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Orbits and escape speed notes and lesson for AP Physics C (free PDF download)

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Orbits and escape speed notes and lesson for AP Physics C (free PDF download)

This AP Physics C lesson on orbits and escape speed notes gives the key ideas first, then worked examples and diagrams. After that, practise with the worksheet on orbits and escape speed and check yourself with the quiz.

Quick answer: Gravitational potential energy is U = −GMm/r, with zero at infinity. A circular orbit has v = √(GM/r) and total energy E = −GMm/2r. A projectile escapes if its total energy is zero or more, giving an escape speed of √(2GM/R).

Level: AP Physics C (Mechanics and E&M, calculus-based) · Curriculum: AP PC:M Unit 7

Orbits and escape speed notes: the key ideas

What is gravitational potential energy?

Near the ground we use U = mgh, but that assumes a constant g. Across large distances Newton’s law of gravitation, F = GMm/r², weakens with distance, so the potential energy must be found by integration. Taking U = 0 at infinite separation, the work needed to bring a mass in from infinity is negative, so U is always negative for a bound system.

Definition

The gravitational potential energy of two masses M and m, with their centres a distance r apart, is U(r) = −∫ from ∞ to r of F dr = −GMm/r. The force is F = −dU/dr, and G = 6.67 × 10⁻¹¹ N m²/kg².

Graph of gravitational potential energy against distance from the centre of Earth: a curve rising from a deep negative value at the surface towards zero at infinity, with a line for a bound orbit energy and a line at zero for escaperU, EE = 0: escapeE below 0: boundsurfaceturning point
Potential energy well: U = −GMm/r. A total energy of zero or more means escape.

The curve is a well. A system with total energy E = K + U below zero is bound and turns back at a maximum distance. If E ≥ 0 it never turns back.

How fast does a satellite orbit?

For a circular orbit gravity is the only force, and it provides the centripetal acceleration: GMm/r² = m v²/r. Solving gives the speed, and the period follows from T = 2πr/v.

A satellite at the top of a circular orbit around Earth: velocity points to the right, gravitational force points down to the centre of Earth, and the orbital radius r is shownEarthvFg = GMm/r²r
Circular orbit: gravity supplies the centripetal force, perpendicular to the velocity.
Formula

v = √(GM/r) and T = 2π√(r³/GM). Here G = 6.67 × 10⁻¹¹ N m²/kg², M is the mass of the central body in kg, r is the orbit radius from the centre in m, v is in m/s and T in s. Squaring the period gives Kepler’s third law: T² = (4π²/GM) r³.

Quantity (circular orbit of radius r)ExpressionDepends on satellite mass?
Orbital speedv = √(GM/r)No
PeriodT = 2π√(r³/GM)No
Kinetic energyK = GMm/2rYes
Potential energyU = −GMm/r = −2KYes
Total energyE = −GMm/2r = −KYes

The energy results are worth remembering: K = −E and U = 2E. A satellite that loses energy to air drag moves to a lower orbit, where it travels faster, because K = −E increases as E becomes more negative.

Worked example 1

A satellite orbits 400 km above Earth, so r = 6.37 × 10⁶ + 4.0 × 10⁵ = 6.77 × 10⁶ m. Using GM = 3.98 × 10¹⁴ N m²/kg² for Earth, v = √(3.98 × 10¹⁴ / 6.77 × 10⁶) = 7.67 km/s. The period is T = 2π(6.77 × 10⁶) / 7670 = 5.55 × 10³ s, which is 92.5 minutes.

What is escape speed?

To escape, a projectile needs total energy zero: ½mv² − GMm/R = 0. The mass cancels, so the escape speed from a body of radius R is v_esc = √(2GM/R). It is √2 times the circular orbital speed at the same radius.

Worked example 2

From Earth’s surface, v_esc = √(2 × 3.98 × 10¹⁴ / 6.37 × 10⁶) = √(1.25 × 10⁸) = 11.2 km/s. From the Moon (M = 7.35 × 10²² kg, R = 1.74 × 10⁶ m) the same method gives 2.37 km/s, which is why the Moon holds no thick atmosphere.

How do elliptical orbits and Kepler’s laws fit in?

An elliptical orbit with the star at one focus: the planet moves fast at the closest point, perihelion, and slowly at the farthest point, aphelion, sweeping out equal areas in equal timesstarfast (perihelion)slow (aphelion)a = semi-major axis
Kepler’s laws: the planet sweeps equal areas in equal times, so it is fastest at perihelion.

Gravity is a central force, so the torque about the star is zero and angular momentum L = m v r⊥ is conserved. This gives Kepler’s second law (equal areas in equal times, dA/dt = L/2m) and says that v is greatest where r is smallest. For an ellipse with semi-major axis a, the total energy is E = −GMm/2a and the period is T = 2π√(a³/GM).

Common mistake

Do not use U = mgh for a satellite, and do not put the orbital height into the formula in place of r. Always measure r from the centre of the planet, so r = R + altitude.

Lina’s tip

To check a gravity answer quickly, remember that E for a circular orbit is minus the kinetic energy. If your total energy comes out positive for a satellite that stays in orbit, you have made a sign error.

Key points to remember
  • Gravitational force F = GMm/r²; potential energy U = −GMm/r (zero at infinity).
  • Circular orbit: v = √(GM/r), T = 2π√(r³/GM), K = −E = GMm/2r.
  • Escape speed: v_esc = √(2GM/R), independent of the projectile’s mass.
  • Elliptical orbit: E = −GMm/2a; angular momentum is conserved, so v is greatest at the closest point.
  • Kepler’s third law: T² = (4π²/GM)a³.

Orbits, escape speed and gravitational energy: frequently asked questions

Why is gravitational potential energy negative?

Because we choose U = 0 at infinite separation. Gravity is attractive, so bringing the masses closer releases energy, and the system energy falls below zero. A negative total energy means the system is bound.

Why does a satellite speed up when it loses energy?

Air drag lowers the total energy E = −GMm/2r, so r decreases. A smaller r means a larger orbital speed v = √(GM/r), and kinetic energy K = −E rises. The satellite spirals inward while gaining speed.

Does escape speed depend on the mass of the rocket?

No. The kinetic energy needed grows with the rocket’s mass, but so does its gravitational potential energy, so the mass cancels in ½mv² = GMm/R. The escape speed depends only on the planet’s mass and radius.

Why do astronauts float if gravity still acts on them?

Both the station and the astronaut are in free fall around Earth with the same acceleration. At 400 km, g is about 8.7 m/s², roughly 89 % of its surface value, but no contact force from the floor is needed, so they feel weightless.

What is the link between Kepler’s second law and angular momentum?

The gravitational force always points to the star, so it exerts no torque about it. Angular momentum m v r⊥ stays constant, which means the area swept per second, dA/dt = ½ r v⊥, is also constant.

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