T = 2π · √(L/g)
A simple pendulum swings more slowly as its length grows when the swing is small. The bob's mass cancels out.
A simple pendulum swings more slowly as its length grows when the swing is small. The bob's mass cancels out.
Select a target and calculate.
A simple pendulum swings more slowly as its length grows when the swing is small. The bob's mass cancels out.
At L = 1.00 m and g = 9.80665 m/s², one full swing takes T = 2π√(1/9.80665) = 2.006 s.
Point-like bob on a massless, inextensible string; small swing angle, no pivot friction or air drag. At larger swings the actual period also depends on the starting angle, and this approximation underestimates it.
How long must a pendulum be to take two seconds for one full swing? This calculator relates its length to the time for a complete out-and-back motion.
The model uses a small bob on a light string. Gravity pulls it back toward its resting position. At small angles this restoring effect is nearly proportional to the angle, so the motion is approximately harmonic: T = 2π√(L/g). T is the period, L the pivot-to-centre-of-mass distance and g local gravitational acceleration. The bob mass cancels out.
T = 2π · √(L/g)
Period: T = 2π√(L/g)Required length: L = g(T/2π)²Gravity from measurement: g = L(2π/T)²| Symbol / input | Meaning |
|---|---|
| Oscillation period T | Time for one complete out-and-back swing, for example from one left turning point to the next. Time several swings and divide by their count; a seconds pendulum has a period near 2 s. |
| Pendulum length L | Distance from the pivot to the bob's centre of mass, not just the free string length. Measure it from the geometry; classroom pendulums are often about 0.2 to 2 m long. |
| Gravitational acceleration g | Local gravitational acceleration; about 9.81 m/s² on Earth. Use the local value for precision measurements. |
Measure L in metres from the pivot to the bob's centre of mass; the string length alone can be too short. Lengths of 0.2 to 2 m are practical for a demonstration. On Earth g is approximately 9.81 m/s²; obtain a precise local value from a survey or measurement. To infer T, time several complete swings and divide by their number.
Enter length and gravity to calculate T. A complete swing ends at the same turning point where it started. Choose L to find the required length, or g to estimate local gravity from measured length and period.
At L = 1.00 m and g = 9.80665 m/s², T = 2π√(1/9.80665) = 2.006 s per full swing. Ten full swings take about 20.06 s. Four times the length doubles T to 4.012 s.
The period grows with the square root of length: doubling length multiplies the period by about 1.41. This is a small-angle approximation; a large starting angle gives a longer period.
Calculations use metres, seconds and m/s² internally. Offered length units are converted to metres first. T is the time for one complete swing, not the time from one extreme to the opposite extreme.
Planning and checking demonstration pendulums, estimating swing times in simple experiments, and checking a gravity measurement made with a pendulum.
The bob is treated as a point mass on a massless, inextensible string with a fixed pivot and small swing angle. Pivot friction and air drag are excluded. Precision clocks, large swings and extended rigid bodies require a more detailed model.
Common mistake: Common errors are measuring only the string instead of the pivot-to-centre distance, or counting half a swing as T. At large amplitudes the formula underestimates the period; bob mass is not a correction factor.
Planning and checking demonstration pendulums, estimating swing times in simple experiments, and checking a gravity measurement made with a pendulum.
Measure L in metres from the pivot to the bob's centre of mass; the string length alone can be too short. Lengths of 0.2 to 2 m are practical for a demonstration. On Earth g is approximately 9.81 m/s²; obtain a precise local value from a survey or measurement. To infer T, time several complete swings and divide by their number.
The bob is treated as a point mass on a massless, inextensible string with a fixed pivot and small swing angle. Pivot friction and air drag are excluded. Precision clocks, large swings and extended rigid bodies require a more detailed model.