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🛰️ Satellites: Orbits, Antennas, and Eyes in the Sky

Sort the sky into its working layers: low-orbit constellations, GPS in the middle, and geostationary giants parked over the equator. You'll understand how satellites are powered, pointed, and kept ali

10
lessons
~60 min
to learn
🔬 Science
subject
Adults
level
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What you’ll learn

  1. Orbit Is Falling, SidewaysReplace the idea that orbiting objects have escaped gravity with the correct one — they are falling continuously and missing — and see why that makes altitude the master variable of the whole subject.A satellite in orbit has not escaped gravity; it is in free fall, accelerating toward Earth exactly as a dropped stone does, but moving sideways so fast that the ground curves away beneath it as fast as it falls. Weightlessness aboard is the shared free fall of spacecraft and occupant, not the absence of gravity — at the ISS's altitude, Earth's pull is still around 90% of its surface value. Because orbiting is a balance between falling and moving sideways, how fast you must go is set by how high you are, which makes altitude the variable that decides everything else.
  2. Higher Means SlowerNail the one relationship that sorts the entire sky — altitude sets orbital period — and use real numbers to see the spread from 90 minutes to 24 hours.Because gravity weakens with distance and the circle to travel grows, a higher orbit means both a slower speed and a longer path, so the period rises steeply with altitude — the relationship Kepler's third law makes exact. The consequences are concrete: a satellite a few hundred kilometres up laps the Earth in about 90 minutes, GPS at 20,200 km takes 11 hours 58 minutes, and at 35,786 km the period reaches one sidereal day. That last coincidence is what makes a satellite appear to hang still, and everything downstream is a consequence of picking a number on this ladder.
  3. GEO: Parked Over the EquatorUnderstand what geostationary orbit buys and what it charges — and see that its two great weaknesses, quarter-second latency and no polar coverage, are unfixable consequences of the same geometry that makes it work.A geostationary satellite hangs over one point on the equator, so ground antennas can be aimed once and never moved, and three of them see nearly the whole populated world — which is why broadcast and weather monitoring live there. The price is fixed by the same geometry: 35,786 km each way means about 240 ms of round-trip delay that no engineering removes, and because the orbit must lie in the equatorial plane, the satellite sits near the horizon at high latitudes and is effectively useless at the poles. There is also only one such ring, which makes slots a finite, allocated resource.
  4. LEO: Close, Fast, and Never ThereUnderstand the low-Earth-orbit trade — superb latency and a small footprint bought at the price of needing a constellation and a network that hands you over constantly.A few hundred kilometres up, the round trip is a handful of milliseconds rather than 240, which makes interactive use possible — but the same closeness shrinks the footprint and the 90-minute period means no satellite stays put. Coverage therefore requires a constellation and continuous handoff: Iridium reaches true global coverage including the poles with 66 active satellites at about 781 km in near-polar orbits, while Starlink's far larger constellation trades satellite count for bandwidth at around 525–535 km. Below about 600 km the residual atmosphere also drags satellites down within years, which is a maintenance cost and a safety feature at once.
  5. MEO: The Deliberate CompromiseSee why GPS sits in the middle of the ladder, and understand medium Earth orbit as a reasoned optimisation rather than a leftover.GPS orbits at 20,200 km with a period of 11 hours 58 minutes — half a sidereal day — which is a deliberate choice rather than a compromise by default. From that altitude a satellite sees a large slice of Earth, so 24 satellites in six inclined planes put about nine in view from anywhere, giving the spread geometry a position fix needs; the half-day period makes each satellite retrace its ground track daily, which simplifies monitoring. Latency does not matter for a one-way broadcast, so GPS spends nothing to avoid GEO's fatal flaw and buys coverage and stability instead.
  6. Power, Heat, and the DarkUnderstand how a satellite stays alive: solar arrays and the battery that carries it through eclipse, and the counterintuitive fact that its hardest thermal problem is getting rid of heat in the cold of space.A satellite runs on sunlight, which means it must survive eclipse — every orbit for a LEO satellite, and around the equinoxes for a geostationary one — on batteries, and those charge-discharge cycles are a major driver of its lifespan. Thermally, space is a vacuum, so there is no air to carry heat away: conduction and convection are unavailable and radiation is the only exit, which is why spacecraft need radiators despite the cold. The result is a vehicle that is simultaneously freezing on its shaded side and overheating on its sunlit one, managed by insulation, coatings, heaters and radiators.
  7. Pointing at NothingUnderstand how a satellite aims itself with nothing to push against — reaction wheels trading momentum with the spacecraft, star trackers telling it which way is up, and magnetorquers dumping the momentum that accumulates.A satellite must aim precisely but has nothing to push against, so it turns by conservation of angular momentum: spinning a reaction wheel one way rotates the spacecraft the other, using electricity rather than fuel. Knowing which way it is pointing comes from star trackers, which photograph the sky and match the pattern against a catalogue. Because external torques keep pushing the same way, the wheels gradually saturate, and the momentum must be dumped — by thrusters, which cost fuel, or by magnetorquers pushing against Earth's magnetic field, which cost only electricity.
  8. Antennas and the Link BudgetUnderstand why satellite communication is an accounting problem — the link budget — and how gain, dishes, spot beams and phased arrays are all answers to the same shortage.Radio spreads out as it travels, so power falls with the square of distance and a satellite link is always short of signal; engineers therefore keep a link budget of every gain and loss down to the receiver. Antenna gain is not amplification but concentration — a dish focuses power into a narrow cone instead of wasting it on the whole sky — which is why both ends use directional antennas. Modern satellites replace one wide beam with many narrow spot beams so each is stronger and the same frequencies can be reused in beams that don't overlap, and phased arrays steer beams electronically so a moving LEO satellite can be tracked without moving parts.
  9. Eyes: Looking Down on PurposeUnderstand remote sensing as a set of orbital choices — why imaging satellites fly sun-synchronous orbits, why weather satellites split between GEO and polar, and why resolution and coverage trade against each other.An imaging satellite needs comparable pictures over time, so it flies a sun-synchronous orbit: a nearly polar orbit at roughly 600–800 km and about 98° inclination, whose plane is precessed about a degree a day by Earth's equatorial bulge so it always crosses a given latitude at the same local solar time, holding the lighting constant. Weather satellites split by need — geostationary ones watch one hemisphere continuously for the motion of storms, polar ones fly low for detail and global coverage. Resolution and swath trade directly, which is why no single satellite watches everything closely.
  10. Kessler: Taking It Seriously Without PanickingUnderstand Kessler syndrome accurately — the mechanism, the real numbers, why altitude decides everything — and hold a proportionate view that is neither dismissive nor apocalyptic.Donald Kessler and Burton Cour-Palais proposed in 1978 that debris density in low orbit could reach a point where collisions cascade, each one generating fragments that cause further collisions. The energies make it plausible: a 1 kg object at 10 km/s can catastrophically break up a 1,000 kg spacecraft, and the 2007 Chinese ASAT test and the 2009 Iridium 33 collision — which alone produced over 2,000 large fragments — showed how fast a population can grow. Altitude decides the stakes, because low orbits self-clean through drag within years while high ones take millennia.

