# Orbiting Earth before heading to Moon

Each of the lunar Apollo missions (Apollo 8-17) entered Earth orbit immediately after launch. Each mission then left Earth after a few orbits by burning the S-IVB engine, and headed off to the Moon. (https://en.wikipedia.org/wiki/Apollo_program#Lunar_mission_profile)

The wikpedia page says orbiting Earth was necessary "to verify readiness of spacecraft systems", but I'm curious how this affected fuel requirements and other aspects of navigation. Would heading toward the Moon directly from the launch pad have required more or less fuel? If orbiting earth first is less efficient, how much extra fuel does it require over leaving directly?

• In addition to Russell's answer, note that in the event of a booster malfunction, at any point between Mode III and TLI, Earth orbit insertion was possible. Any kind of abort prior to TLI meant you lost the entire Moon mission (not even like Apollo 13 which at least rounded the Moon and got some snapshots of it), but going into an Earth parking orbit greatly lengthened the window where problems could be dealt with. (Compare Apollo 12: without parking orbit, that might have been an abort.)
– user
Commented Jan 15, 2016 at 10:06

Going from Earth's surface direct to Moon orbit without stopping in LEO would offer negligible savings -- depending on your assumptions, maybe 20 m/s worth of ∆v (and 2-3 hours worth of consumables).1

According to Apollo By The Numbers and Bob Braeunig's simulations, the ∆v budget for launch to orbit plus trans-lunar injection for the Apollo missions totalled about 12250 m/s, so any difference would be far less than 1% of the fuel budget.

1. Assuming ascent to circular orbit at the Kármán line in either case, then in the first case doing two Hohmann transfers, from Kármán line to 160km parking orbit then from parking orbit to lunar altitude; and in the second case a single Hohmann transfer from Kármán line to lunar altitude. The Apollo missions did a faster trajectory than Hohmann (saving 2 days travel time each way) but the difference between the parking orbit and non-stop versions is probably very similar.
• A Hohmann orbit from Earth to LEO isn't an option. Commented Jan 15, 2016 at 4:18
• @SamHallerman it is possible, but very ineffective as you fight the gravity all the way up. (I did it in Kerbal Space Program for example, needed a big rocket) Commented Jan 15, 2016 at 7:51
• @SamHallerman Space isn't like that.
– user
Commented Jan 15, 2016 at 9:59
• @SamHallerman the problem with space isn't getting high enough, it's getting fast enough. Picture one of those coin funnel things where you put a coin in the slot and it spirals faster and faster as it rolls into the middle. That's what a gravity well is like. If your coin could somehow speed up, it would spiral up out of the funnel instead of down into it. The Apollo craft did the same thing: they sped up to climb out of the Earth's gravity, until they got close enough to the Moon to fall into its (rather smaller) gravity well. Commented Jan 15, 2016 at 11:29
• @SamHallerman If you are interested in space orbit mechanics, play Kerbal Space Program (and kill a large number of Kerbals). The physics is far from perfect, but it is good enough. The experience of getting a space ship to orbit the Mun (the Moon), then return to Kerbal (Earth), in KSP is a real education; and, "cheating" by "not designing everything yourself" is encouraged (copy copy copy!), as the problem-space is rich enough that you need all the help you can get.
– Yakk
Commented Jan 15, 2016 at 19:23

The wikpedia page says orbiting Earth was necessary "to verify readiness of spacecraft systems", but I'm curious how this affected fuel requirements and other aspects of navigation.

The use of a parking orbit most likely saved fuel compared to a direct translunar insertion. A direct insertion into a translunar trajectory would have saved a tiny amount of fuel compared to that need by adding a parking orbit if everything went perfectly. However, nothing ever works perfectly. Rocket thrust varies, and navigation sensors are imperfect. Launch in the Apollo era was largely a dead reckoning process; there was no such thing as GPS in the Apollo era.

