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Lesson 6 · Orbits, rockets and Voyager

Getting There

Orbiting is not floating above the Earth. It is falling, sideways, so fast that you keep missing. Everything about spaceflight follows from that, and from one equation that punishes every kilogram.

Space is closer than you think
100 km up
That is where space officially begins, a drive from London to Cambridge, straight up. Reaching it is easy. Staying there is the hard part, and it needs a sideways speed of 7.8 kilometres every second.

The International Space Station is only about 400 km up. At that height gravity is still 88% as strong as on the ground. The astronauts float because they and the station are in free fall, together, all the time. They are falling toward Earth at every moment, and moving sideways so fast that the Earth curves away beneath them as fast as they fall.

You are in a spacecraft in a circular orbit, and you fire your engine forward, in the direction you are moving. What happens to your speed, a little later on?
Your orbit rises, and you end up moving slower. Firing forward adds energy and lifts the far side of your orbit to a higher altitude. Higher orbits are slower: the speed for a circular orbit goes as 1/√r. You gave the engine more fuel and ended up going slower. To catch up with something ahead of you in the same orbit, you have to slow down first, drop to a lower and faster orbit, and then climb back.
The Saturn V rocket weighed about 2,970 tonnes at lift-off. The Apollo capsule that splashed down weighed about 5.5 tonnes. What fraction of the rocket came home?
About 0.2%. The rest was fuel and parts thrown away on the way. That ratio is not a design flaw. It is what the physics demands, and the equation that explains it is the subject of this lesson.
Part 1

Newton's cannon

Isaac Newton described it in 1687. Imagine a cannon on top of a very tall mountain firing horizontally. Fire gently and the ball lands nearby. Fire faster and it lands farther. Fire fast enough and the ground curves away beneath the ball as it falls, and it never lands. That speed is the circular orbital velocity:

vcircular = √(GM / r)

At 400 km it is about 7.7 km/s, which is 27,600 km/h. One lap takes about 92 minutes, so the ISS crew sees 16 sunrises a day. Go faster and your orbit stretches into an ellipse. At exactly √2 times the circular speed, the path stops curving back. This is escape velocity: about 11.2 km/s from Earth's surface, 10.9 km/s from 400 km up. Go any faster and you leave for good, though you never escape gravity entirely; it just fades away.

The lab on the next tab lets you fire the cannon yourself.

Part 2

The most important equation in spaceflight

In 1903 a nearly deaf Russian schoolteacher named Konstantin Tsiolkovsky published the key result. A rocket moves by throwing mass backwards. The speed it gains, its delta-v, depends on how fast it throws the exhaust (ve) and on the ratio of its starting mass to its finishing mass:

Δv = ve × ln(mstart / mend)

The ln is a logarithm (there is a button for it on any scientific calculator), and it is the problem. To get a bit more speed you must carry exponentially more fuel. Fuel itself needs more fuel to carry it. Reaching low Earth orbit takes about 9.4 km/s of delta-v (7.7 for the orbit and the rest lost to gravity and air drag), and the best chemical rockets, with exhaust speeds of about 4.4 km/s, need roughly 88% of the launch mass to be propellant. A Saturn V managed to put about 5% of its launch mass into orbit, and about 1.6% on the way to the Moon.

The fixes are all clever ways around the same equation: staging (dropping empty tanks), reuse (landing the boosters; the first Falcon 9 landing was in December 2015), and better exhaust speed. An ion engine, such as the one on NASA's Dawn mission, throws charged atoms out at 30 km/s or more, many times faster than chemical fuel. But its thrust is only about the weight of a couple of sheets of paper, so it takes months of gentle pushing. Dawn became the first spacecraft to orbit two different bodies, Vesta and then Ceres.

Part 3

Stealing speed from a planet

If fuel is so expensive, can speed be had for free? Yes, by a gravity assist. A spacecraft that swings past a moving planet can leave with a different speed relative to the Sun. It takes a tiny amount of the planet's orbital momentum, and the planet slows by an amount too small to measure.

