← 2025 Paper 1

UPSC 2025 Maths Optional Paper 1 Q6a — Step-by-Step Solution

15 marks · Section B

Properties of Laplace transform (linearity, shift, derivative, convolution) · ODEs · asked 4× in 14 yrs · Read the full method →

Question

If F(s)F(s) and G(s)G(s) are Laplace transforms of f(t)f(t) and g(t)g(t) respectively, then prove that L(∫0tf(x) g(t−x) dx)=F(s) G(s)\mathcal{L}\left(\displaystyle\int_0^t f(x)\,g(t - x)\,dx\right) = F(s)\,G(s). Using this result, solve the equation y(t)=t+∫0ty(x)sin⁡(t−x) dxy(t) = t + \displaystyle\int_0^t y(x)\sin(t - x)\,dx.

Technique

Prove the Laplace convolution theorem, then apply it to the integral equation: transform to the ss-domain, solve algebraically for Y(s)Y(s), and invert.

Solution

Part 1 — Proof of the convolution theorem

By definition,

L ⁣(∫0tf(x) g(t−x) dx)=∫0∞e−st(∫0tf(x) g(t−x) dx)dt.\mathcal{L}\!\left(\int_0^t f(x)\,g(t-x)\,dx\right) = \int_0^\infty e^{-st}\left(\int_0^t f(x)\,g(t-x)\,dx\right)dt.

The region of integration is {(x,t):0≤x≤t<∞}\{(x,t): 0\le x\le t<\infty\}. Interchange the order (Fubini, valid since both transforms exist absolutely):

=∫0∞f(x)(∫x∞e−st g(t−x) dt)dx.= \int_0^\infty f(x)\left(\int_x^\infty e^{-st}\,g(t-x)\,dt\right)dx.

In the inner integral put τ=t−x\tau = t - x (dτ=dtd\tau = dt, τ:0→∞\tau: 0\to\infty):

∫x∞e−stg(t−x) dt=∫0∞e−s(τ+x)g(τ) dτ=e−sx∫0∞e−sτg(τ) dτ=e−sxG(s).\int_x^\infty e^{-st} g(t-x)\,dt = \int_0^\infty e^{-s(\tau+x)} g(\tau)\,d\tau = e^{-sx}\int_0^\infty e^{-s\tau} g(\tau)\,d\tau = e^{-sx}G(s).

Therefore

L ⁣(∫0tf(x)g(t−x) dx)=∫0∞f(x) e−sx dx⋅G(s)=F(s) G(s).■\mathcal{L}\!\left(\int_0^t f(x)g(t-x)\,dx\right) = \int_0^\infty f(x)\,e^{-sx}\,dx \cdot G(s) = F(s)\,G(s). \qquad\blacksquare

Part 2 — Solving the integral equation

y(t)=t+∫0ty(x)sin⁡(t−x) dx=t+(y∗sin⁡)(t).y(t) = t + \int_0^t y(x)\sin(t-x)\,dx = t + (y * \sin)(t).

Take Laplace transforms, with Y(s)=L{y}Y(s)=\mathcal{L}\{y\}, L{t}=1s2\mathcal{L}\{t\}=\dfrac{1}{s^2}, L{sin⁡t}=1s2+1\mathcal{L}\{\sin t\}=\dfrac{1}{s^2+1}, and using the convolution theorem on the last term:

Y=1s2+Y⋅1s2+1.Y = \frac{1}{s^2} + Y\cdot\frac{1}{s^2+1}.

Solve for YY:

Y(1−1s2+1)=1s2  ⟹  Y⋅s2s2+1=1s2  ⟹  Y(s)=s2+1s4=1s2+1s4.Y\left(1 - \frac{1}{s^2+1}\right) = \frac{1}{s^2} \;\Longrightarrow\; Y\cdot\frac{s^2}{s^2+1} = \frac{1}{s^2} \;\Longrightarrow\; Y(s) = \frac{s^2+1}{s^4} = \frac{1}{s^2} + \frac{1}{s^4}.

Invert termwise, using L−1{1/s2}=t\mathcal{L}^{-1}\{1/s^2\}=t and L−1{1/s4}=t33!=t36\mathcal{L}^{-1}\{1/s^4\}=\dfrac{t^3}{3!}=\dfrac{t^3}{6}:

y(t)=t+t36.y(t) = t + \frac{t^3}{6}.

Answer

  L ⁣(∫0tf(x)g(t−x) dx)=F(s)G(s),y(t)=t+t36.  \boxed{\;\mathcal{L}\!\left(\int_0^t f(x)g(t-x)\,dx\right) = F(s)G(s),\qquad y(t) = t + \frac{t^3}{6}.\;}
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