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Laplace of derivatives

The Laplace transform turns a derivative into an algebraic factor ss plus an initial-condition term. This is why Laplace transforms differential equations into algebraic equations that are easy to solve.

L{f′(t)}=sF(s)−f(0)\mathcal L\{f'(t)\} = sF(s) - f(0)transform of the first derivative
L{f′′(t)}=s2F(s)−sf(0)−f′(0)\mathcal L\{f''(t)\} = s^2F(s) - sf(0) - f'(0)transform of the second derivative

Symbols

F(s)F(s)the Laplace transform of f(t)

Example

Solve y′+3y=0y'+3y=0, y(0)=4y(0)=4: sY−4+3Y=0⇒Y(s)=4s+3sY-4+3Y=0 \Rightarrow Y(s)=\dfrac{4}{s+3}, so y=4e−3ty=4e^{-3t}.

Transform the whole equation, solve for Y(s)Y(s), then use a table backwards (inverse transform).
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Part of Laplace, Fourier and PDEs: The Laplace transform.