Small-Angle Period Correction Series
Extends the small-angle pendulum period to larger amplitudes by adding successive correction terms: T ≈ T₀·(1 + θ₀²/16 + 11θ₀⁴/3072 + …)
The equation
What it solves
Extends the small-angle pendulum period to larger amplitudes by adding successive correction terms: T ≈ T₀·(1 + θ₀²/16 + 11θ₀⁴/3072 + …). Each term is positive, so the true period is always longer than the small-angle approximation.
When to use it
When the amplitude is moderate (15°–60°) and you need more accuracy than the simple formula but do not want to evaluate the full elliptic integral. Two terms give < 0.1% error for θ₀ < 60°.
When NOT to use it
The series diverges (actually converges slowly) for angles approaching 180°. For θ₀ > 70°, use the complete elliptic integral expression for better accuracy.
Common mistakes
Using θ₀ in degrees instead of radians in the correction formula. Stopping at the first correction term and ignoring the second when the angle is above 30°. Applying the correction multiplicatively as a separate factor rather than multiplying the entire small-angle period by (1 + …).
Topics that use this equation
Problems using this equation
- [challenge] A pendulum of length L = 1.0 m is released from rest at θ₀ = 0.6 rad (~34°). This amplitude lies out…
- [easy] A simple pendulum of length L = 1.0 m is pulled to θ₀ = 30° (π/6 rad) and released from rest. The sm…
- [medium] A pendulum of length L = 1.5 m is released from θ₀ = 0.8 rad (≈ 45.8°). The period can be expanded a…
- [exam] A clock pendulum of length L = 1.0 m is pulled to θ₀ = 1.4 rad (≈ 80.2°) and released. (a) Compute t…