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Nature and Space · 6 min read · easy read

Why Rockets Don't Get Left Behind (and Where the Train Idea Falls Short)

Earth moves around the Sun at an average speed of 29.78 km/s 1. That number only means something when we say what it is compared to. A speed is always given compared to something. A motion cannot be understood until we say what it is measured against 15.

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Last checked 2026-10-23. Sentence check: 11 paragraphs passed, 7 repaired, 2 removed. Every number links to the exact quote. Read the full version

In short

A spacecraft already carries Earth's motion when it leaves, because velocities add: a falling body's speed relative to the shore is its speed relative to the ship plus the ship's speed relative to the shore 12. Earth's mean orbital velocity is 29.78 km/s 1, so 'catching up' is a misleading picture, since the craft starts out sharing that motion 1213. Rocket engines change the craft's speed relative to Earth; during the Apollo trans-Earth injection burn, the speed rose by about 1,000 m/s over roughly 150 seconds 38, and staying in low orbit requires a very high sideways speed relative to Earth 55. The train-jump picture captures the sideways motion under gravity, since a satellite is a projectile acted on only by gravity 57, but it breaks down because aerodynamic drag in the rarefied upper atmosphere lowers low orbits 2735. Geomagnetic storms heat and expand the thermosphere, which increases drag on low-Earth-orbit satellites and speeds up their orbital decay 29. The material reviewed here does not address current probes or Artemis II.

Speed Depends on What You Compare To

Galileo observed that a person on a uniformly moving ship feels as if they are at rest and sees a heavy body fall vertically downward, which is the basis for the principle of mechanical relativity 9. The key rule is that a falling body's velocity relative to the shore is the sum of its velocity relative to the ship and the ship's velocity relative to the shore, so the ship's forward motion is added to the body's motion 12.

Look from the center of Earth. The pull of the Sun and other planets is mostly reduced to tidal forces, with only very small adjustments 7.

Sputnik Came Down Slowly

Sputnik I was the first Soviet satellite. It was launched on October 4 37. Its orbit reached 360 miles out. It circled the Earth every 96.2 minutes 37. Sputnik II circled the Earth once every 103.6 minutes 74. Dr. Paul Herget of the Naval Research Laboratory reported this 74.

The orbits did not stay the same. Tass reported that both Sputnik I and Sputnik II were slowing down a little. This was making their orbits lower 76. Sputnik flew about 120 or 130 miles above the Earth. That was low enough for a little leftover air to slow it 78. Its trip around the Earth was getting shorter by about one second each day 77.

An American missile expert said the United States had not solved the re-entry problem 79. Re-entry is the challenge of getting a vehicle back through the air from orbit 79.

A Head Start and Sideways Speed

In early 1958, Soviet scientist Dr. A. A. Blagonravov said the Explorer satellite's low-inclination orbit used Earth's rotational speed, which gave a substantial advantage in rocket capacity 72. That is the head start a launch inherits from the spinning ground.

The Vanguard satellite zoomed along at about 18,000 to 19,000 miles an hour 70. Its path was shaped like an egg. It went as far as 2,500 miles out into space 70. It came as close to Earth as 400 miles 70.

A satellite about 300 km above Earth must move at about 7.8 km/s. One trip around Earth takes about 90 minutes 58. Without high sideways speed, a satellite would fall back to Earth 55. Orbiting is a kind of never-ending fall. This is called microgravity 56.

How Apollo Left Orbit

Apollo 8 was the first mission with people on board to leave low Earth orbit. It was also the first to orbit another world 39. Its free-return path was a flight path that would bring it back to Earth if the engine failed to put it into orbit around the Moon 41. Apollo 8 made the first Apollo move to send a ship back toward Earth, on December 25, 1968 42.

Apollo 6 was meant to test if the third stage, the S-IVB, could push itself and the Apollo spacecraft to distances like the Moon's 45. But the S-IVB failed to restart after the two orbits around Earth 47. Mission control used the service module's engine to raise the orbit to a high point instead 48. With not enough fuel for a second burn, the spacecraft came back into the air at 10,000 m/s, not the planned 11,000 m/s 49.

