1 · Linearization, revisited
Near a, f(x) ≈ f(a) + f′(a)(x−a) = L(x). The tangent line is the degree-1 Taylor polynomial. Adding the next term gives a quadratic that hugs the curve longer; adding every term gives a series — not a polynomial, but something even more powerful.
2 · Higher-degree approximations
The Taylor polynomial of degree n at a is
Pₙ(x) = f(a) + f′(a)(x−a) + f″(a)(x−a)²/2! + ⋯ + f⁽ⁿ⁾(a)(x−a)ⁿ/n!
Each term irons out one more piece of local behavior: value, slope, curvature, jerk. More terms, wider trust region (usually).
3 · Taylor’s theorem and the remainder
If f is smooth, the error after n terms is
f(x) − Pₙ(x) = f⁽ⁿ⁺¹⁾(ξ)·(x−a)ⁿ⁺¹/(n+1)! for some ξ between x and a.
This Lagrange remainder is what lets us prove an approximation good before we trust it — not assert it.
Approximate e^{0.1} to 4 decimals. Use P₂(x) = 1 + x + x²/2 at x = 0.1: gives 1.10517. Remainder ≤ e^{ξ}(0.1)³/6 ≤ e^{0.1}(0.001)/6 ≈ 1.84×10⁻⁴. So the true value is 1.10517 ± 0.00018 — a guarantee, not a hope.
4 · Maclaurin series — Taylors at 0
Set a = 0 and you get the famous five:
eˣ = Σ xⁿ/n! · sin x = Σ (−1)ⁿx^{2n+1}/(2n+1)! · cos x = Σ (−1)ⁿx^{2n}/(2n)! · 1/(1−x) = Σ xⁿ (|x|<1) · ln(1+x) = Σ (−1)^{n−1}xⁿ/n.
Each is a polynomial machine that sums to a transcendental function inside its radius.
5 · Power series in general
A power series Σ cₙ(x−a)ⁿ converges inside an interval centered at a, diverges outside, and needs checking at the endpoints. Differentiating or integrating term-by-term inside the interval stays valid — a calculus superpower we'll exploit in Chapter 26.
Pₙ(x) = Σ_{k=0}^{n} f⁽ᵏ⁾(a)(x−a)ᵏ/k!
Rem. |f(x) − Pₙ(x)| ≤ M·|x−a|ⁿ⁺¹/(n+1)! (M = max |f⁽ⁿ⁺¹⁾|)
Maclaurin: sin x ≈ x − x³/6 + x⁵/120 · cos x ≈ 1 − x²/2 + x⁴/24
eˣ ≈ 1 + x + x²/2 + x³/6 · ln(1+x) ≈ x − x²/2 + x³/3 · 1/(1−x) ≈ 1 + x + x² + ⋯
Common mistakes
- Forgetting the /k! — the factorial is not optional decoration, it’s the slope correction per order.
- Mismatching center: an a=0 series cannot approximate well around a=2 unless you shift.
- Claiming series = function everywhere, even though endpoints/radius may forbid it.
- Confusing linearization (degree-1 Taylor) with differentials (dy) — related but not identical.
- Using eˣ’s series where |x|≫1; the polynomials may oscillate wildly outside a modest interval.