Separation, centre to centre
— km
—
Time for light to cross
—
A signal returned would take —
Rate of separation, this instant
—
Reckoned from the change in range over the coming day — bodies on eccentric or fast-shifting paths may show a momentary figure rather than a steady one.
Looking ahead, one year
The same two bodies, their range traced forward three hundred and sixty-five days from today.
Nearest approach in the year ahead
—
—
Farthest range in the year ahead
—
—
Doppler shift on a carrier of
MHz
—
As reckoned from the rate of separation alone — a first approximation, ignoring the motion of the receiving station.
Synodic period — the cycle of returning alignments
—
Applies to two bodies that each circle the Sun directly.
Apparent disc, seen from the first body
—
—
Were you to travel there
The same range, set against the pace of various known conveyances — a straight-line division of distance by speed, not a real trajectory. No acceleration, no coasting, no gravity assists, and no allowance for air or vacuum are reckoned here; actual missions take longer and follow curved paths. Treat these as a sense of scale, not a flight plan.
| By | Speed | Time required |
|---|
Routed by way of a third body
A signal need not travel direct — here it is relayed through an intermediate body, received and resent.
Relay via
Total light-time by this route, against the direct path
—
—
Surface gravity—
Escape velocity—
—
Surface gravity—
Escape velocity—
Travel through time
Slide the range to reckon the separation at any moment within two years either side of today. The orrery and all figures above move with it.
now
Hohmann transfer — minimum-energy orbit
Gravity-assist Δv budget
Your weight, worlds compared
Surface weight of a given mass on every body in this catalogue.
A mass of
weighs —
Notable events — next two years
Local minima and maxima of the separation — conjunctions, oppositions, and greatest elongations — scanned forward 730 days.
Launch windows — Hohmann opportunities
Each window is a moment when departing on a Hohmann transfer arc will place you near the destination at arrival. The Δv figures are computed from mean orbital radii and are therefore constant per body pair — a real porkchop plot would show per-window variation. Only meaningful for two planets.