Laplace Transforms and Their Domain

Compute elementary transforms and retain the initial-value terms in derivatives.

Builds on Frequency Response and RLC Models

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

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The idea

The one-sided Laplace transform packages a function on t≥0t\ge0 into F(s)=∫0∞e−stf(t)dtF(s)=\int_0^\infty e^{-st}f(t)dt. Exponential weighting makes many growing functions integrable for sufficiently large real ss. Linearity turns sums of inputs into sums of transforms.

Visual guide

VISUAL GUIDEThe exponential weight can overcome growth
For f(t) = e²ᵗ, the transform integrand is e⁻⁽ˢ⁻²⁾ᵗ. At s = 3 it decays and integrates to 1; at s = 2 it stays at 1 and has infinite area. The convergence condition s > 2 matters.001.250.3252.50.653.750.97551.3tintegrand
  • s = 3: e⁻ᵗ
  • s = 2: constant 1
For f(t) = e²ᵗ, the transform integrand is e⁻⁽ˢ⁻²⁾ᵗ. At s = 3 it decays and integrates to 1; at s = 2 it stays at 1 and has infinite area. The convergence condition s > 2 matters.

Method and assumptions

For piecewise continuous functions of exponential order, the transform exists in a right half-plane. Useful pairs include 1↔1/s1\leftrightarrow1/s, eat↔1/(s−a)e^{at}\leftrightarrow1/(s-a), sin⁡bt↔b/(s2+b2)\sin bt\leftrightarrow b/(s^2+b^2) and cos⁡bt↔s/(s2+b2)\cos bt\leftrightarrow s/(s^2+b^2). Integration by parts gives L[y′]=sY−y(0)\mathcal L[y']=sY-y(0).

Worked example: an exponential

L[e2t]=∫0∞e−(s−2)tdt=1/(s−2)\mathcal L[e^{2t}]=\int_0^\infty e^{-(s-2)t}dt=1/(s-2) for s>2s>2. The expression alone does not record the convergence condition; the integral diverges when s≤2s\le2.

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.

If Y(s)=ℒ{y(t)}, what is ℒ{y′(t)}?

Hint 1 · Find a starting point

Integration by parts leaves a boundary term.

Hint 2 · Take the next step

The initial value appears with a minus sign.

Show the reasoning

Answer: sY(s)−y(0)

ℒ{y′}=sY−y(0), under the transform’s existence conditions. Omitting y(0) changes an initial-value problem.

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

Worked example: a second derivative

Apply the derivative rule twice: L[y′′]=s2Y−sy(0)−y′(0)\mathcal L[y'']=s^2Y-sy(0)-y'(0). For y=cos⁡ty=\cos t, this is s3/(s2+1)−s=−s/(s2+1)s^3/(s^2+1)-s=-s/(s^2+1), matching the transform of −cos⁡t-\cos t.

Interpreting the result

Derivative formulas require suitable regularity and growth. Keep initial terms until after substituting the stated values. Losing them replaces the intended initial-value problem with a different one.

Practice

  1. Find the transform of 3+2e−t3+2e^{-t}.
  2. Find the transform of tt.
  3. What is L[y′]\mathcal L[y'] if y(0)=4y(0)=4?
Show worked solutions
  1. 3/s+2/(s+1)3/s+2/(s+1) for s>0s>0.
  2. 1/s21/s^2 for s>0s>0, by integration by parts.
  3. sY−4sY-4.

Further study

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

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