Inverse Laplace transform

At a Glance

Why This Chapter Matters

Both UPSC questions on inverse Laplace transforms are short (5–6 marks) and follow a fixed recipe: decompose the expression into recognisable pieces, apply the matching inversion rule to each piece, combine. The 2018 question is a straightforward partial-fractions inversion. The 2015 question combines two harder rules — the log-derivative rule for ln⁡(1+1/s2)\ln(1+1/s^2) and the second-shift theorem for the e−πse^{-\pi s} factor — but each sub-step is mechanical. Knowing four rules cold (partial fractions, first-shift, second-shift, log-derivative via L{tf}=−F′(s)\mathcal{L}\{tf\}=-F'(s)) covers everything in this atom and also supports the IVP-solving questions in P1-OD-15.

Minimum Theory

Linearity. L−1{aF+bG}=aL−1{F}+bL−1{G}\mathcal{L}^{-1}\{aF+bG\}=a\mathcal{L}^{-1}\{F\}+b\mathcal{L}^{-1}\{G\}.

Standard inverse pairs.

L−1 ⁣{1s−a}=eat,L−1 ⁣{n!sn+1}=tn,L−1 ⁣{as2+a2}=sin⁡at,L−1 ⁣{ss2+a2}=cos⁡at.\mathcal{L}^{-1}\!\left\{\frac{1}{s-a}\right\}=e^{at},\qquad \mathcal{L}^{-1}\!\left\{\frac{n!}{s^{n+1}}\right\}=t^n,\qquad \mathcal{L}^{-1}\!\left\{\frac{a}{s^2+a^2}\right\}=\sin at,\qquad \mathcal{L}^{-1}\!\left\{\frac{s}{s^2+a^2}\right\}=\cos at.

Second shift theorem. If L−1{F(s)}=f(t)\mathcal{L}^{-1}\{F(s)\}=f(t), then L−1{e−asF(s)}=f(t−a) u(t−a)\mathcal{L}^{-1}\{e^{-as}F(s)\}=f(t-a)\,u(t-a), where uu is the Heaviside step function.

Log-derivative rule. If L{tf(t)}=−F′(s)\mathcal{L}\{tf(t)\}=-F'(s), then L−1{F(s)}=f(t)\mathcal{L}^{-1}\{F(s)\}=f(t) where tf(t)=L−1{−F′(s)}tf(t)=\mathcal{L}^{-1}\{-F'(s)\}. Concretely: differentiate F(s)F(s), recognise −F′(s)-F'(s) as the transform of some g(t)g(t), then f(t)=g(t)/tf(t)=g(t)/t.

Partial fractions. For a proper rational function N(s)/D(s)N(s)/D(s) (degree N<N < degree DD) with distinct simple poles at s=aks=a_k: cover-up rule gives residue Ak=N(ak)/D′(ak)A_k = N(a_k)/D'(a_k), so F(s)=∑Ak/(s−ak)F(s)=\sum A_k/(s-a_k) and f(t)=∑Akeaktf(t)=\sum A_k e^{a_k t}.

Question Archetypes

ArchetypeYou are seeing this when…
inverse-laplaceGiven F(s)F(s); find f(t)=L−1{F(s)}f(t)=\mathcal{L}^{-1}\{F(s)\} via partial fractions, shift theorems, or log-derivative

inverse-laplace (2 question(s); 2015, 2018)

Recognition Cues

Solution Template

  1. Split F(s)F(s) into pieces, one per tool.
  2. For rational pieces: check degree (proper = numerator degree << denominator degree). Factor denominator; apply cover-up rule for residues; invert.
  3. For e−asG(s)e^{-as}G(s) pieces: identify g(t)=L−1{G(s)}g(t)=\mathcal{L}^{-1}\{G(s)\}; answer is g(t−a)u(t−a)g(t-a)u(t-a).
  4. For logarithm pieces: differentiate F(s)F(s); recognise −F′(s)-F'(s) as a standard transform; divide by tt.
  5. Combine and box the answer.

Worked Example

2018 Paper 1, 2018-P1-Q5d-ii (5 marks)

Find the inverse Laplace transform of 5s2+3s−16(s−1)(s−2)(s+3)\dfrac{5s^2+3s-16}{(s-1)(s-2)(s+3)}.

Step 1 — Partial fractions. Degree of numerator (2) << degree of denominator (3): no polynomial part.

5s2+3s−16(s−1)(s−2)(s+3)=As−1+Bs−2+Cs+3.\frac{5s^2+3s-16}{(s-1)(s-2)(s+3)} = \frac{A}{s-1}+\frac{B}{s-2}+\frac{C}{s+3}.

Cover-up rule:

A=5(1)2+3(1)−16(1−2)(1+3)=−8−4=2.A = \frac{5(1)^2+3(1)-16}{(1-2)(1+3)} = \frac{-8}{-4} = 2.

B=5(4)+3(2)−16(2−1)(2+3)=105=2.B = \frac{5(4)+3(2)-16}{(2-1)(2+3)} = \frac{10}{5} = 2.

C=5(9)+3(−3)−16(−4)(−5)=2020=1.C = \frac{5(9)+3(-3)-16}{(-4)(-5)} = \frac{20}{20} = 1.

