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Deriving v_esc = √(2GM/r) = √(2gr)

Escape means arriving at infinity with zero KE and zero PE, so by conservation of energy ½mv² + (−GMm/r) = 0, giving v_esc = √(2GM/r) = √(2gr), which is √2 × the orbital speed at the same radius.

½mv_esc² = GMm/r ⇒ v_esc = √(2GM/r) = √(2gR) ≈ 11 km s⁻¹

What this actually means

Open with the energy statement, not the formula: KE_i + U_i = KE_∞ + U_∞ = 0 + 0. Both terms at infinity are zero, KE because 'minimum' means arriving with nothing left, U because infinity is where we set the zero. That sentence is usually worth a mark on its own.

Then substitute: ½mv² + (−GMm/r) = 0, so ½mv² = GMm/r. All the launch kinetic energy is spent paying off the depth of the potential well. Cancel m, multiply by 2, take the root.

Say out loud that m cancels, and say why it matters: escape speed is a property of the PLANET, not of the thing escaping. A pebble and a rocket need the same 11 km s⁻¹.

The √(2gR) form comes from GM = gR² at the surface. Use it when the question gives you g and R but not M, which it usually does. For Earth, √(2 × 9.81 × 6.4 × 10⁶) = 1.1 × 10⁴ m s⁻¹.

Compare with orbit: v_orbit = √(GM/r), so v_esc = √2 × v_orbit at the same radius. Handy sanity check, and it also answers the 'how much extra KE to escape from orbit' question, since KE scales as v² so you need exactly double the kinetic energy.

Two facts the mark scheme wants stated explicitly: independent of the object's mass, and independent of launch direction (energy is a scalar). Air resistance and the planet's own rotation are ignored in this treatment, which is worth flagging if asked for assumptions.

The trap

Setting KE at infinity to some non-zero value, or forgetting the minus sign on the potential energy term.

Prove it — watch it be true

  1. Open the escape-velocity launcher and sweep the launch speed from low to high, watching the outcome flip from fall back, to orbit, to escape.
  2. Find the exact threshold where the outcome first reads escape and compare it with √(2gR) for that planet.
  3. Compare that threshold with the circular-orbit speed shown for the same radius and confirm the ratio is √2.
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