INGENIA

CLS-06

Kepler's third law

T² = 4π² a³ /(G M) for a circular (or Keplerian) orbit.

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GravityKepler 1619Newton 1687

Governing equation

T2=4π2a3GMT^2=\dfrac{4\pi^2 a^3}{GM}

a∈[1×108,1×1013]a \in \left[1\times 10^{8}, 1\times 10^{13}\right]

where

M
Central mass (kg)
a
Semi-major axis (m)
T
Period (d)
T
Period (yr)

The figure, part by part

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CLS-06 · orbit
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①

Governing law — red

T2=4π2a3GMT^2=\dfrac{4\pi^2 a^3}{GM}

a∈[1×108,1×1013]a \in \left[1\times 10^{8}, 1\times 10^{13}\right]

a=1×108a = 1\times 10^{8}T=1.73×10−5T = 1.73\times 10^{-5}

②

Domain of the variable — blue

amin⁡=1×108,amax⁡=1×1013a_{\min} = 1\times 10^{8},\quad a_{\max} = 1\times 10^{13}

a∈[1×108,1×1013]a \in \left[1\times 10^{8}, 1\times 10^{13}\right]

a=1×108a = 1\times 10^{8}a=1×108a = 1\times 10^{8}

③

Response curve — green

T2=4π2a3GMT^2=\dfrac{4\pi^2 a^3}{GM}

a∈[1×108,1×1013]a \in \left[1\times 10^{8}, 1\times 10^{13}\right]

a=1×108a = 1\times 10^{8}T=1.73×10−5T = 1.73\times 10^{-5}

④

Rate of change — amber

dTda\frac{\mathrm{d}T}{\mathrm{d}a}

a∈[1×108,1×1013]a \in \left[1\times 10^{8}, 1\times 10^{13}\right]

a=6.3×1010a = 6.3\times 10^{10}T′=6.14×10−12T^{\prime} = 6.14\times 10^{-12}

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-06 — Kepler's third law) is the form associated with Kepler 1619 · Newton 1687. Working symbols: MM, aa →\rightarrow TT, TT. Newton derived Kepler's T² ∝ a³ from inverse-square gravity. For a circular orbit the centripetal requirement is GM/a² = ω² a.

Purpose

Purpose: compute TT, TT from MM, aa in Classical mechanics via T2=4π2a3GMT^2=\dfrac{4\pi^2 a^3}{GM} T² = 4π² a³ /(G M) for a circular (or Keplerian) orbit. 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 M=1.989e+30 kgM = 1.989e+30\,\mathrm{kg}, a=1.496e+11 ma = 1.496e+11\,\mathrm{m}, the governing relation T2=4π2a3GMT^2=\dfrac{4\pi^2 a^3}{GM} yields T=365.211 dT = 365.211\,\mathrm{d}, T=0.9999 yrT = 0.9999\,\mathrm{yr}. Point mass M ≫ m, circular orbit, G = 6.674×10⁻¹¹. Move a slider: the numbers are this situation, not a canned story.

Calculator

Inputs

Outputs

  • Period T365.211 d
  • Period T0.9999 yr
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CLS-06 · orbit
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Narration of this film

Point mass M ≫ m, circular orbit, G = 6.674×10⁻¹¹.

Newton derived Kepler's T² ∝ a³ from inverse-square gravity. For a circular orbit the centripetal requirement is GM/a² = ω² a.

Reading speed

Watch on YouTube