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Recipe

Compute the L¹, L², and L∞ norms of a function

Use when: you have an explicit, possibly piecewise, formula for f on an interval and need one or more of its three norms

Goal: exact values for \lVert f\rVert_1, \lVert f\rVert_2, and \lVert f\rVert_\infty, computed directly from f's formula

Taught in The L1, L2, and L∞ norms compared

  1. 1

    Write f piecewise if a single formula doesn't cover the whole interval, and mark where each piece is positive, negative, or zero.

    Example

    Let f(t)=2 for |t|\le1.5 and f(t)=0 for 1.5<|t|\le\pi. There are two pieces: constant 2 on [-1.5,1.5], and 0 elsewhere.

    Why: \lVert f\rVert_1 needs |f|, and getting each piece's sign right is what "integrating |f|" actually means in practice.

  2. 2

    On each piece, integrate |f|, not f itself, then add the pieces together.

    Example

    On [-1.5,1.5], f=2\ge0, so \lVert f\rVert_1=\displaystyle\int_{-1.5}^{1.5}2\,dt=2(3)=6. The zero piece contributes nothing.

    • f never changes sign on a piece — integrate f (or -f) directly, whichever is nonnegative there.
    • f changes sign inside one piece — split that piece at the sign change first, then integrate each half separately.

    Why: \lVert f\rVert_1 is defined as \int|f|, so skipping the absolute value silently cancels area that should add.

  3. 3

    Square f first; this removes the sign issue automatically. Integrate over each piece, add the results, then take the square root.

    Example

    \displaystyle\int_{-1.5}^{1.5}2^2\,dt=4(3)=12, so \lVert f\rVert_2=\sqrt{12}=2\sqrt3\approx3.464.

    ⚡ Shortcut

    When f takes only the values 0 and one height h, f^2=h\cdot f on the nonzero piece. That gives \lVert f\rVert_2=\sqrt{h\cdot\lVert f\rVert_1}, with no separate integral needed. Here h=2 and \lVert f\rVert_1=6, so \sqrt{2\cdot6}=2\sqrt3, matching the long way exactly.

    Why: squaring makes every value nonnegative on its own, so the sign bookkeeping Step 2 required disappears completely.

  4. 4

    Scan each piece for its largest |f|-value, then take the largest across all pieces; that number is \lVert f\rVert_\infty.

    Example

    The two pieces have magnitudes 2 and 0; the larger is 2, so \lVert f\rVert_\infty=2.

    • f is piecewise-constant — the tallest constant piece's magnitude is the answer directly.
    • f varies continuously within a piece — find that piece's maximum with calculus (critical points and endpoints) before comparing across pieces.

    Why: the supremum is the tightest bound |f(t)| never exceeds, and one missed interior peak invalidates the whole answer.

Common mistakes

  • Integrating f directly instead of |f| when f is negative somewhere, which cancels area instead of adding it.
  • Reporting \sqrt{\int f\,dt} as \lVert f\rVert_2 instead of \sqrt{\int f^2\,dt}.
  • Assuming \lVert f\rVert_\infty only occurs at an interval endpoint and missing an interior peak.
  • Expecting \lVert f\rVert_\infty to grow when the interval widens, the way \lVert f\rVert_1 and \lVert f\rVert_2 do.