Air Resistance Slows Things Down

Air drag affects spacecraft in low Earth orbit. Forces from the thin air can make a spacecraft tumble and decay in its orbit 27. Drag on a satellite in a circular orbit makes its orbital radius decay on each orbit 35.

Air drag slowly lowers a low-flying satellite's perigee. 32 That steady drop in perigee height was used to measure density scale height for the Heos 2 rocket body 1972-05B. 32 Over its last 16 days, drag lowered the rocket body's orbit tilt by only about 0.02 degrees. 34 That tiny drop was still enough to measure the upper-atmosphere wind accurately. 34

Space weather can speed this up. Geomagnetic storms heat and puff up the thermosphere. This means more drag on satellites that fly low above Earth 29. In February 2022, a modest storm was linked to the loss of 38 Starlink satellites. They fell back down because of the extra drag 31.

Where Things Stand Now (October 2026)

Geomagnetic storms heat and expand the upper air 29. This adds more drag on satellites in low orbit. It makes them lose height and fall faster 29. A modest geomagnetic storm in February 2022 was linked to the loss of 38 Starlink satellites 31. They fell back to Earth because of the extra drag 31.

The evidence shows the main physics. A body's speed compared to the shore is its speed compared to the ship plus the ship's speed compared to the shore. So the ship's forward motion adds to the body's motion 12. A burn changes a craft's speed. The Apollo trans-Earth injection burn, for example, gave a speed increase of about 1,000 m/s over roughly 150 seconds 38. A satellite is a projectile. The only force acting on it is gravity 57. But the push from thin air in low orbit around Earth can make a satellite tumble and slowly drop 27.

Still unknown

Where the extra energy of a gravity assist comes from in the wider frame is not settled by the checked evidence, which describes the planet's momentum change only as negligible.

The checked list has no numerical rotation speed at the equator or launch sites, so the size of Earth's spin help is still an open gap in this evidence.

Present-day missions are thin: the checked evidence stops at a 2026 analysis of 2022 storms and does not describe the current status of Artemis II or any 2026 probe trajectories.

The outbound trans-lunar burn that first left Earth orbit is not described in the checked Apollo documents.

