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04 / CHAPTER 10

Orbits and escape

Use energy and angular momentum to classify trajectories.

Rotation & Gravitation: original course diagram
A visual model for this course. Read it as a prompt for the assumptions behind the chapter.

ANCHOR EQUATION

Specific orbital energy

ε=v22−GMr

In symbols: ε = v²/2 − GM/r

The sign of specific orbital energy classifies bound and unbound trajectories.

Orbits trade kinetic and potential energy

An orbit is continuous free fall: gravity bends the velocity so the object keeps missing the surface. Energy and angular momentum together distinguish circular, elliptical, parabolic, and hyperbolic motion.

Classify by specific energy

Divide total mechanical energy by mass: ε = v²/2 − GM/r. For a circular orbit, gravity supplies centripetal acceleration v²/r = GM/r², so v_c = √(GM/r). Substitution gives ε_c = −GM/(2r), negative because the orbit is bound.

At r = 7.0×10⁶ m around Earth, v_c = √(3.986×10¹⁴/7.0×10⁶) = 7.55 km/s. A low circular orbit takes T = 2πr/v ≈ 97 minutes.

Escape is a speed threshold, not a lack of gravity

Setting ε = 0 gives v_escape = √(2GM/r) = √2 v_c. A spacecraft above escape speed still feels gravity; it follows an unbound trajectory rather than stopping being attracted.

Work it: At altitude 400 km, use Earth radius 6.37×10⁶ m to compute circular and escape speeds. Explain why the satellite does not need continuous upward thrust to stay aloft.