Post-mission disposal — where it appears
Named by 3 essays across one field — each of them below, with the objects they name alongside it.
A collision rate that needs no collision
The flux through an orbital shell is a gas-kinetic calculation with no orbits in it. Production goes as the square of the population and removal goes as the first power, so a quadratic overtakes a linear once and never comes back — and which side of that a shell is on is decided by its altitude.
Fifty objects that hold most of the future
Low Earth orbit holds thousands of dead satellites and spent rocket stages, and the debris of the future will come mostly from their collisions. But not in equal shares. A derelict's contribution is the chance it is hit, times the fragments it would make, times how long they would stay up — and all three favour the heaviest objects in the most crowded, highest orbits. Ranked that way, a few tens of rocket bodies near 850 kilometres carry nearly half the risk, and the arithmetic of cleaning space becomes the arithmetic of choosing them.
A removal rate set by one percentage
How many dead satellites have to be taken out of a high orbit each year is decided less by the orbit than by how often a satellite fails to dispose of itself. Above eight hundred kilometres a derelict stays for centuries, so the removal rate needed to keep a shell stable is very nearly the failure rate, and moving disposal reliability from ninety per cent to ninety-nine cuts the work tenfold.
Named alongside it
The objects these essays reach for when they reach for this one.
Kessler syndromeOrbital debrisOrbital lifetimeActive debris removalAtmospheric dragBallistic coefficientBreakup modelCollision cross-sectionCollision probabilityCollision rateConjunction analysisCritical density