This meant that navigation errors built up during launch. A launch directly into a translunar trajectory would have meant correcting for those errors and the injection error after the launch+injection. This would have more than offset the tiny extra cost of placing the vehicle into a parking orbit before undergoing the translunar injection. With a parking orbit, most of the launch errors were corrected for by the translunar injection burn. Correction burns were still needed, but these were much smaller than those that would have been needed for a direct launch.

Much more importantly, the use of a parking orbit made the missions possible. A direct translunar insertion launch would have required an instantaneous launch window. The launch would have had to have been delayed by a day (or perhaps by several months) if something went wrong during the countdown in the case of a direct insertion into a translunar trajectory. Mission planners deemed that a 2.5 hour launch window was the minimum needed to have a reasonable chance of success. This alone ruled out the possibility of a launch directly into a translunar trajectory.

Something did indeed go wrong during the countdown in two of the Apollo missions. Apollo 14 launched 40 minutes late due to weather problems, and Apollo 17 launched 2 hours and 40 minutes late due to an automatic cutoff at the T-30 second mark.

That NASA used the parking orbit as a means for verifying the readiness of spacecraft systems for the continuation of the mission was an added benefit of using a parking orbit. This was not the primary driver. The primary driver was that the use of a parking orbit made the missions feasible.

• There was no GPS in the Apollo era, but there were the Transit satellites , a much simpler satellite navigation system.
– Uwe
Commented Nov 1, 2017 at 19:00
• @Uwe, Transit couldn't be used to locate a spacecraft. It used a combination of time, Doppler shift, and pattern of change in Doppler shift to determine the receiver location. This only works well when the receiver is stationary or nearly so: submarines get good accuracy, ships get reasonable accuracy, airplanes get poor accuracy, and Apollo could only tell that it was somewhere in the vicinity of Earth.
– Mark
Commented Sep 13, 2022 at 23:48
• @Mark Yes it is true, Transit was not useful for any spacecraft. If a submarine surfaced for only a short time to catch a single overflight of Transit, the submarine did not know if it was left or right of the Transit ground track. Two overflights were needed to exclude the wrong location.
– Uwe
Commented Sep 14, 2022 at 0:07

Achieving orbital velocity on earth's surface is not practical due to earth's atmosphere. First a ship must get above the atmosphere and then achieve orbital velocity.

Once altitude is gained, the most efficient way to achieve orbital velocity is by a horizontal burn. You could do the major burn along a non zero flight path angle but then the vertical component of the thrust suffers gravity loss.

Typically, the first part of a space ship's trajectory is nearly vertical but then leans to the east to give the thrust vector a bigger horizontal component as the atmosphere gets thinner.

When the ship's above the atmosphere it does the major burn and is traveling at a near zero flight path angle (In other words, horizontally).

So a direct insertion to lunar orbit would be doing burn to achieve 10.9 km/s horizontal velocity when above the atmosphere. But at sometime during this burn, the ship will be traveling at a horizontal velocity of 7.8 km/s. At this point I would say the ship is in orbit. After achieving orbital velocity the ship could keep on firing to achieve another 3.1 km/s for Trans Lunar Insertion (TLI).

Or it could cut off the engines after achieving orbital velocity and the do the remaining 3.1 km/s TLI burn later. What is the difference is delta V? Zero.

From John Schilling's launch simulator methodology pdf:

The Townsend technique begins by assuming that all space launches consist of a direct ascent to a low circular parking orbit, followed by a series of on-orbit maneuvers to the final destination orbit. In fact, many launch vehicles fly only a direct-ascent trajectory, even to a high or non- circular orbit. However, an observation of these trajectories almost invariably finds the launch vehicle, at an altitude of a few hundred kilometers, accelerating almost horizontally through the local circular orbit velocity. One may simplify the problem by treating this as an instantaneous "parking orbit", reached by direct ascent, and with all subsequent powered flight treated as an "on-orbit maneuver".