← 2013 Paper 1
UPSC Maths 2013 Paper 1 Q6d — Solution
15 marks · Section B
Question
By using Laplace transform method, solve the differential equation
(D2+n2)x=asin(nt+α),D2≡dt2d2
subject to the initial conditions x=0 and dtdx=0 at t=0, in which a,n,α are constants.
Technique
Standard Laplace approach for linear ODEs with constant coefficients and zero IC; the RHS Laplace produces a denominator (s2+n2), which when multiplied by the system transfer denominator yields (s2+n2)2 — a resonance signature.
Solution
Strategy. Apply Laplace transform; the zero initial conditions simplify the L{x′′} term; invert via standard pairs.
With X(s)=L{x(t)} and x(0)=x′(0)=0:
L{x′′}=s2X(s).
For the RHS, expand sin(nt+α)=sinntcosα+cosntsinα, so
L{sin(nt+α)}=s2+n2ncosα+ssinα.
The transformed ODE:
(s2+n2)X(s)=a⋅s2+n2ncosα+ssinα⟹X(s)=(s2+n2)2a(ncosα+ssinα).
Step 2 — Inverse Laplace via standard pairs
Use these inverse-Laplace results:
L−1{(s2+n2)21}=2n3sinnt−ntcosnt,L−1{(s2+n2)2s}=2ntsinnt.
(The first is derived via convolution of sinnt/n with itself; the second is a standard table entry, equivalent to L{tsinnt}=2ns/(s2+n2)2.)
Substitute:
x(t)=a⋅ncosα⋅2n3sinnt−ntcosnt+asinα⋅2ntsinnt.
Simplify:
x(t)=2n2acosα(sinnt−ntcosnt)+2natsinαsinnt.
Factor out 2n2a:
x(t)=2n2a[cosαsinnt−ntcosαcosnt+ntsinαsinnt].
The middle and last terms combine: −nt(cosαcosnt−sinαsinnt)=−ntcos(nt+α). Therefore
Answer
x(t)=2n2a[cosαsinnt−ntcos(nt+α)].