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Small-angle period T0 = 2π√(l/g)
2.006409
seconds (amplitude-independent)
Amplitude α (°) Exact period T (s) Approx T0 (s) Ratio T/T0
5 2.007365 2.006409 1.000476
10 2.010236 2.006409 1.001907
15 2.015038 2.006409 1.004301
20 2.021796 2.006409 1.007669
25 2.030548 2.006409 1.012031
30 2.041338 2.006409 1.017409
35 2.054229 2.006409 1.023833
40 2.069291 2.006409 1.031341
45 2.086612 2.006409 1.039973
50 2.106294 2.006409 1.049783
55 2.128458 2.006409 1.060829
60 2.153242 2.006409 1.073182
65 2.180811 2.006409 1.086922
70 2.211354 2.006409 1.102145
75 2.24509 2.006409 1.118959
80 2.282276 2.006409 1.137493
85 2.323211 2.006409 1.157895
90 2.368246 2.006409 1.180341
95 2.417797 2.006409 1.205037
100 2.472356 2.006409 1.232229
105 2.532513 2.006409 1.262212
110 2.598982 2.006409 1.29534
115 2.672637 2.006409 1.33205
120 2.75456 2.006409 1.372881
125 2.846117 2.006409 1.418513
130 2.949059 2.006409 1.469819
135 3.065688 2.006409 1.527948
140 3.199111 2.006409 1.594446
145 3.353671 2.006409 1.671479
150 3.535702 2.006409 1.762204
155 3.754993 2.006409 1.871499
160 4.027882 2.006409 2.007507
165 4.384894 2.006409 2.185444
170 4.89436 2.006409 2.439363
175 5.773771 2.006409 2.877664

As α → 180° the elliptic modulus k → 1 and the period diverges; the table stops just below 180°.

What this calculator does

A simple pendulum's familiar period formula, \(T_0 = 2\pi\sqrt{l/g}\), is only an approximation valid for tiny swings. For finite release angles the real pendulum swings slower. This tool computes the exact period using the complete elliptic integral of the first kind and tabulates it next to the small-angle value and their ratio across a range of amplitude angles.

How to use it

Enter the string length l in meters and the gravitational acceleration g in m/s² (the default 9.80665 is standard gravity). Choose an amplitude step of 5° or 10°. The result shows the constant small-angle period T0 as the headline value, then a row for every amplitude α from the step up to just below 180°, with the exact period T and the ratio T/T0.

The formula explained

The exact period is $$T = 4\sqrt{\frac{l}{g}}\cdot K(k)$$ where \(k = \sin(\alpha/2)\) is the elliptic modulus and $$K(k) = \int_0^{\pi/2} \frac{d\varphi}{\sqrt{1-k^2\sin^2\varphi}}.$$ We evaluate K with the fast, exact arithmetic–geometric mean (AGM): start \(a_0=1\), \(b_0=\cos(\alpha/2)\), iterate \(a_{n+1}=(a_n+b_n)/2\) and \(b_{n+1}=\sqrt{a_n b_n}\) until they converge, then \(K = \pi/(2a_\infty)\). The ratio simplifies to \(\frac{2}{\pi}K(\sin(\alpha/2))\), which is 1 at zero amplitude and diverges as α approaches 180°.

Curve showing period ratio rising above 1 as amplitude increases, with small-angle line flat at 1
The exact period grows above the small-angle value T0 as amplitude increases.
Pendulum swinging from a pivot showing amplitude angle alpha, length l, and gravity g
A simple pendulum of length l swinging with amplitude alpha under gravity g.

Worked example

For l = 1 m and g = 9.80665 m/s²: \(\sqrt{l/g} = 0.319330\) s, so \(T_0 = 2.006419\) s. At \(\alpha = 30°\), \(k = \sin 15° = 0.258819\), \(K = 1.598142\), giving \(T = 2.041253\) s and ratio \(1.017362\) — about 1.74% longer than the small-angle estimate, matching the textbook \(1 + \alpha^2/16\) correction.

FAQ

Why does the period grow with amplitude? The restoring torque is proportional to \(\sin\theta\), not \(\theta\); for larger swings \(\sin\theta < \theta\), so the effective restoring force is weaker and each cycle takes longer.

Why does it stop before 180°? At exactly 180° the pendulum starts at the unstable inverted point, \(k = 1\), and K diverges to infinity, so the period is unbounded. The table caps just below 180°.

Is the AGM exact? It converges quadratically to machine precision in under ten iterations, so the tabulated values are exact to the displayed precision — far better than truncating the power series.

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