3.2.3 · D5Orbital Mechanics & Astrodynamics

Question bank — Orbit equation r = p - (1 + e·cos θ) — derivation from equations of motion

2,141 words10 min readBack to topic

Before we hunt traps, look at the picture every question secretly depends on. This one diagram names every symbol used on the page — pin it in your mind.

Figure — Orbit equation r = p - (1 + e·cos θ) — derivation from equations of motion

True or false — justify

Every answer begins with True or False and then why — a bare verdict earns nothing.

TF1 — In , the angle is measured from the center of the ellipse.
False. is the true anomaly, measured from perihelion as seen from the focus (the Sun), not the geometric center; the angle measured at the center is the eccentric anomaly, a different angle entirely.
TF2 — Setting turns the equation into , a constant, i.e. a circle.
True. With the term vanishes, so for all — a fixed radius is precisely a circle, and here too.
TF3 — For a bound ellipse, is largest when is largest.
False. is a fraction with on the bottom; is largest when the denominator is smallest, i.e. when at (aphelion).
TF4 — The semi-latus rectum equals the semi-major axis for every orbit.
False. In general ; they only coincide when (circle). For any real ellipse .
TF5 — Specific angular momentum is conserved because gravity does no work on the planet.
False. is conserved because gravity is a central force (always along the radial direction ), giving zero torque about the focus — that is a statement about direction, not about work.
TF6 — A parabolic orbit () has a finite aphelion distance.
False. At the denominator as , so ; the body escapes and never returns, so there is no aphelion.
TF7 — Two orbits with the same but different pass through the same point at .
True. At , so regardless of ; all conics sharing a cross the semi-latus-rectum point together.
TF8 — Increasing while holding fixed makes the perihelion move closer to the focus.
True. shrinks as grows, so a more eccentric orbit at fixed dives nearer the Sun at closest approach.
TF9 — The orbit equation was derived assuming the two masses are equal.
False. It assumes one mass dominates so ; it also holds exactly for the relative coordinate of any two-body system with .

Spot the error

Each line contains a plausible-looking but flawed statement. The reveal names the flaw.

SE1 — "Since repeats every , the orbit equation gives two different radii for and , so the orbit isn't closed."
The error: repeating is exactly what makes the orbit retrace itself each revolution; different giving different is the oval shape, not a break in closure. A bound orbit closes precisely because is periodic in over .
SE2 — "Perihelion is where the planet moves slowest, since it's turning the sharp corner."
The error: perihelion is where the planet moves fastest. By , small forces large ; the corner is sharp because the planet is whipping through it, not crawling.
SE3 — "Because , a heavier orbiting satellite follows a wider orbit for the same launch conditions."
The error: since depends only on the central body, dividing by removes the satellite's own mass. Same launch conditions ⇒ identical path regardless of the small mass.
SE4 — "Writing instead of describes a completely different orbit."
The error: it's the same orbit, just with perihelion relabelled to instead of . The sign only rotates the angle origin; the geometric shape is untouched.
SE5 — ", so a faster-spinning orbit (bigger ) is always a smaller orbit."
The error: bigger increases (it's in the numerator), making the orbit larger, not smaller. More angular momentum flings the body wider.
SE6 — "The substitution is just algebraic bookkeeping with no physical reason."
The error: it's chosen because plotting against turns the orbit's curve into a plain cosine wave — the force becomes and the ODE becomes the linear oscillator , whose solution is . The whole derivation hinges on that tool choice.
SE7 — "At the planet is at the end of the minor axis of the ellipse."
The error: at we are at measured from the focus, which is the end of the latus rectum, not the minor-axis tip. That tip is measured from the center and its distance there equals the semi-minor axis — a different point and a different length.

Why questions

WQ1 — Why does the derivation switch from time derivatives to derivatives?
Because we want the shape , not the timing , and increases monotonically over , so it's a clean, single-valued independent variable — while goes back and forth in time.
WQ2 — Why is the driving term a constant in the oscillator equation?
Both (central-body property) and (conserved specific angular momentum) are fixed once the orbit is set, so the right-hand side never varies with , giving a simple constant-forced harmonic oscillator.
WQ3 — Why does conserved angular momentum immediately imply a flat (planar) orbit?
is perpendicular to both position and velocity; if never changes direction, position and velocity are forever confined to the single plane perpendicular to .
WQ4 — Why does the eccentricity come out as a free constant rather than being fixed by the physics?
When we solve the oscillator , the wave part carries an amplitude constant (the height of the cosine, set by initial conditions); bundling it as makes free. The equations permit any shape, and it is where you launch and how fast that selects circle, ellipse, parabola or hyperbola.
WQ5 — Why does exactly at regardless of ?
Because kills the entire -dependent term, leaving ; this is why is literally the distance "sideways" from perihelion for any conic.
WQ6 — Why can the same formula describe both a captured planet and an escaping comet?
The sign of in the denominator changes behaviour: for the denominator stays positive for all (closed ellipse), while for it can reach zero, sending (open escape) — one equation, all conics.

Edge cases

EC1 — What does the formula predict as for the aphelion distance ?
It blows up: . The ellipse stretches without bound and, at exactly , becomes an open parabola with no far turning point.
EC2 — What happens to for at the angle where ?
The denominator , so : these two angles are the asymptote directions of the hyperbola, beyond which the formula would give unphysical negative (that branch is not travelled).
EC3 — Is (aphelion) meaningful for a hyperbolic orbit?
No. For , gives negative , which is unphysical; the body never reaches because it has already escaped along an asymptote.
EC4 — What is the orbit if exactly?
A degenerate radial "orbit" — zero specific angular momentum means , so the body falls straight in (or straight out) along a line; the polar formula collapses since .
EC5 — In the circle limit , where is perihelion?
Everywhere and nowhere — with constant there is no unique closest point, so the choice of becomes arbitrary; perihelion is only well-defined once .
EC6 — For a bound ellipse, can the denominator ever reach zero?
No. Since , the smallest value is at ; the denominator stays strictly positive, so is always finite — exactly why the orbit is closed.

Active recall

Recall One-line reflexes (cover the answers!)
  • is measured from what point? → the focus (the Sun), not the center.
  • Which of the three anomalies appears in the orbit equation? → the true anomaly (measured at the focus).
  • Largest occurs at which for an ellipse? → (aphelion), where the denominator is smallest.
  • Does the small orbiting mass affect the path shape? → No; depends only on the central body.
  • What makes possible? → denominator , needing .

See also: Kepler's Laws, Conic Sections, Specific Angular Momentum h, Eccentricity and Orbital Energy, Central Force Motion, Vis-viva Equation.