In 1964 a young aerospace student, Gary Flandro, noticed that the four giant planets would line up in the late 1970s in a way that happens only about once every 175 years. A spacecraft launched at the right moment could visit all four, using each planet to sling it on to the next. NASA launched two spacecraft in 1977. Voyager 2 visited Jupiter (1979), Saturn (1981), Uranus (1986) and Neptune (1989), and remains the only spacecraft ever to visit Uranus or Neptune. Voyager 1 took a faster path out of the plane of the planets.

Today both are in interstellar space (Voyager 1 crossed the boundary of the Sun's bubble in 2012, Voyager 2 in 2018). Voyager 1 travels at about 17 km/s, or 3.6 AU a year (an AU is the Earth–Sun distance, about 150 million km). NASA expects it to be one light-day from Earth, about 173 AU, around November 2026. Its radio signals, from a transmitter with the power of a refrigerator bulb, now take almost a day to arrive. It also carries a golden record of sounds and images from Earth.

The fastest object ever built is the Parker Solar Probe, which used repeated Venus flybys to lose orbital energy and fall closer and closer to the Sun. On 24 December 2024 it passed 6.1 million km from the Sun's surface at about 192 km/s (692,000 km/h).

Part 4

The next star is very far

The nearest star beyond the Sun, Proxima Centauri, is 4.24 light-years away, which is about 268,000 AU, or more than 1,500 times farther than Voyager 1 has travelled in nearly fifty years. At Voyager's speed the trip takes about 75,000 years. Even the Parker Solar Probe's speed would take more than 6,000.

The most serious proposal so far is Breakthrough Starshot, announced in 2016: chips weighing a gram, attached to light sails and pushed by a huge array of lasers to 20% of the speed of light, reaching Proxima in about 20 years. It is a concept, not a project. Dust grains hitting a chip at 60,000 km/s, building a laser array of that power, and sending back a signal are all unsolved. Every other idea (fusion rockets, antimatter, enormous generation ships) is even further out. Einstein's relativity adds one more twist: at very high speed, clocks aboard the ship run slow, so the trip feels shorter to the travellers than to people on Earth. Try it in the lab.

Why it matters. The rocket equation is the reason we have been to the Moon, but nowhere further with people. It is not a technology problem to be solved with more money, but a physical limit to be worked around. New ideas have to change the exhaust speed or the propulsion method, not just the size.

Fire Newton's cannon

You launch a spacecraft sideways from 400 km above the Earth. Try different speeds. Air resistance is ignored. Speeds are in kilometres per second.

Result
Lowest point
Highest point
Time for one lap

The rocket equation

Choose an engine and how much of the rocket's mass is fuel. See the speed you can reach and how little is left at the end for payload.

Speed gained (delta-v)
Mass left at the end, as a share of launch mass

How long to the next star?

Proxima Centauri is 4.24 light-years away. Pick a speed. Times ignore the time spent speeding up and slowing down.

Trip time (Earth clock)
Time on the ship’s clock

Check yourself

Five questions.

Say it out loud

A younger friend asks: “Why don't astronauts in the space station fall down?” Answer without using the word zero-gravity. Use falling, sideways speed and orbit. Then explain why a rocket needs so much fuel, using the rocket equation.

Rabbit holes

The Oberth effectA rocket burn gives more speed when the spacecraft is already moving fast, deep in a gravity well. This is why the Parker Solar Probe and many deep-space missions burn near a planet and not far from it. Where does the extra energy come from?
Lagrange pointsFive places in the Sun–Earth system where gravity and orbital motion balance. The James Webb Space Telescope sits at the second one, 1.5 million km away. Why there?
Space elevatorsA cable from the ground to above geostationary orbit (the orbit 36,000 km up where a satellite stays over the same spot on Earth) would avoid rockets completely. No known material is strong enough yet at the length needed. Carbon nanotubes are candidates.
Solar sailsLight carries momentum. A very large, very light sail can use it, with no fuel. Japan’s IKAROS (2010) flew the first one between planets.
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