,
is
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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25
The relationships between Cartesian and spherical coordinates are Select all that apply.
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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26
In the previous three problems, the product solutions are
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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27
Consider the steady-state temperature distribution in a circular cylinder of radius 2 and height 3, with zero temperature at
and at
and a temperature of 10 at
. The mathematical model for this problem is
A)
B)
C)
D)
E)



A)

B)

C)

D)

E)

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28
In the problem
, separate variables, using
. The resulting problems for
and
are
A)
is bounded;
is bounded on
.
B)
is bounded;
is bounded on
.
C)
is bounded;
is bounded on
.
D)
is bounded;
is bounded on
.
E)
is bounded;
is bounded on
.




A)



B)



C)



D)



E)



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29
The Laplacian in polar coordinates is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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30
Consider the steady-state temperature distribution in a circular disc of radius
centere at the origin, with temperature given as a function,
on the boundary. The mathematical model of this situation is
A)
B)
C)
D)
E)


A)

B)

C)

D)

E)

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31
In the previous four problems, the infinite series solution is (for certain values of the constants)
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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32
In the three previous problems, the product solutions are
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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33
The solution of
is
A)
B)
C)
D)
E) none of the above

A)

B)

C)

D)

E) none of the above
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34
In the previous problem, the solution of the eigenvalue problem is
A)
B)
C)
D)
E)
A)

B)

C)

D)

E)

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Unlock Deck
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35
In the previous two problems, the product solutions are
A)
B)
C)
D)
E) none of the above
A)

B)

C)

D)

E) none of the above
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Unlock Deck
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36
In the previous problem, after separating variables, the resulting problems are
A)
is bounded, 
B)
is bounded, 
C)
is bounded, 
D)
is bounded, 
E)
is bounded, 
A)


B)


C)


D)


E)


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37
When changing from Cartesian to spherical coordinates, 
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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Unlock Deck
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38
In the previous four problems, the infinite series solution of the original problem is
where Select all that apply.
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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Unlock Deck
k this deck
39
In the previous problem, the solution of the eigenvalue problem is
A)
, where 
B)
, where 
C)
D)
E)
A)


B)


C)

D)

E)

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40
When changing from Cartesian to spherical coordinates, 
A)
B)
C)
D)
E)

A)

B)

C)

D)

E)

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Unlock Deck
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