← General Physics I
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Universal Gravitation

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 m1m_1 and m2m_2 attract each other with force Fg=Gm1m2/r2F_g = Gm_1m_2/r^2, where G=6.674Γ—10βˆ’11G = 6.674\times10^{-11} NΒ·mΒ²/kgΒ² and rr is the center-to-center distance.
Gravitational Field
The gravitational field gβƒ—\vec{g} at a point is the force per unit mass felt by a test particle there: gβƒ—=Fβƒ—g/m=βˆ’GMr^/r2\vec{g} = \vec{F}_g/m = -GM\hat{r}/r^2. At Earth's surface, gβ‰ˆ9.8g \approx 9.8 m/sΒ².
Gravitational Potential Energy (general)
U=βˆ’Gm1m2/rU = -Gm_1m_2/r. Negative because gravity is attractive. Zero at infinity. Near Earth's surface: Uβ‰ˆmghU \approx mgh (when r≫Δrr \gg \Delta r).
Escape Velocity
Minimum launch speed to escape a planet's gravity: vesc=2GM/Rv_\text{esc} = \sqrt{2GM/R} (from the surface). Derived from K+U=0K + 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) T2∝a3T^2 \propto a^3 where aa is the semi-major axis.
Circular Orbits
For circular orbit of radius rr: gravitational force provides centripetal force. Orbital speed v=GM/rv = \sqrt{GM/r} and period T=2Ο€r3/GMT = 2\pi\sqrt{r^3/GM}.

Key Equations

Gravitational force
Fg=Gm1m2r2F_g = \frac{Gm_1m_2}{r^2}
Attractive, along the line joining the centers. G = 6.674Γ—10⁻¹¹ NΒ·mΒ²/kgΒ².
Orbital speed (circular orbit)
v=GMrv = \sqrt{\frac{GM}{r}}
Speed required to maintain a circular orbit of radius r around mass M.
Kepler's Third Law
T2=4Ο€2GM r3T^2 = \frac{4\pi^2}{GM}\,r^3
Period squared proportional to orbital radius cubed. For elliptical orbits, replace r with semi-major axis a.
Escape velocity
vesc=2GMRv_\text{esc} = \sqrt{\frac{2GM}{R}}
Minimum speed to escape to infinity from the surface of a body of mass M and radius R.
Gravitational PE (general)
U=βˆ’Gm1m2rU = -\frac{Gm_1m_2}{r}
Zero at r β†’ ∞. More negative = more tightly bound. Near-surface: U β‰ˆ 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. (ME=5.97Γ—1024M_E = 5.97\times10^{24} kg, RE=6.37Γ—106R_E = 6.37\times10^6 m.)

Solution

Orbital radius: r=RE+h=6.37Γ—106+4.08Γ—105=6.778Γ—106r = R_E + h = 6.37\times10^6 + 4.08\times10^5 = 6.778\times10^6 m.

Orbital speed:

v=GMEr=6.674Γ—10βˆ’11Γ—5.97Γ—10246.778Γ—106β‰ˆ7660Β m/sv = \sqrt{\frac{GM_E}{r}} = \sqrt{\frac{6.674\times10^{-11}\times5.97\times10^{24}}{6.778\times10^6}} \approx 7660 \text{ m/s}

Period:

T=2Ο€rv=2π×6.778Γ—1067660β‰ˆ5560Β sβ‰ˆ92.7Β minT = \frac{2\pi r}{v} = \frac{2\pi\times6.778\times10^6}{7660} \approx 5560 \text{ s} \approx 92.7 \text{ min}
Answer ISS orbital speed β‰ˆ 7.66 km/s; period β‰ˆ 92.7 minutes.
Practice

Exercises

7 problems
1 of 7

Two spheres of mass m1=5m_1 = 5 kg and m2=10m_2 = 10 kg are separated by 0.50.5 m center-to-center. What is the gravitational force (in N) between them? Use G=6.674Γ—10βˆ’11G = 6.674\times10^{-11} NΒ·mΒ²/kgΒ².

N
2 of 7

What is the gravitational acceleration (in m/sΒ²) on the surface of Mars? Mars has mass M=6.39Γ—1023M = 6.39\times10^{23} kg and radius R=3.39Γ—106R = 3.39\times10^6 m. Use G=6.674Γ—10βˆ’11G = 6.674\times10^{-11} NΒ·mΒ²/kgΒ².

m/sΒ²
3 of 7

A satellite orbits Earth in a circular orbit at an altitude of h=800h = 800 km above the surface. What is its orbital speed (in m/s)? Use GME=3.986Γ—1014GM_E = 3.986\times10^{14} mΒ³/sΒ², RE=6.37Γ—106R_E = 6.37\times10^6 m.

m/s
4 of 7

What is the orbital period (in minutes) of the satellite in Exercise 3?

min
5 of 7

What is the escape velocity (in km/s) from Earth's surface? Use GME=3.986Γ—1014GM_E = 3.986\times10^{14} mΒ³/sΒ², RE=6.37Γ—106R_E = 6.37\times10^6 m.

km/s
6 of 7

A planet orbits a star with a period of T=3T = 3 years. Another planet orbits the same star with a period of T2=12T_2 = 12 years. If the first planet's semi-major axis is a1=1.5Γ—1011a_1 = 1.5\times10^{11} m, what is the second planet's semi-major axis (in AU)? (1 AU = 1.5Γ—10111.5\times10^{11} m.)

AU
7 of 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 GME=3.986Γ—1014GM_E = 3.986\times10^{14} mΒ³/sΒ², RE=6371R_E = 6371 km.

km

Key Takeaways

  • Gravity follows an inverse-square law: doubling the distance reduces the force by a factor of 4.
  • General U=βˆ’Gm1m2/rU = -Gm_1m_2/r reduces to mghmgh near Earth's surface β€” consistent because Ξ”U=mgΞ”r\Delta U = mg\Delta r for small Ξ”rβ‰ͺRE\Delta r \ll R_E.
  • Orbital speed decreases with altitude: higher orbit β†’ slower speed but longer period.
  • Kepler's Third Law T2∝r3T^2 \propto r^3 holds for any central force orbit around the same central mass.
  • Escape velocity is 2\sqrt{2} times the circular orbital speed at that radius.