Taylor Series

Work in progress. This note is still being written and incomplete.

If f(z)f(z) is analytic at z=αz = \alpha, the series

∑n=0∞f(n)(α)n!(z−α)n=f(α)+f′(α)(z−α)+f′′(α)2!(z−α)2+⋯\sum_{n=0}^{\infty} \frac{f^{(n)}(\alpha)}{n!}(z-\alpha)^n = f(\alpha) + f'(\alpha)(z-\alpha) + \frac{f''(\alpha)}{2!}(z-\alpha)^2 + \cdots

is called the Taylor series of f(z)f(z) centered at α\alpha. When α=0\alpha = 0, it is called the Maclaurin series of f(z)f(z).

Taylor’s Theorem

Let ff be analytic in a domain GG, and let the disk DR(α)D_R(\alpha) be contained in GG. Then the Taylor series of ff centered at α\alpha converges to f(z)f(z) for all z∈DR(α)z \in D_R(\alpha).

f(z)=∑n=0∞f(n)(α)n!(z−α)n,z∈DR(α)f(z) = \sum_{n=0}^{\infty} \frac{f^{(n)}(\alpha)}{n!}(z-\alpha)^n, \quad z \in D_R(\alpha)

The convergence is uniform on every closed disk {z:∣z−α∣≤r}\{z : |z-\alpha| \le r\} with 0<r<R0 < r < R.

Radius from Singular Points

Let ff be analytic in a domain GG containing α\alpha. Let z0z_0 be a nearest singular point of ff to α\alpha, and let R=∣z0−α∣R = |z_0 - \alpha|.

  • The Taylor series of ff centered at α\alpha converges to f(z)f(z) for each z∈DR(α)z \in D_R(\alpha).
  • No disk centered at α\alpha with a radius larger than RR can be a disk on which the series represents ff.

Uniqueness

Suppose

f(z)=∑n=0∞an(z−α)n=∑n=0∞bn(z−α)nf(z) = \sum_{n=0}^{\infty} a_n (z-\alpha)^n = \sum_{n=0}^{\infty} b_n (z-\alpha)^n

in some disk Dr(α)D_r(\alpha) with r>0r > 0. Then an=bna_n = b_n for each n∈N∪{0}n \in \mathbb{N} \cup \{0\}.

Any power series representation of f(z)f(z) in a disk centered at α\alpha is automatically the Taylor series of ff centered at α\alpha.

Examples:

  • 1(1−z)2=∑n=0∞(n+1)zn\frac{1}{(1-z)^2} = \sum_{n=0}^{\infty} (n+1) z^n is valid for z∈D1(0)z \in D_1(0)
  • sin⁡z=∑n=0∞(−1)nz2n+1(2n+1)!\sin z = \sum_{n=0}^{\infty} \frac{(-1)^n z^{2n+1}}{(2n+1)!}

Worked Examples

Maclaurin Series of Sine

Find the Maclaurin series of sin⁡z\sin z.

The derivatives at 00 cycle through sin⁡z,cos⁡z,−sin⁡z,−cos⁡z\sin z, \cos z, -\sin z, -\cos z, so

f(0)=0,f′(0)=1,f′′(0)=0,f′′′(0)=−1,…f(0) = 0, \quad f'(0) = 1, \quad f''(0) = 0, \quad f'''(0) = -1, \quad \ldots

Only odd powers survive.

sin⁡z=∑n=0∞(−1)nz2n+1(2n+1)!\sin z = \sum_{n=0}^{\infty} \frac{(-1)^n z^{2n+1}}{(2n+1)!}

sin⁡z\sin z is entire, so the series is valid for all zz.

Series by Differentiation

Show that 1(1−z)2=∑n=0∞(n+1)zn\frac{1}{(1-z)^2} = \sum_{n=0}^{\infty} (n+1) z^n for z∈D1(0)z \in D_1(0).

Start with the geometric series.

11−z=∑n=0∞zn,∣z∣<1\frac{1}{1-z} = \sum_{n=0}^{\infty} z^n, \quad |z| < 1

Differentiate both sides term by term.

1(1−z)2=∑n=1∞nzn−1=∑n=0∞(n+1)zn\frac{1}{(1-z)^2} = \sum_{n=1}^{\infty} n z^{n-1} = \sum_{n=0}^{\infty} (n+1) z^n

The only singular point is z=1z = 1, so R=1R = 1.

Series Centered at a Nonzero Point

Find the Taylor series of 1z\frac{1}{z} centered at α=1\alpha = 1 and its disk of validity.

Write z=1+(z−1)z = 1 + (z-1).

1z=11+(z−1)=∑n=0∞(−1)n(z−1)n\frac{1}{z} = \frac{1}{1 + (z-1)} = \sum_{n=0}^{\infty} (-1)^n (z-1)^n

The geometric series converges for ∣z−1∣<1|z-1| < 1. The nearest singular point is 00, so R=∣0−1∣=1R = |0 - 1| = 1 and the disk is D1(1)D_1(1).

Series Valid in a Disk

Find the Taylor series of 1z+2\frac{1}{z+2} centered at 00 and its disk of validity.

1z+2=12⋅11+z2=∑n=0∞(−1)nzn2n+1\frac{1}{z+2} = \frac{1}{2} \cdot \frac{1}{1 + \frac{z}{2}} = \sum_{n=0}^{\infty} \frac{(-1)^n z^n}{2^{n+1}}

The nearest singular point is −2-2, so R=2R = 2 and the disk is D2(0)D_2(0).

Coefficients from Uniqueness

Find a0,…,a4a_0, \ldots, a_4 if ∑n=0∞anzn=ez+z2\sum_{n=0}^{\infty} a_n z^n = e^z + z^2 near 00.

By uniqueness, the ana_n are the Taylor coefficients of ez+z2e^z + z^2.

ez+z2=1+z+(12+1)z2+z36+z424+⋯e^z + z^2 = 1 + z + \left(\frac{1}{2} + 1\right) z^2 + \frac{z^3}{6} + \frac{z^4}{24} + \cdots a0=1,a1=1,a2=32,a3=16,a4=124a_0 = 1, \quad a_1 = 1, \quad a_2 = \frac{3}{2}, \quad a_3 = \frac{1}{6}, \quad a_4 = \frac{1}{24}

Polynomial Times Cosine

Find the Maclaurin series of z2cos⁡zz^2 \cos z and its radius of convergence.

z2cos⁡z=z2∑n=0∞(−1)nz2n(2n)!=∑n=0∞(−1)nz2n+2(2n)!z^2 \cos z = z^2 \sum_{n=0}^{\infty} \frac{(-1)^n z^{2n}}{(2n)!} = \sum_{n=0}^{\infty} \frac{(-1)^n z^{2n+2}}{(2n)!}

z2cos⁡zz^2 \cos z is entire, so R=∞R = \infty.

Written by October 6, 2026 2 min read
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