kma354 partial differential equations applications & methods
TRANSCRIPT
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Student ID No:Pages: 6
Questions : 5
UNIVERSITY OF TASMANIA
EXAMINATIONS FOR DEGREES AND DIPLOMAS
October / November 2011
KMA354 Partial Differential EquationsApplications & Methods
First and Only Paper
Examiner: Dr Michael Brideson
Time Allowed: TWO (2) hours.
Instructions:
- Attempt all FIVE (5) questions.
- All questions carry the same number of marks.
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KMA354 Partial Differential Equations, 2011 - 2 -
1. A solution to the Telegraph equation,
∂2E
∂t2+ α
∂E
∂t− c2
∂2E
∂x2= 0 ,
can be obtained by letting E(x, t) = v(t)U(x, t) with a view to removing the first
order time derivative.
Use this process to obtain the Klein-Gordon equation,
∂2U
∂t2− c2
∂2U
∂x2−
α2
4U = 0 .
Continued . . .
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KMA354 Partial Differential Equations, 2011 - 3 -
2. (a) Use the Method of Characteristics to solve the following initial value prob-
lem.∂U
∂x+
∂U
∂t+ 2U = 0 ,
U(x, 0) = sin(x).
(b) Use the one sided Green’s function technique to solve
U ′′(x) + U ′(x) = ex x > 0
U(0) = 1
U ′(0) = 0.
Continued . . .
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KMA354 Partial Differential Equations, 2011 - 4 -
3. Consider the nonhomogeneous wave equation
∂2U
∂t2−
∂2U
∂x2= x , 0 < x < 1, t > 0 ;
with initial and boundary conditions,
BCs : U(0, t) = 0 , t > 0 ;
U(1, t) = 0 , t > 0 ;
ICs : U(x, 0) = x , 0 < x < 1 ;
∂U
∂t(x, 0) = 0 0 < x < 1.
Make a suitable substitution to turn this into two subproblems and solve for
U(x, t).
You do not have to evaluate the integral for the Fourier coefficients but you must
show its derivation.
Continued . . .
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KMA354 Partial Differential Equations, 2011 - 5 -
4. (a) Use an appropriate power series method to solve
dy
dx− y = x2 .
Hint: Consider the Maclaurin series for ex.
(b) Consider the Cauchy-Euler equation,
x2d2y
dx2+ x
dy
dx− k2 y = 0 with k ∈ IR.
Show that x = 0 is a regular singular point.
Continued . . .
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KMA354 Partial Differential Equations, 2011 - 6 -
5. (a) In the context of the regular Sturm-Liouville boundary value problem
d
dx
[
H(x)dy
dx
]
+ (Q(x) + λW (x))y = 0 −∞ < a ≤ x ≤ b < ∞
a1 y(a) + a2 y′(a) = 0
b1 y(b) + b2 y′(b) = 0 ,
interpret the expression
(λj − λk)∫ b
aW (x) yj(x) yk(x) dx =
[
H(x)(yj(x) y′
k(x)− yk(x) y′
j(x))]b
a.
You do not have to consider all specific cases for the right hand side, but you
must comment on the two general cases, j = k and j 6= k.
(b) The equation,
(1− x2)d2y
dx2− 2x
dy
dx+ l (l + 1) y = 0 ,
has polynomial solutions Pl(x) for integer l.
Put the equation in self-adjoint form and give an orthogonality relation.
END OF EXAM PAPER
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