Example 1
l = 1 m, blank g.
This is the school model: a point mass on a massless string, small angle, no drag. The formula matches the practical pendulum page, T = 2π√(l/g). l = 1 m and blank g give T ≈ 2.01 s.
Swing and clock version: pendulum period. From T you get f on frequency from period and ω on angular velocity.
Length l (m) and g (m/s², optional). The result shows up here.
A simple pendulum is a school contract: mass at a point, string or rod with no mass of its own, motion in one plane, no friction, small angle. Under those assumptions T = 2π√(l/g). l = 1 m and g = 9.81 m/s² give T ≈ 2.01 s, the same numbers as the practical page.
The l field is string length in meters. g is optional, and blank means 9.81. There is no mass field, because T does not depend on m in this model. Amplitude stays out too, as long as the angle is small and sin θ ≈ θ.
At a large angle the harmonic model breaks and the period grows. A real string with mass, or a bob with a visible radius, is a physical pendulum: moment of inertia and center of mass enter, a different formula, a different page outside this set.
l = 0.5 m at 9.81 shortens T to about 1.42 s. l = 4 m stretches it to about 4.01 s, twice the 1 m period. On the Moon, l = 1 m and g = 1.62 give about 4.94 s. A comma and a period both parse.
Type l, leave g blank or enter your own, then Calculate. The calculator example is 1 m and blank g. For a swing or a clock without the assumption list, go back to the practical pendulum. f = 1/T is on the neighbouring page, with the same T.
A spring computes f from k and m, not from length and g. Swapping l for k does not work. ω = 2π/T from this period sits on angular velocity.
T = 2π √(l/g)
Assumptions: small angle, point mass, massless string, no drag.
School model: point mass, massless string, small angle. T = 2π√(l/g) at l = 1 m and blank g is again ≈ 2.01 s, but the length letter is l, not L.
l = 1 m, blank g.
l = 0.5 m.
l = 2 m.
l = 0.8 m.
l = 1 m, g = 1.62.
l = 0.25 m.
l = 1 m, g = 9.81.
l = 1.2 m.
l = 0.1 m.
l = 3 m.
An ideal model: point mass, massless string, small angle, no drag. The formula is T = 2π√(l/g).
About 2.01 s. l = 0.5 m shortens T to about 1.42 s. Mass does not enter.
Same formula. That page has playground and clock examples. Here you get the assumption list a teacher wants to hear.
At small θ, sin θ ≈ θ and the motion is harmonic. At large angles the period grows.
No. In the simple model T depends on l and g, not on m.
f = 1/T on frequency from period. ω = 2π/T on angular velocity. From 2.01 s that is about 0.50 Hz and 3.13 rad/s.
Not in this model. A physical pendulum uses the center of mass and the moment of inertia, a different formula.
Like the square root of l. l = 4 m is about 4.01 s, twice the period at 1 m.
Here T comes from length and g. A spring gets f from k and m. Putting l where k belongs does nothing useful.
Yes. 1,2 and 1.2 are the same l. At 9.81, T ≈ 2.20 s.
The formula is the school one. Units follow SI; NIST SP 330 and BIPM define the measures, not your result.
Page updated in 2026.