Laplace Inversion and Initial-Value Problems

Solve transformed algebra and reconstruct the time response by recognizable pairs.

Builds on Laplace Transforms and Their Domain

The bigger question: Can we turn a changing-time problem into algebra?

On this page

The idea

Laplace methods move differentiation into algebra while retaining initial data. The difficult step is often inversion: rewrite the rational expression into known transform pairs, using partial fractions or completing a square.

Visual guide

VISUAL GUIDEInitial data select a damped oscillation
The transform 1/((s + 1)² + 1) inverts to e⁻ᵗ sin t. The exponential envelope bounds the oscillation, while the graph starts at zero with slope one, matching the initial-value problem.0-1.22-0.64060.681.2ty
  • e⁻ᵗ sin t
  • Upper envelope
  • Lower envelope
The transform 1/((s + 1)² + 1) inverts to e⁻ᵗ sin t. The exponential envelope bounds the oscillation, while the graph starts at zero with slope one, matching the initial-value problem.

Method and assumptions

Transform both sides, substitute every initial value, solve for Y(s)Y(s), decompose and invert term by term. Finally check the initial data and at least one substitution in the original equation. A correct algebraic transform can still be inverted with an incorrect numerator.

Worked example: first-order response

For y′+2y=3y'+2y=3, y(0)=1y(0)=1, (s+2)Y=1+3/s(s+2)Y=1+3/s. Thus Y=3/(2s)−1/[2(s+2)]Y=3/(2s)-1/[2(s+2)] and y=3/2−e−2t/2y=3/2-e^{-2t}/2. At t=0t=0 it equals 11 and its steady value is 3/23/2.

PAUSE & THINKA quick check, not a grade

Try it yourself.

Choose an answer and explain your reasoning to yourself. Use a hint if you get stuck.

Which time function has transform 1/(s+2)?

Hint 1 · Find a starting point

Use ℒ{eᵃᵗ}=1/(s−a).

Hint 2 · Take the next step

Here a=−2.

Show the reasoning

Answer: e⁻²ᵗ

The inverse is e⁻²ᵗ for t≥0, with transform defined for Re(s)>−2.

Before moving on: what would make one of the other answers wrong? Saying why is part of understanding.

Worked example: damped oscillation

For y′′+2y′+2y=0y''+2y'+2y=0, y(0)=0,y′(0)=1y(0)=0,y'(0)=1, Y=1/(s2+2s+2)=1/[(s+1)2+1]Y=1/(s^2+2s+2)=1/[(s+1)^2+1]. The inverse is e−tsin⁡te^{-t}\sin t, which has the required initial slope.

Interpreting the result

A shift in ss produces an exponential in time. A factor e−ase^{-as} produces a time delay instead; these are different transform rules. Repeated poles require terms for each power in partial fractions.

Practice

  1. Invert 1/[s(s+1)]1/[s(s+1)].
  2. Invert 1/(s+2)21/(s+2)^2.
  3. Invert (s+1)/[(s+1)2+4](s+1)/[(s+1)^2+4].
Show worked solutions
  1. 1/s−1/(s+1)1/s-1/(s+1) gives 1−e−t1-e^{-t}.
  2. te−2tte^{-2t}.
  3. e−tcos⁡2te^{-t}\cos2t.

Further study

MIT OpenCourseWare: Differential Equations provides a full university course with additional lectures and exercises.

MAKE IT YOURS

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