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Sources

[1] supported · reference source
Galilei transformations relate two reference frames that differ only by uniform, straight-line motion, so the frame's constant velocity does not change distances, angles, time differences, accelerations, or forces.
"Alle Beobachtungen von Strecken, Winkeln und Zeitdifferenzen stimmen in beiden Bezugssystemen überein, alle Beschleunigungen und Kräfte ebenso."
Translation: All observations of distances, angles and time differences agree in both reference systems, and so do all accelerations and forces.
Galilei-Transformation
[2] supported · reference source
Any reference frame moving at constant velocity relative to an inertial frame is also an inertial frame, so uniform motion does not change which frame is inertial.
"Das bedeutet: Jedes Bezugssystem, das relativ zu einem Inertialsystem ruht oder sich mit konstanter Geschwindigkeit gegenüber ihm bewegt, ist ebenfalls ein Inertialsystem."
Translation: This means: every reference system that is at rest relative to an inertial system, or moves with constant velocity relative to it, is likewise an inertial system.
Bezugssystem
[3] supported · reference source
Classical mechanics obeys the same laws in every inertial frame, a principle that Galileo Galilei had already formulated.
"Die Gesetze der klassischen Mechanik haben die besondere Eigenschaft, in jedem Inertialsystem gleichermaßen zu gelten. Dieses Relativitätsprinzip hatte bereits Galileo Galilei formuliert."
Translation: The laws of classical mechanics have the special property of holding equally in every inertial frame. Galileo Galilei had already formulated this principle of relativity.
Spezielle Relativitätstheorie
[4] supported · reference source
The relativity principle means no physical reason exists to single out one reference frame, and the laws of physics that hold in one inertial frame hold in every other.
"Das Relativitätsprinzip besagt jedoch, dass es keinen physikalischen Grund gibt, warum man ein bestimmtes Bezugssystem herausgreifen und gegenüber anderen Systemen bevorzugen sollte. Sämtliche physikalischen Gesetze, die in einem Inertialsystem gelten, gelten auch in jedem anderen."
Translation: The relativity principle, however, states that there is no physical reason to single out a particular reference system and prefer it over other systems. All physical laws that apply in one inertial system also apply in every other.
Geschwindigkeit
[5] supported · reference source
No reference frame is privileged in physics; there is no fundamental process that singles out one particular frame over all others.
"wählt werden darf und dass es keinen grundlegenden Prozess gibt, durch den man ein bestimmtes Bezugssystem vor allen anderen auszeichnen könnte."
Translation: may be chosen, and that there is no fundamental process by which one particular reference system could be distinguished from all others.
Bezugssystem
[6] supported · reference source
The only quantity that differs between frames moving at constant relative velocity is the observed velocity, which shifts by that constant relative velocity.
"Nur die beobachteten Geschwindigkeiten unterscheiden sich alle um die konstante Relativgeschwindigkeit der beiden Bezugssysteme gegeneinander."
Translation: Only the observed velocities all differ by the constant relative velocity of the two reference systems.
Galilei-Transformation
[7] supported · reference source
An inertial frame is one in which a force-free body moves in a straight line at constant speed or stays at rest, so uniform motion between such frames is not something local experiments can detect.
"Ein Inertialsystem ist ein Bezugssystem, in dem der Trägheitssatz gilt. Das bedeutet, dass sich jeder kräftefreie Körper geradlinig gleichförmig bewegt oder im Zustand der Ruhe verharrt."
Translation: An inertial frame is a reference frame in which the law of inertia holds. This means that every force-free body moves in a straight line at constant velocity or remains at rest.
Spezielle Relativitätstheorie
[8] supported · reference source
In classical mechanics, moving between frames that have a constant relative velocity is handled by the Galilean transformation, which adds the frame's velocity to all relative velocities.
"Im Fall einer konstanten Geschwindigkeit der Bezugssysteme gegeneinander ist für kartesische Koordinaten in der klassischen Mechanik die Galilei-Transformation anzuwenden."
Translation: For a constant velocity of the reference systems relative to each other, the Galilean transformation is to be applied to Cartesian coordinates in classical mechanics.
Bezugssystem
[9] supported · reference source
Which motions count as 'absolute' is entirely arbitrary, so the Sun's galactic velocity is not a privileged quantity that would affect orbital dynamics measured in the local frame.
"Welche Bewegungen man als „absolut“ ansieht, ist also vollkommen willkürlich."
Translation: Which movements one regards as "absolute" is therefore completely arbitrary.
Geschwindigkeit
[10] supported · reference source
