l = 1 m, default g
l = 1 m, blank g.
Enter string length l. Blank g = 9.81. School model: point mass, massless rod, small angle.
Practical version (swing, clock): pendulum period. Then f = 1/T on frequency from period. ω: angular velocity.
Enter values. The result shows up here.
A simple (mathematical) pendulum is a model: point mass on a massless string (or rod) of length l, planar motion, no friction, small angle. Then T = 2π√(l/g).
Same numbers as the practical page: l = 1 m, g = 9.81 m/s² → T ≈ 2.01 s. The difference is emphasis: here we state the school assumptions.
At large angles the formula is no longer exact. Mass and amplitude do not enter this T. Blank g = 9.81.
Compare with the practical pendulum when you want playground or clock examples.
T = 2π √(l/g)
Assumptions: small angle, point mass, massless string, no drag.
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.
Ideal model: point mass, massless string, small angle, no drag. Formula T = 2π√(l/g).
Same formula. That page is practical examples; this one stresses school assumptions. Link: <a href="pendulum-period.html">pendulum period</a>.
For small θ, sin θ ≈ θ and the motion is harmonic. At large angles the period grows.
No. In the simple model T does not depend on m.
We use 9.81 m/s².
f = 1/T on <a href="frequency-from-period.html">frequency from period</a>; ω = 2π/T on <a href="angular-velocity.html">angular velocity</a>.
Not in this model. A physical pendulum uses centre of mass and moment of inertia.
Length must be positive.
Like √l at fixed g.
Spring: f from k and m. Pendulum: T from l and g.
Slightly. You can enter your own g instead of 9.81.