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UPSC 2024 Maths Optional Paper 1 Q8a — Step-by-Step Solution

15 marks · Section B

Laplace transform applied to IVP for second-order linear ODE with constant coefficients · ODEs · asked 11× in 14 yrs · Read the full method →

Question

Using Laplace transform, solve the initial value problem

y′′+2y′+5y=δ(t−2),y(0)=0,y′(0)=0,y''+2y'+5y=\delta(t-2),\quad y(0)=0,\quad y'(0)=0,

where δ(t−2)\delta(t-2) denotes the Dirac delta function.

Technique

Standard Laplace transform; complete-the-square inversion; time-shift theorem for the e−2se^{-2s} factor.

Solution

Step 1 — Laplace transform.

With zero initial conditions and L{δ(t−2)}=e−2s\mathcal L\{\delta(t-2)\}=e^{-2s}:

(s2+2s+5)Y(s)=e−2s  ⇒  Y(s)=e−2ss2+2s+5.(s^2+2s+5)Y(s)=e^{-2s}\;\Rightarrow\;Y(s)=\frac{e^{-2s}}{s^2+2s+5}.

Step 2 — Invert 1/(s2+2s+5)1/(s^2+2s+5).

Complete the square: s2+2s+5=(s+1)2+4s^2+2s+5=(s+1)^2+4.

L−1 ⁣{1(s+1)2+4}=12e−tsin⁡2t.\mathcal L^{-1}\!\left\{\frac{1}{(s+1)^2+4}\right\}=\tfrac{1}{2}e^{-t}\sin 2t.

Step 3 — Time-shift theorem.

Since Y(s)=e−2s⋅F(s)Y(s)=e^{-2s}\cdot F(s) with f(t)=12e−tsin⁡2tf(t)=\tfrac{1}{2}e^{-t}\sin 2t:

y(t)=u(t−2)⋅f(t−2)=u(t−2)⋅12e−(t−2)sin⁡ ⁣(2(t−2)).y(t)=u(t-2)\cdot f(t-2)=u(t-2)\cdot\tfrac{1}{2}e^{-(t-2)}\sin\!\bigl(2(t-2)\bigr).

Explicitly:

Answer

  y(t)=u(t−2)⋅12e−(t−2)sin⁡ ⁣(2(t−2)).  \boxed{\;y(t)=u(t-2)\cdot\tfrac{1}{2}e^{-(t-2)}\sin\!\bigl(2(t-2)\bigr).\;}
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