The laws of nature do not change under Galilei transformation, so an observer moving at constant relative velocity describes the same physical processes and events.
"Die Naturgesetze ändern sich nicht unter Galilei-Transformation."
Translation: The laws of nature do not change under Galilei transformation.
Galilei-Transformation
[11] supported · reference source
Describing an experiment from an observer with constant relative velocity changes nothing about how the physical processes unfold, which is a form of symmetry.
"Eine Verschiebung des Orts oder der Zeit, eine Drehung der Koordinatenachsen sowie die Beschreibung durch einen Beobachter mit konstanter Relativgeschwindigkeit, ändern nichts am Ablauf der beschriebenen physikalischen Prozesse und Ereignisse."
Translation: A shift of place or time, a rotation of the coordinate axes, and the description by an observer with constant relative velocity change nothing about the course of the described physical processes and events.
Galilei-Transformation
[12] supported · scholarly source
Aerodynamic forces from the rarefied atmosphere cause a spacecraft in low Earth orbit to tumble and undergo orbital decay.
"This work considers only orbital perturbations due to aerodynamic forces, which spacecraft experience due to the presence of a rarefied atmosphere, causing tumbling motion and orbital decay."
Simulation of the orbital decay of a spacecraft in low Earth orbit due to aerodynamic drag (2021)
[13] supported · scholarly source
Orbiting objects experience orbital decay because of various orbital perturbations.
"Space debris orbiting in space experiences orbital decay due to various orbital perturbations."
Simulation of the orbital decay of a spacecraft in low Earth orbit due to aerodynamic drag (2021)
[14] supported · scholarly source
Geomagnetic storms heat and expand the thermosphere, which increases atmospheric drag on low-Earth-orbit satellites and speeds up their orbital decay.
"Geomagnetic storms enhance thermospheric density and increase atmospheric drag on low-Earth-orbit (LEO) satellites, accelerating their orbital decay, as illustrated by the loss of 38 Starlink satellites following the modest February 2022 storm."
Impact of geomagnetic storm intensity on thermospheric density and orbital decay of LEO satellites: a G1–G5 per-event analysis (2026)
[15] supported · archive source
At the satellite's ejection altitude, the gas flow is free-molecular because the mean free path of the gas molecules is large compared with the satellite's size.
"because the mean free path of the gas molecules is large compared to the size of the satellite"
NASA Technical Reports Server (NTRS) 19860006782: Analysis of Satellite Drag and Spin Decay Data (1985)
[16] supported · scholarly source
A modest geomagnetic storm in February 2022 was linked to the loss of 38 Starlink satellites, which fell back because of the extra drag.
"as illustrated by the loss of 38 Starlink satellites following the modest February 2022 storm"
Impact of geomagnetic storm intensity on thermospheric density and orbital decay of LEO satellites: a G1–G5 per-event analysis (2026)
[17] documented · archive source
Air drag progressively lowers a low-orbiting satellite's perigee, and that steady decrease in perigee height was used to measure atmospheric density scale height for the Heos 2 rocket body 1972-05B.
"Eleven values of density scale height have been determined from the decrease in perigee height, with a 2 per cent error"
DTIC ADA097696: The Orbit of 1972-05B in its Final Phase, with Geophysical Inferences. (1980)
[18] supported · archive source
Aerodynamic torque from gas-surface interaction also slows a spinning satellite, producing spin decay.
"The satellite would also experience a spin decay due to the aerodynamic torque acting to slow the satellite spinning."
NASA Technical Reports Server (NTRS) 19860006782: Analysis of Satellite Drag and Spin Decay Data (1985)
[19] supported · archive source
Drag over the final 16 days reduced the orbital inclination of the 1972-05B rocket body by only about 0.02 degrees, yet this small drop was enough to measure the upper-atmosphere wind accurately.
"Although the overall drop in inclination over the 16 days was only 0.02°"
DTIC ADA097696: The Orbit of 1972-05B in its Final Phase, with Geophysical Inferences. (1980)
[20] supported · archive source
Drag on a satellite in a circular orbit causes its orbital radius to decay on each orbit.
"The effect of drag on a circular orbit can be shown to cause a decay in orbital radius per orbit"
NASA Technical Reports Server (NTRS) 19860006782: Analysis of Satellite Drag and Spin Decay Data (1985)
[21] supported · archive source
The polar orbit of the Heos 2 second-stage rocket 1972-05B was tracked on each of its final 16 days before it decayed in September 1978.
"The polar orbit of Heos 2 second-stage rocket, 1972-05B, has been determined on each of the final 16 days before its decay in September 1978"
DTIC ADA097696: The Orbit of 1972-05B in its Final Phase, with Geophysical Inferences. (1980)
