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The Laplace transform

The Laplace transform turns differential equations into algebra. It is the engineer's favourite tool for circuits, control systems, and switched inputs.

Definition

The Laplace transform of \(f(t)\) is \(F(s) = \mathcal{L}\{f\} = \int_0^\infty e^{-st}f(t)\,dt\), defined for values of \(s\) where the integral converges. It converts a function of time \(t\) into a function of a new variable \(s\). For \(f = 1\), \(\mathcal{L}\{1\} = \frac{1}{s}\) for \(s > 0\).

\mathcal{L}\{f\}(s) = \int_0^\infty e^{-st} f(t)\,dt

A table of basic transforms

\(\mathcal{L}\{e^{at}\} = \frac{1}{s - a}\); \(\mathcal{L}\{t^n\} = \frac{n!}{s^{n+1}}\); \(\mathcal{L}\{\sin bt\} = \frac{b}{s^2 + b^2}\); \(\mathcal{L}\{\cos bt\} = \frac{s}{s^2 + b^2}\). Most problems are solved by combining these entries with a few rules, rather than by integrating directly.

Linearity

\(\mathcal{L}\{af + bg\} = aF + bG\). So \(\mathcal{L}\{3e^{2t} - 4\sin t\} = \frac{3}{s - 2} - \frac{4}{s^2 + 1}\). Linearity is what makes transforms practical.

Transforms of derivatives

Integration by parts gives \(\mathcal{L}\{f'\} = sF(s) - f(0)\) and \(\mathcal{L}\{f''\} = s^2F(s) - sf(0) - f'(0)\). Differentiation in \(t\) becomes multiplication by \(s\), and the initial conditions are built in automatically. This is the key to solving initial value problems.

\mathcal{L}\{y''\} = s^2Y - sy(0) - y'(0)

The shifting theorem

Multiplying by an exponential shifts the transform: \(\mathcal{L}\{e^{at}f(t)\} = F(s - a)\). So \(\mathcal{L}\{e^{-2t}\cos 3t\} = \frac{s + 2}{(s + 2)^2 + 9}\). This handles damped oscillations directly.

Existence

The transform exists for functions that are piecewise continuous and of exponential order, meaning \(|f(t)| \le Me^{ct}\) for large \(t\). Almost every function in applications qualifies, though \(e^{t^2}\) grows too fast to have a Laplace transform.

Worked example: computing a transform

Find \(\mathcal{L}\{te^{3t}\}\). From the table, \(\mathcal{L}\{t\} = \frac{1}{s^2}\). Shifting by \(a = 3\) gives \(\frac{1}{(s - 3)^2}\). Rules plus a table replace a page of integration by parts.

Common mistakes

Forgetting initial conditions in the derivative formulas. Mixing up the sine and cosine entries (sine has \(b\) on top; cosine has \(s\)). Shifting in the wrong direction: \(e^{at}\) gives \(s - a\), not \(s + a\).

Key takeaways

The Laplace transform \(\int_0^\infty e^{-st}f(t)\,dt\) converts time functions to \(s\)-functions. Use a table and rules: linearity, derivative formulas that include initial conditions, and the shift \(e^{at}f \to F(s - a)\). Derivatives become multiplication by \(s\), turning ODEs into algebra.

Flashcard

\mathcal{L}\{f\} = \int_0^\infty e^{-st}f\,dt

Laplace transform

Converts t to s.

Check your understanding

What is the Laplace transform of e^(5t)?

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