INGENIA

CLS-11

Simple-pendulum period

T = 2π √(ℓ/g) for small angles.

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OscillationsHuygens 1673

Governing equation

T=2πgT=2\pi\sqrt{\dfrac{\ell}{g}}

where

\ell
Length (m)
g
Gravity (m/s²)
T
Period (s)

Lecture brief

Historical brief

Newtonian mechanics (1687) plus energy, angular momentum, Kepler and the ballistic parabola remain the first language of motion. Every sheet here is a closed-form orbit, throw, spin or oscillator. This sheet (CLS-11 — Simple-pendulum period) is the form associated with Huygens 1673. Working symbols: \ell, gg \rightarrow TT. Linearising ẍ + (g/ℓ) sin θ ≈ (g/ℓ) θ gives SHM of period 2π √(ℓ/g), Huygens' clock law.

Purpose

Purpose: compute TT from \ell, gg in Classical mechanics via T=2πgT=2\pi\sqrt{\dfrac{\ell}{g}} T = 2π √(ℓ/g) for small angles. Use it when a real classical mechanics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given =1.000m\ell = 1.000\,\mathrm{m}, g=9.810m/s2g = 9.810\,\mathrm{m/s^{2}}, the governing relation T=2πgT=2\pi\sqrt{\dfrac{\ell}{g}} yields T=2.0061sT = 2.0061\,\mathrm{s}. Massless rod, point bob, θ ≲ 15°, vacuum. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Period T2.0061 s
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CLS-11 · pendulum
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Narration of this film

Massless rod, point bob, θ ≲ 15°, vacuum.

Linearising ẍ + (g/ℓ) sin θ ≈ (g/ℓ) θ gives SHM of period 2π √(ℓ/g), Huygens' clock law.

Reading speed

Watch on YouTube