1. How much speed does Earth's spin really add at the equator and at Tanegashima?
The Earth turns once a day, so the ground is moving eastward. At the equator, the ground travels all the way around the planet (about 40,000 km) in a little under 24 hours, which works out to roughly 465 meters per second. Farther from the equator, the circle of latitude is smaller, so the ground moves more slowly. The speed shrinks in proportion to the cosine of the latitude, and it reaches zero at the poles. A rocket launched toward the east keeps that ground speed as a free head start [1].
Plugging in the latitudes gives about 463 m/s at Kourou in French Guiana (5.05° N), about 409 m/s at Cape Canaveral in Florida (28.5° N), and about 401 m/s at Tanegashima (30.4° N). These are my own calculations. ESA gives a similar figure for its own site, saying the Earth's rotation adds about 460 meters per second there [1].
The gap between Kourou and Tanegashima is about 62 m/s. A satellite in low orbit travels at around 7,800 m/s (a commonly quoted value), so the gap is roughly 0.8% of that. It is real, but it cannot be the whole reason that agencies prize sites near the equator. Something else must be doing most of the work.
2. Why a launch site's latitude limits how tilted or flat an orbit can be
That "something else" is the tilt of the orbit. A satellite's path around the Earth lies in a flat plane that passes through the Earth's center. The tilt of that plane compared with the equator is called the inclination. An orbit exactly above the equator has an inclination of 0°.
Many communications and weather satellites need a geostationary orbit, the one where a satellite seems to hover over one spot, about 36,000 km up. That orbit lies in the equator's plane, so its inclination is 0° [2]. But a rocket does not go straight to 36,000 km. It first leaves the satellite in an oval path called a geostationary transfer orbit, and the satellite then uses its own fuel to finish the trip [2].
Here is where the latitude matters. A rocket launched due east from a site cannot get into an orbit tilted less than the site's latitude. The orbital plane has to pass through both the launch site and the center of the Earth, and for a due-east launch that geometry sets the plane's minimum tilt. From Florida, at 28.5° north, the flattest orbit you can reach by launching due east is tilted about 28.5°. This is geometry I worked out myself, not a quotation. Launching in other directions can make the tilt larger, but not smaller.
To flatten the orbit onto the equator, something has to bend the path partway through the flight. A widely quoted description is that, from a site at about 28° north, putting a rocket into an equatorial orbit takes a costly "dogleg" maneuver, a bend in the flight path [3]. Bending the path means burning extra propellant that could otherwise have carried payload.
3. How being near the equator saves fuel, money, and satellite lifetime
From Kourou, which lies just over 500 km north of the equator, a launch needs to change very little to reach geostationary transfer orbit. ESA says this nearness means few changes have to be made to a satellite's path, and that together with the speed boost it saves fuel and money and prolongs the active life of satellites [1].
The reason fuel connects to lifetime is that a satellite carries only so much. Whatever it spends on fixing its orbit is no longer available for keeping itself in position later. ESA's statement says exactly that the savings prolong satellites' working lives [1]. How many extra years that adds depends on each satellite's design, so I do not put a number on it.
That brings us back to the opening question. The equator is valuable less because the rocket gets a push, and more because the satellite is spared a tilt-correcting burn that it would have to pay for out of its own tank.
4. Why Japan built its main launch site at Tanegashima, 30° north, anyway
Japan's Tanegashima Space Center sits on an island in southern Japan at about 30°24' north and 130°58' east. According to the Japanese-language Wikipedia article on the center (the page itself notes that it lacks citations, so treat this as reported rather than confirmed), two conditions guided the choice. First, launches toward the southeast had to be safe for land, sea, and air. Second, the site had to be as close to the equator as possible within Japan [4].
The same article says Tanegashima was not the southernmost place in Japan. The Ogasawara (Bonin) Islands, farther south, had only been returned to Japan in 1968, and Okinawa had not yet returned. So when the site was being planned, Tanegashima was reported to be the best available location under Japanese control [4]. In other words, it was a compromise between a southern latitude, open ocean to the east, and the borders of the time.
