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A

Section A: Long Answer Questions

Attempt all / any as specified.

4 questions
1long12 marks

(a) Define the Laplace transform of a function f(t)f(t) and state the conditions of existence. Find the Laplace transform of f(t)=e2ttcos3tf(t) = e^{-2t}\,t\cos 3t using the appropriate shifting and differentiation theorems. [6]

(b) Using the Laplace transform method, solve the initial value problem

y+4y+4y=e2t,y(0)=0,  y(0)=1.y'' + 4y' + 4y = e^{-2t}, \qquad y(0)=0,\; y'(0)=1.

[6]

laplace-transformsinverse-laplaceode-ivp
2long12 marks

(a) Obtain the Fourier series expansion of the periodic function defined by

f(x)={x,π<x<0    x,    0<x<πf(x) = \begin{cases} -x, & -\pi < x < 0 \\ \;\;x, & \;\;0 < x < \pi \end{cases}

with period 2π2\pi, and hence deduce that n=11(2n1)2=π28\displaystyle \sum_{n=1}^{\infty} \frac{1}{(2n-1)^2} = \frac{\pi^2}{8}. [8]

(b) Find the half-range cosine series for f(x)=xf(x) = x in the interval 0<x<20 < x < 2. [4]

fourier-serieshalf-range-expansion
3long12 marks

A laterally insulated thin rod of length LL has its ends at x=0x=0 and x=Lx=L maintained at zero temperature. The initial temperature distribution is u(x,0)=f(x)u(x,0)=f(x).

(a) Using the method of separation of variables, derive the solution of the one-dimensional heat equation ut=c22ux2\dfrac{\partial u}{\partial t} = c^2 \dfrac{\partial^2 u}{\partial x^2} subject to the given boundary and initial conditions. [8]

(b) Hence write down the temperature distribution when f(x)=3sinπxL5sin4πxLf(x) = 3\sin\dfrac{\pi x}{L} - 5\sin\dfrac{4\pi x}{L}. [4]

partial-differential-equationsheat-equationboundary-value-problems
4long12 marks

(a) Using the Frobenius (power series) method, find the series solution of the differential equation

2xy+(1x)yy=02x\,y'' + (1-x)\,y' - y = 0

about the regular singular point x=0x=0, obtaining the indicial equation and the recurrence relation. [8]

(b) Show that the Bessel equation of order nn, x2y+xy+(x2n2)y=0x^2 y'' + x y' + (x^2 - n^2)y = 0, reduces to the elementary form whose solution for n=12n=\tfrac12 can be expressed in terms of sinxx\dfrac{\sin x}{\sqrt{x}}. [4]

series-solution-odefrobenius-methodbessel-functions
B

Section B: Short Answer Questions

Attempt all / any as specified.

7 questions
5short8 marks

(a) State and prove the convolution theorem for Laplace transforms, and use it to evaluate L1{1(s2+a2)2}\mathcal{L}^{-1}\left\{\dfrac{1}{(s^2+a^2)^2}\right\}. [5]

(b) Find the Laplace transform of the full-wave rectified sine wave f(t)=sintf(t)=|\sin t|, which is periodic with period π\pi. [3]

laplace-transformsconvolutionperiodic-functions
6short8 marks

(a) Evaluate the line integral C[(3x28y2)dx+(4y6xy)dy]\displaystyle \oint_C \left[(3x^2 - 8y^2)\,dx + (4y - 6xy)\,dy\right] where CC is the boundary of the region bounded by y=xy=\sqrt{x} and y=x2y=x^2, using Green's theorem. [5]

(b) Determine whether the vector field F=(2xy+z3)i^+x2j^+3xz2k^\vec{F} = (2xy + z^3)\hat{i} + x^2\hat{j} + 3xz^2\hat{k} is conservative, and if so find its scalar potential. [3]

line-integralsgreens-theorem
7short8 marks

(a) Verify the Divergence (Gauss) theorem for F=x2i^+y2j^+z2k^\vec{F} = x^2\hat{i} + y^2\hat{j} + z^2\hat{k} taken over the surface of the cube bounded by x=0,x=1,y=0,y=1,z=0,z=1x=0,\,x=1,\,y=0,\,y=1,\,z=0,\,z=1. [5]

(b) State Stokes' theorem and explain its physical significance. [3]

surface-integralsdivergence-theoremstokes-theorem
8short8 marks

(a) State Rodrigues' formula for the Legendre polynomials Pn(x)P_n(x) and use it to obtain P2(x)P_2(x) and P3(x)P_3(x). [4]

(b) Prove the orthogonality property 11Pm(x)Pn(x)dx=0\displaystyle \int_{-1}^{1} P_m(x)\,P_n(x)\,dx = 0 for mnm \neq n. [4]

legendre-functionsrodrigues-formulaorthogonality
9short8 marks

(a) Derive the Cauchy-Riemann equations and use them to show that f(z)=z2f(z)=z^2 is analytic everywhere, finding f(z)f'(z). [4]

(b) Given the harmonic function u(x,y)=x33xy2u(x,y) = x^3 - 3xy^2, find the conjugate harmonic function v(x,y)v(x,y) and express the corresponding analytic function f(z)=u+ivf(z)=u+iv in terms of zz. [4]

complex-analysiscauchy-riemannanalytic-functions
10short8 marks

(a) Form the partial differential equation by eliminating the arbitrary functions from z=f(x+ct)+g(xct)z = f(x+ct) + g(x-ct). [3]

(b) Using d'Alembert's method, obtain the solution of the one-dimensional wave equation 2yt2=c22yx2\dfrac{\partial^2 y}{\partial t^2} = c^2 \dfrac{\partial^2 y}{\partial x^2} for an infinite string with initial displacement y(x,0)=ϕ(x)y(x,0)=\phi(x) and initial velocity yt(x,0)=0\dfrac{\partial y}{\partial t}(x,0)=0. [5]

partial-differential-equationswave-equationdalembert-solution
11short8 marks

(a) Find the complex (exponential) form of the Fourier series of f(x)=exf(x)=e^{x} on the interval π<x<π-\pi < x < \pi. [5]

(b) State Parseval's identity for Fourier series and explain its significance in terms of average power. [3]

fourier-seriescomplex-fourierparseval-theorem