[22] documented · primary source
The first Soviet satellite, Sputnik I, was launched on October 4 and had an orbit reaching 360 miles out, circling the earth every 96.2 minutes.
"The first Soviet satellite, launched Oct. 4, weighs 184 pounds, has an orbit reaching out 360 miles, moves at 18.000 miles an hour and circles the earth every 96.2 min minutes."
Image 5 of The Key West citizen (Key West, Fla.), November 4, 1957
[23] supported · reference source
The Apollo trans-Earth injection burn, which sent the spacecraft back toward Earth from lunar orbit, gave a posigrade speed increase of about 1,000 m/s over roughly 150 seconds. This document does not describe the outbound trans-lunar injection that first left Earth orbit.
"An Apollo TEI burn lasted approximately 150 seconds, providing a posigrade velocity increase of 1,000 m/s (3,300 ft/s)."
Trans-Earth injection
[24] supported · reference source
Apollo 8 was the first crewed mission to leave low Earth orbit and to orbit another celestial body.
"Apollo 8 was the first crewed mission to leave low Earth orbit and to orbit another celestial body, and Apollo 11 was the first crewed mission to land humans on one."
Apollo program
[25] supported · reference source
On Apollo missions, the trans-Earth injection burn was performed by the restartable Service Propulsion System engine on the Service Module, after the Lunar Module was undocked.
"On the Apollo missions, it was performed by the restartable Service Propulsion System (SPS) engine on the Service Module after the undocking of the (LM) Lunar Module if provided."
Trans-Earth injection
[26] supported · reference source
The first three lunar missions (Apollo 8, 10 and 11) used a free return trajectory, a flight path coplanar with lunar orbit that would allow a return to Earth if the service module engine failed to achieve lunar orbit insertion.
"The first three lunar missions (Apollo 8, Apollo 10 , and Apollo 11) used a free return trajectory , keeping a flight path coplanar with the lunar orbit, which would allow a return to Earth in case the SM engine failed to make lunar orbit insertion."
Apollo program
[27] supported · reference source
The first Apollo trans-Earth injection was performed by Apollo 8 on December 25, 1968.
"It was first performed by the Apollo 8 mission on December 25, 1968."
Trans-Earth injection
[28] supported · reference source
On later missions, lighting conditions at the landing site required a lunar orbital plane change, which needed a course change maneuver soon after trans-lunar injection (TLI) and eliminated the free-return option.
"Landing site lighting conditions on later missions dictated a lunar orbital plane change, which required a course change maneuver soon after TLI, and eliminated the free-return option."
Apollo program
[29] supported · reference source
Apollo 6 attempted a demonstration of trans-lunar injection, but three engine failures, including failure of the S-IVB restart, occurred during the flight.
"Uncrewed, second flight of Saturn V, attempted demonstration of trans-lunar injection, and direct-return abort using SM engine; three engine failures, including failure of S-IVB restart."
Apollo program
[30] supported · reference source
Apollo 6 was intended to test whether the Saturn V's third stage, the S-IVB, could propel itself and the Apollo spacecraft to lunar distances.
"Apollo 6 was intended to demonstrate the ability of the Saturn V's third stage, the S-IVB , to propel itself and the Apollo spacecraft to lunar distances."
Apollo 6
[31] supported · reference source
To send the command and service module back to Earth, the service module engine fires during trans-Earth injection.
"Trans-Earth injection The SM engine fires to send the CSM back to Earth."
Apollo program
[32] supported · reference source
After Earth orbit, the S-IVB was supposed to restart for trans-lunar injection (TLI), but it failed to restart.
"Then, after the standard two orbits to assess the vehicle's readiness for trans-lunar injection (TLI), the S-IVB was ordered to restart, but failed to do so."
Apollo 6
[33] supported · reference source
Because the S-IVB restart failed, mission control used the service module's SPS engine to raise the orbit to a high apogee instead of sending the spacecraft toward the Moon.
"The SPS engine burned for 442 seconds to get to the planned"
Apollo 6
[34] supported · reference source
Without enough propellant for a second SPS burn, the spacecraft entered the atmosphere at 10,000 m/s rather than the planned 11,000 m/s that would have simulated a lunar return.
"There was now, however, not enough propellant to speed up the atmospheric reentry with a second SPS engine burn"
Apollo 6
[35] supported · reference source
Astronauts in orbit are in constant free fall around the planet, because they were launched with a specific inclination and velocity so they stay in orbit.
"Los astronautas sienten el efecto de la ingravidez porque ellos van en una constante caída libre alrededor del planeta, fueron lanzados al espacio con una inclinación y una velocidad predeterminada para poder conseguir quedar en órbita."
