Newton's law of universal gravitation unifies terrestrial and celestial mechanics under one equation: every mass attracts every other with a force proportional to their masses and inversely proportional to the square of their separation. This single law explains free fall, tides, planetary orbits, and the structure of the Solar System.
Key Concepts
Newton's Law of Gravitation
Every pair of masses m1β and m2β attract each other with force Fgβ=Gm1βm2β/r2, where G=6.674Γ10β11 NΒ·mΒ²/kgΒ² and r is the center-to-center distance.
Gravitational Field
The gravitational field gβ at a point is the force per unit mass felt by a test particle there: gβ=Fgβ/m=βGMr^/r2. At Earth's surface, gβ9.8 m/sΒ².
Gravitational Potential Energy (general)
U=βGm1βm2β/r. Negative because gravity is attractive. Zero at infinity. Near Earth's surface: Uβmgh (when rβ«Ξr).
Escape Velocity
Minimum launch speed to escape a planet's gravity: vescβ=2GM/Rβ (from the surface). Derived from K+U=0 at launch.
Kepler's Laws
(1) Orbits are ellipses with the star at one focus. (2) A line from star to planet sweeps equal areas in equal times (consequence of angular momentum conservation). (3) T2βa3 where a is the semi-major axis.
Circular Orbits
For circular orbit of radius r: gravitational force provides centripetal force. Orbital speed v=GM/rβ and period T=2Οr3/GMβ.
Key Equations
Gravitational force
Fgβ=r2Gm1βm2ββ
Attractive, along the line joining the centers. G = 6.674Γ10β»ΒΉΒΉ NΒ·mΒ²/kgΒ².
Orbital speed (circular orbit)
v=rGMββ
Speed required to maintain a circular orbit of radius r around mass M.
Kepler's Third Law
T2=GM4Ο2βr3
Period squared proportional to orbital radius cubed. For elliptical orbits, replace r with semi-major axis a.
Escape velocity
vescβ=R2GMββ
Minimum speed to escape to infinity from the surface of a body of mass M and radius R.
Gravitational PE (general)
U=βrGm1βm2ββ
Zero at r β β. More negative = more tightly bound. Near-surface: U β mgh.
Worked Example
Orbital Period of the International Space Station
Problem
The ISS orbits at altitude 408 km above Earth's surface. Find its orbital speed and period. (MEβ=5.97Γ1024 kg, REβ=6.37Γ106 m.)
Solution
Orbital radius: r=REβ+h=6.37Γ106+4.08Γ105=6.778Γ106 m.
Orbital speed:
v=rGMEβββ=6.778Γ1066.674Γ10β11Γ5.97Γ1024βββ7660Β m/s
Period:
T=v2Οrβ=76602ΟΓ6.778Γ106ββ5560Β sβ92.7Β min
AnswerISS orbital speed β 7.66 km/s; period β 92.7 minutes.
Practice
Exercises
7 problems
1of 7
Two spheres of mass m1β=5 kg and m2β=10 kg are separated by 0.5 m center-to-center. What is the gravitational force (in N) between them? Use G=6.674Γ10β11 NΒ·mΒ²/kgΒ².
N
2of 7
What is the gravitational acceleration (in m/sΒ²) on the surface of Mars? Mars has mass M=6.39Γ1023 kg and radius R=3.39Γ106 m. Use G=6.674Γ10β11 NΒ·mΒ²/kgΒ².
m/sΒ²
3of 7
A satellite orbits Earth in a circular orbit at an altitude of h=800 km above the surface. What is its orbital speed (in m/s)? Use GMEβ=3.986Γ1014 mΒ³/sΒ², REβ=6.37Γ106 m.
m/s
4of 7
What is the orbital period (in minutes) of the satellite in Exercise 3?
min
5of 7
What is the escape velocity (in km/s) from Earth's surface? Use GMEβ=3.986Γ1014 mΒ³/sΒ², REβ=6.37Γ106 m.
km/s
6of 7
A planet orbits a star with a period of T=3 years. Another planet orbits the same star with a period of T2β=12 years. If the first planet's semi-major axis is a1β=1.5Γ1011 m, what is the second planet's semi-major axis (in AU)? (1 AU = 1.5Γ1011 m.)
AU
7of 7
At what altitude (in km) above Earth's surface must a satellite orbit so that its period equals exactly 24 hours (geosynchronous orbit)? Use GMEβ=3.986Γ1014 mΒ³/sΒ², REβ=6371 km.
km
Key Takeaways
Gravity follows an inverse-square law: doubling the distance reduces the force by a factor of 4.
General U=βGm1βm2β/r reduces to mgh near Earth's surface β consistent because ΞU=mgΞr for small ΞrβͺREβ.
Orbital speed decreases with altitude: higher orbit β slower speed but longer period.
Kepler's Third Law T2βr3 holds for any central force orbit around the same central mass.
Escape velocity is 2β times the circular orbital speed at that radius.