Questions this course answers

Why do astronauts float aboard the International Space Station?

Gravity is very much present — about 90% of surface strength at that altitude. You feel weight only when something pushes back at you, and nothing does: the floor is falling at the same rate you are. Astronauts are weightless not because gravity is absent but because it is the only thing acting on them.

What does it mean to say an orbit is 'falling and missing'?

Newton's cannonball: fire it hard enough and its downward curve matches the curve of a spherical Earth, so it never arrives. Gravity hasn't stopped and no engine is fighting it — orbit is a permanent, exquisitely-tuned failure to hit the planet, which is why nearly all a launch's energy goes into sideways speed rather than altitude.

Why does a higher orbit have a longer period?

Two effects compound. Weaker gravity means less sideways speed is needed to keep missing the Earth, and a bigger orbit means a longer path. Slower around a longer circle is why the period climbs so steeply — Kepler's third law, worked out from planetary data centuries before anyone knew the mechanism.

What makes a geostationary orbit possible at 35,786 km specifically?

It is a coincidence of numbers being exploited. The period at that altitude is 1,436 minutes — one sidereal day — matching Earth's rotation. The satellite is still moving at about 3 km/s and still falling; it merely appears motionless from the ground, which is why a TV dish can be aimed once and bolted down forever.

Why is altitude called the master variable of satellite design?

There is no throttle in orbital mechanics. Pick an altitude and physics hands you the rest: speed, period, footprint, signal distance and constellation size all follow. That is why the sky sorts into distinct bands, and why every satellite you've heard of is best understood as somebody choosing a rung on that ladder.

Why is the ~240 ms round-trip delay of a geostationary link impossible to engineer away?

The magic and the misery are the same number. Hanging still requires a one-day period, a one-day period requires 35,786 km, and 35,786 km costs a quarter-second round trip at light speed. There is no version where you get the fixed dish without the delay — no bandwidth, modem or budget touches it.

Grounded in trusted sources

  • Wikipedia — Geostationary orbit (https://en.wikipedia.org/wiki/Geostationary_orbit)
  • Wikipedia — Low Earth orbit (https://en.wikipedia.org/wiki/Low_Earth_orbit)
  • Wikipedia — Medium Earth orbit (https://en.wikipedia.org/wiki/Medium_Earth_orbit)
  • Wikipedia — Orbital mechanics (https://en.wikipedia.org/wiki/Orbital_mechanics)
  • Wikipedia — Kepler's laws of planetary motion (https://en.wikipedia.org/wiki/Kepler%27s_laws_of_planetary_motion)
  • Wikipedia — Starlink (https://en.wikipedia.org/wiki/Starlink)
  • Wikipedia — Iridium satellite constellation (https://en.wikipedia.org/wiki/Iridium_satellite_constellation)
  • Wikipedia — Sun-synchronous orbit (https://en.wikipedia.org/wiki/Sun-synchronous_orbit)

Every Wunder lesson is built from real, reputable sources — never invented.

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