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Questions from the university of cambridge tripos examination for the natural sciences, focusing on mathematics and physics. Topics include gradient in cartesian and orthogonal curvilinear coordinates, vibrations of a violin string, fourier transforms, eigenvalues and eigenvectors, and sturm-liouville equations.
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Tuesday 30 May 2006 9 to 12
You may submit answers to no more than six questions. All questions carry the same number of marks.
The approximate number of marks allocated to a part of a question is indicated in the right hand margin.
Write on one side of the paper only and begin each answer on a separate sheet.
Each question has a number and a letter (for example, 6A).
Answers must be tied up in separate bundles, marked A, B or C according to the letter affixed to each question.
Do not join the bundles together.
For each bundle, a blue cover sheet must be completed and attached to the bundle.
A separate yellow master cover sheet listing all the questions attempted must also be completed.
Every cover sheet must bear your examination number and desk number.
Let x, y, z be Cartesian co-ordinates, and let Φ be a scalar field.
Define the gradient ∇Φ in Cartesian co-ordinates. Let q 1 , q 2 , q 3 be orthogonal curvilinear co-ordinates. Show that the gradient of Φ in orthogonal curvilinear co-ordinates is
∂q 1
e 1 h 1
∂q 2
e 2 h 2
∂q 3
e 3 h 3
and define the quantities ei and hi which appear in this expression. (^) [8]
Oblate spheroidal co-ordinates (R, θ, φ) are defined by
x = cosh R cos θ cos φ y = cosh R cos θ sin φ z = sinh R sin θ.
Show that the co-ordinate surfaces associated with R, θ, φ intersect at right angles. (^) [8]
Show that for these co-ordinates,
hR = hθ =
sinh^2 R + sin^2 θ, hφ = cosh R cos θ.
Paper 1
The Fourier transform of a function f is given by
f˜ (k) =
−∞
f (x)e−ikxdx.
Give the expression for the inverse Fourier transform.
Let α > 0 and define for non-negative integer n:
fn(x) =
xne−αx^ x > 0 0 x 6 0
Show that
f˜ 0 (k) = 1 α + ik
and f˜n(k) = n α + ik
f˜n− 1 (k) , n = 1, 2 ,...
Hence compute f˜n(k). (^) [8]
Prove the following identity (Parseval’s theorem) for functions f and g:
∫ (^) ∞
−∞
[f (x)]∗g(x)dx =
2 π
−∞
[ f˜ (k)]∗^ g˜(k)dk ,
where ∗^ denotes complex conjugation. (^) [8]
Hence show that
∫ (^) ∞
−∞
(α^2 + k^2 )n+^
dk =
2 π(2n)! (n!)^2 (2α)^2 n+^
[In this question all functions may be assumed to be sufficiently integrable so that their Fourier transforms and inverse Fourier transforms are well-defined.]
Paper 1
(i) Let a ∈ Rn^ be a fixed n-component real vector, a 6 = 0. Let A+^ and A−^ be real n × n matrices with components
(A±)ij = δij ± aiaj.
Obtain the eigenvalues of A±^ and describe the corresponding eigenvectors. (^) [4]
Show that A+^ is always invertible and obtain necessary and sufficient conditions for A−^ to be invertible. [4]
(ii) Let b ∈ R^3 be a fixed vector, b 6 = 0. Let B+^ and B−^ be real 3 × 3 matrices with components (B±)ij = δij ± bibj + ijkbk.
By choosing a suitable basis for R^3 , or otherwise, determine the real eigenvalues of B± and the corresponding eigenvectors. (^) [6]
Show that B+^ is invertible and obtain necessary and sufficient conditions for B− to be invertible. [6]
What does it mean for a n × n square matrix to be diagonalizable? (^) [2]
Suppose that A is a n × n square matrix such that Ap^ = 0 for some positive integer p. Show that A has 0 as an eigenvalue. Show also that A cannot be diagonalizable unless A = 0. [6]
Let B and C be the matrices
4 + 2α − 2 − 2 − 4 α 3 α − 3 9 − 6 α 2 + α − 1 − 1 − 2 α
for α ∈ R, and
C =
By considering the characteristic polynomials of B and C, determine whether B and C are diagonalizable. (^) [12]
Paper 1 [TURN OVER
7C Show how to express the eigenvalue equation
d^2 y dx^2
dy dx
(where u(x), v(x), w(x) are real functions and w(x) > 0 for a 6 x 6 b) in Sturm–Liouville form, (^) [6] d dx
p(x)
dy dx
Suppose that y satisfies the boundary conditions
k 1 y(a) + k 2 y′(a) = 0 , l 1 y(b) + l 2 y′(b) = 0 ,
where k 1 , k 2 , l 1 , l 2 are constants. Show that two eigenfunctions ym, yn, with distinct eigenvalues λm 6 = λn satisfy the orthogonality condition
∫ (^) b
a
r(x)ymyndx =
λm − λn
p(b)(y′ n(b)ym(b) − y m′(b)yn(b))
− p(a)(y′ n(a)ym(a) − y′ m(a)yn(a))
Find the eigenfunctions and the values of the eigenvalue λ that satisfy the equation
y′′^ + 2αy′^ + (α^2 + λ)y = 0 ,
where y(0) = y(π) = 0. (^) [6]
Put the equation in Sturm–Liouville form and hence determine the orthogonality condition for the eigenfunctions. (^) [4]
Paper 1 [TURN OVER
By first finding the appropriate Green’s function, solve the differential equation
y′′(x) + k^2 y(x) = f (x) ,
where k is a non-zero real number for the cases:
y(0) = y′(0) = 0 , f (x) = 2k cos kx ,
[10]
and
y(0) = y
( (^) π
6 k
= 0 , f (x) =
k^2 2
[You may use the identity sin(A ± B) = sin A cos B ± cos A sin B.]
Paper 1
10C State the Euler equation obtained by minimizing
∫ (^) x 2 x 1 f^ (x, y(x), y
′(x)) dx, with
y(x 1 ) and y(x 2 ) fixed at the boundaries. (^) [3]
If f is not an explicit function of x, show that
y′^
∂f ∂y′^
− f
is constant. [3]
A bead slides down a frictionless wire, starting at rest at x = 0, y = 0 and reaching a point B at x = xB , y = yB after a time t. By considering the bead’s total energy, show that its velocity at any point during its motion is given by v =
2 gy. (^) [4]
Hence, show that the time T [y] taken to reach B depends on the shape of the wire y(x) according to
T [y] =
2 g
∫ (^) xB
0
1 + y′^2 y
dx.
Consider the variational problem that determines the shape of the wire that minimizes the time (the brachistochrone) and show that the quantity y(1 + y′^2 ) is constant for such a shape. Hence, determine the parametric equations of the brachistochrone,
x = c(θ − 12 sin 2θ) , y = c sin^2 θ ,
where c is a constant and θ parameterizes the curve. (^) [5]
Show that if xB = l and yB = 0 the minimum time is equal to
2 πl/g. (^) [5]
Paper 1