5. How Japan's H-IIA rocket makes up for Tanegashima's higher latitude
Rocket designers can partly make up for a launch site's latitude. A leaflet from JAXA, Japan's space agency, describes an upgrade to the second stage of the H-IIA rocket. The stage was changed so that it can fly for a long time in space and restart its engine, an idea called a long coast (coasting means flying with the engine off). In the leaflet's example, the engine fires near the lowest point of the transfer orbit, the stage coasts for about four hours with the satellite still attached, and then it fires again near the highest point before releasing the satellite [2].
The result is that the rocket can leave the satellite in an orbit closer to the final geostationary one. The satellite then needs less of its own fuel, and JAXA says the saved weight can go into a bigger sensor or into fuel for a longer life [2]. The leaflet does not mention latitude, so linking it to Tanegashima's position is my reading, not JAXA's words. It does show the same principle at work: fuel the rocket spends is fuel the satellite keeps.
6. Why the equator is helpful but not the only thing that makes a good launch site
Location is not just about the tilt. ESA points out that French Guiana is sparsely populated, that forests cover about 90% of the territory, and that it has no risk of cyclones. Its position also allows launches over a wide range of directions, from east to north [1]. Safe, open space to the east matters for the same reason at Tanegashima.
The equator also does not suit every mission. A satellite that circles the Earth from pole to pole needs to be launched north or south, where the Earth's spin gives no help. So the best site depends on where the satellite is going. For many satellites headed to the geostationary orbit, though, launching from near the equator is an advantage.
7. Try it yourself: measure the speed ratio with a globe and a piece of string
If you have a globe, use a piece of string to measure once around the equator. Then measure once around the circle of latitude at 30° north, the latitude of Tanegashima. The second string should be about 0.87 times as long as the first (the cosine of 30° is about 0.866).
Imagine spinning the globe once a day. The longer circle has to move faster to keep up. The ratio of the strings matches the ratio of the ground speeds: 401 divided by 465 is about 0.86. Now check an atlas for other launch sites, and look at whether they have open ocean to the east. What seems to matter most at each one, the tilt, the safety, or the direction it can launch?
Sources
The ground speeds for each site, the 62 m/s gap, the 0.8% figure, and the "orbit cannot be flatter than the latitude" rule are my own calculations and geometry, not quotations. The 7,800 m/s low-orbit speed is a commonly quoted value that I did not take from these sources. I could not find a primary source that gives the fuel cost of the tilt correction, so I give no number.
- European Space Agency, "Europe's Spaceport": https://www.esa.int/Enabling_Support/Space_Transportation/Europe_s_Spaceport/Europe_s_Spaceport2 (read in full: latitude 5°3', few changes to the trajectory, 460 m/s boost, fuel and money savings, longer satellite life, 102° launch angle, sparse population, no cyclones)
- JAXA, leaflet on the H-IIA second-stage upgrade (Japanese): https://fanfun.jaxa.jp/countdown/f29/files/flyer.pdf (read in full: geostationary orbit about 36,000 km up above the equator, transfer orbit, satellite uses its own fuel, long coast of about 4 hours, saved fuel and weight)
- "Near-equatorial orbit," Wikipedia: https://en.wikipedia.org/wiki/Near-equatorial_orbit (read in part: the costly dogleg for equatorial orbit from about 28° N. The statement comes through a footnote citing a NASA history, which I did not open, so it is stated as reported)
- "Tanegashima Space Center," Japanese Wikipedia (Japanese): https://ja.wikipedia.org/wiki/種子島宇宙センター (read in part: site-selection conditions and the Ogasawara and Okinawa timing. The page itself lacks citations and I did not confirm it against JAXA, so it is stated as reported)
Update history
- : First published.