analyse circular orbits in gravitational fields by relating the gravitational force to the centripetal acceleration it causes

Gravitational Force Between Point Masses

In physics, the gravitational force between two point masses is described by Newton’s law of universal gravitation.

Think of it like a cosmic handshake: the more massive the objects, the stronger the handshake, and the farther apart they are, the weaker it becomes. 🤝

1️⃣ The Gravitational Force Formula

\$F = G\frac{m1m2}{r^2}\$

where:

  • \$F\$ = gravitational force (N)
  • \$G\$ = gravitational constant \$6.674\times10^{-11}\,\text{Nm}^2\text{/kg}^2\$
  • \$m1, m2\$ = masses (kg)
  • \$r\$ = distance between centres (m)

2️⃣ Centripetal Acceleration

For an object moving in a circle of radius \$r\$ at speed \$v\$, the required centripetal acceleration is

\$a_c = \frac{v^2}{r}\$

The gravitational force provides this acceleration when the object orbits a massive body. 🌍

3️⃣ Circular Orbit Condition

In a stable circular orbit, the gravitational force equals the centripetal force:

\$G\frac{M m}{r^2} = m\frac{v^2}{r}\$

Simplifying (cancel \$m\$):

\$v^2 = \frac{GM}{r}\$

So the orbital speed depends only on the mass of the central body (\$M\$) and the orbital radius (\$r\$).


🔄 If you double the radius, the speed drops to about \$1/\sqrt{2}\$ of its previous value.

4️⃣ Example: Earth‑Moon System

Let’s calculate the Moon’s orbital speed around Earth.

  • \$M_{\text{Earth}} = 5.97\times10^{24}\,\text{kg}\$
  • \$r_{\text{Earth–Moon}} = 3.84\times10^8\,\text{m}\$

Using \$v = \sqrt{GM/r}\$:

\$v = \sqrt{\frac{6.674\times10^{-11}\times5.97\times10^{24}}{3.84\times10^8}} \approx 1.02\times10^3\,\text{m/s}\$

So the Moon travels about 1 km/s around Earth. 🚀

5️⃣ Exam Tips Box

📝 Key Points to Remember:

  1. Always write the full equation \$F = Gm1m2/r^2\$ before simplifying.
  2. When cancelling the orbiting mass \$m\$, note that it disappears from the final speed expression.
  3. Check units: \$G\$ is in \$\text{Nm}^2\text{/kg}^2\$, so \$v\$ will be in \$\text{m/s}\$.
  4. For circular orbits, remember \$v^2 = GM/r\$; for elliptical orbits, use the vis‑viva equation.
  5. Use the “handshake” analogy to explain why more massive bodies pull harder.

6️⃣ Quick Practice Problems

  1. Calculate the orbital speed of a satellite at an altitude of 300 km above Earth’s surface.
  2. If a planet has twice Earth’s mass but the same radius, how does the orbital speed at its surface change?
  3. Show that the gravitational force between two equal masses at a distance of 10 m is 1/100 of the force when they are 1 m apart.

7️⃣ Summary Box

Remember:

  • Gravitational force decreases with the square of distance.
  • In a circular orbit, the required centripetal acceleration is supplied by gravity.
  • Orbital speed depends only on the central mass and orbital radius.