Step 2 — Invert. Using L−1{1/(s−a)}=eat\mathcal{L}^{-1}\{1/(s-a)\}=e^{at}:

  L−1 ⁣{5s2+3s−16(s−1)(s−2)(s+3)}=2et+2e2t+e−3t.  \boxed{\;\mathcal{L}^{-1}\!\left\{\frac{5s^2+3s-16}{(s-1)(s-2)(s+3)}\right\} = 2e^{t}+2e^{2t}+e^{-3t}.\;}


2015 Paper 1, 2015-P1-Q7a-i (6 marks)

Obtain the inverse Laplace transform of ln⁡ ⁣(1+1s2)+ss2+25 e−πs\ln\!\left(1+\dfrac{1}{s^2}\right)+\dfrac{s}{s^2+25}\,e^{-\pi s}.

Split into two pieces.

Piece 1: L−1 ⁣{ss2+25e−πs}\mathcal{L}^{-1}\!\left\{\dfrac{s}{s^2+25}e^{-\pi s}\right\}.

Standard pair: L−1 ⁣{ss2+25}=cos⁡5t\mathcal{L}^{-1}\!\left\{\dfrac{s}{s^2+25}\right\}=\cos 5t.

Second-shift theorem with a=πa=\pi:

L−1 ⁣{ss2+25e−πs}=cos⁡(5(t−π)) u(t−π).\mathcal{L}^{-1}\!\left\{\frac{s}{s^2+25}e^{-\pi s}\right\} = \cos(5(t-\pi))\,u(t-\pi).

Simplify: cos⁡(5t−5π)=cos⁡5tcos⁡5π=−cos⁡5t\cos(5t-5\pi)=\cos 5t\cos 5\pi=-\cos 5t (since cos⁡5π=cos⁡π=−1\cos 5\pi=\cos\pi=-1).

So Piece 1 =−cos⁡(5t) u(t−π)= -\cos(5t)\,u(t-\pi).

Piece 2: L−1 ⁣{ln⁡ ⁣(1+1s2)}=L−1 ⁣{ln⁡s2+1s2}\mathcal{L}^{-1}\!\left\{\ln\!\left(1+\dfrac{1}{s^2}\right)\right\} = \mathcal{L}^{-1}\!\left\{\ln\dfrac{s^2+1}{s^2}\right\}.

Let F(s)=ln⁡(s2+1)−ln⁡(s2)F(s)=\ln(s^2+1)-\ln(s^2). Differentiate:

F′(s)=2ss2+1−2s.F'(s) = \frac{2s}{s^2+1}-\frac{2}{s}.

So −F′(s)=2s−2ss2+1=L{2}−L{2cos⁡t}=L{2−2cos⁡t}-F'(s)=\dfrac{2}{s}-\dfrac{2s}{s^2+1}=\mathcal{L}\{2\}-\mathcal{L}\{2\cos t\}=\mathcal{L}\{2-2\cos t\}.

Since L{tf(t)}=−F′(s)\mathcal{L}\{tf(t)\}=-F'(s), we have tf(t)=2−2cos⁡ttf(t)=2-2\cos t, so f(t)=2(1−cos⁡t)tf(t)=\dfrac{2(1-\cos t)}{t}.

L−1 ⁣{ln⁡ ⁣(1+1s2)}=2(1−cos⁡t)t.\mathcal{L}^{-1}\!\left\{\ln\!\left(1+\frac{1}{s^2}\right)\right\} = \frac{2(1-\cos t)}{t}.

Combine:

  L−1 ⁣{ln⁡ ⁣(1+1s2)+ss2+25e−πs}=2(1−cos⁡t)t−cos⁡(5t) u(t−π).  \boxed{\;\mathcal{L}^{-1}\!\left\{\ln\!\left(1+\frac{1}{s^2}\right)+\frac{s}{s^2+25}e^{-\pi s}\right\} = \frac{2(1-\cos t)}{t} - \cos(5t)\,u(t-\pi).\;}

Common Traps


Marks-Aware Writing

5-mark question (2018): Three residues (1 mark each) plus inversion and boxed answer (2 marks). Each cover-up computation should show the numerator evaluated at the pole and the denominator product; do not just write the answer.

6-mark question (2015): Two pieces of roughly equal weight. For the second-shift piece: state the standard pair, apply the theorem, simplify the cosine expression (2–3 marks). For the log piece: differentiate, recognise −F′(s)-F'(s), divide by tt (2–3 marks). Combine clearly.

Practice Set

YearPaper/QMarksOne-line hint
2023P1-Q5b10Inversion via Frullani/integral-property; after proving the identity, evaluate ∫0∞F(p) dp\int_0^\infty F(p)\,dp
2020P1-Q7b10After solving for Y(s)=1/s+C/(s+2)2Y(s)=1/s+C/(s+2)^2, invert using L−1{1/(s+2)2}=te−2t\mathcal{L}^{-1}\{1/(s+2)^2\}=te^{-2t}
2025P1-Q6a15After solving Y=(s2+1)/s4Y=(s^2+1)/s^4, invert termwise: L−1{1/s2}=t\mathcal{L}^{-1}\{1/s^2\}=t, L−1{1/s4}=t3/6\mathcal{L}^{-1}\{1/s^4\}=t^3/6
2016P1-Q6d10Partial fractions with possibly repeated roots; cover-up for simple poles, differentiation for repeated

Ready to drill what you just read?

Daily Practice turns these patterns into one adaptive set a day — practised daily until they're automatic, free for everyone.

See Daily Practice →

This chapter is part of the Maths Coverage Map — 14 years, mapped. Get the take-away PDF free.