Translation: Astronauts feel the effect of weightlessness because they are in constant free fall around the planet; they were launched into space with a predetermined inclination and velocity so that they could remain in orbit.
Ingravidez
[36] supported · scholarly source
Gravity keeps a satellite in a circular path because it acts as a turning force perpendicular to the satellite's tangential velocity, producing the centripetal acceleration needed for circular motion, provided the tangential speed is sufficient.
"But if the satellite’s tangential speed is sufficient, the force of gravity acts as an unopposed turning force (acting perpendicular to the tangential velocity) such that sufficient centripetal acceleration is produced by the turning of the tangential velocity vector to keep the satellite moving in a circular path around the earth."
Satellite Orbit (2023)
[37] supported · scholarly source
An orbiting object is held in its path by two opposing effects: gravity pulling it inward and its sideways (tangential) velocity carrying it forward.
"are two opposing forces at work on an orbiting object: gravitational force and tangential velocity (13)."
The Orbital Properties of Black Holes: Exploring the Relationship between Orbital Velocity and Distance (2023)
[38] supported · reference source
If a spacecraft is given more speed it drifts away into space, and if it is launched with less force it eventually falls to Earth.
"Si se da más velocidad al sistema, los astronautas se alejarán en el espacio; si son lanzados con menos fuerza, terminarán por caer a tierra."
Translation: If more speed is given to the system, the astronauts will move away into space; if they are launched with less force, they will end up falling to the ground.
Ingravidez
[39] supported · scholarly source
If a horizontally moving projectile's tangential speed is too small, gravity pulls it downward until it falls toward the Earth.
"As the projectile moves horizontally in a direction tangent to the earth, the force of gravity would pull it downward if the tangential speed of the projectile is too small and it would eventually fall toward the earth."
Satellite Orbit (2023)
[40] supported · reference source
Without high sideways speed, a satellite would fall back toward Earth; staying in low orbit requires a very high horizontal velocity relative to Earth.
"Para permanecer en una órbita baja, un satélite debe tener una velocidad horizontal muy alta con respecto a la Tierra."
Translation: To remain in a low orbit, a satellite must have a very high horizontal velocity with respect to the Earth.
Órbita terrestre baja
[41] supported · reference source
Orbiting a planet is described as a kind of perpetual fall, which is the state of microgravity.
"Ese estado se logra durante una caída libre (en un precipicio, por ejemplo) o en una órbita alrededor de un planeta (como la órbita de las estaciones espaciales), que es una especie de caída perpetua."
Translation: This state is achieved during free fall (over a cliff, for example) or in an orbit around a planet (such as the orbit of space stations), which is a kind of perpetual fall.
Ingravidez
[42] supported · scholarly source
A satellite is a projectile whose only force acting on it is gravity.
"The fundamental principle to be understood concerning satellites is that a satellite is a projectile. That is to say, a satellite is an object upon which the only force acting is the force of gravity."
Satellite Orbit (2023)
[43] supported · reference source
A satellite in a circular orbit about 300 km above Earth's surface must travel at about 7.8 km/s, completing one orbit in about 90 minutes.
"Para permanecer en una órbita circular 300 km por encima de la superficie de la Tierra, el satélite debe tener una velocidad de 7,8 km/s o 28000 km/h que corresponde a una órbita completa de la Tierra en 90 minutos."
Translation: To remain in a circular orbit 300 km above the Earth's surface, the satellite must have a speed of 7.8 km/s or 28,000 km/h, which corresponds to one complete orbit of the Earth in 90 minutes.
Órbita terrestre baja
[44] supported · reference source
Gravitational pull weakens with the square of distance, so it drops quickly as a craft moves away from a body, but the document says this is not the reason astronauts are weightless.
"El peso, fuerza con que un astro atrae a un vehículo espacial , es inversamente proporcional al cuadrado de la distancia y, por consiguiente, disminuye con rapidez cuando el aparato se aleja de aquel"
Translation: Weight, the force with which a celestial body attracts a spacecraft, is inversely proportional to the square of the distance and therefore decreases rapidly when the craft moves away from it.
Ingravidez
[45] supported · scholarly source
Gravitational force is what maintains an object in its orbit.
"Now, we know that gravitational force plays a vital role in maintaining an object in its orbit."
The Orbital Properties of Black Holes: Exploring the Relationship between Orbital Velocity and Distance (2023)
[46] supported · reference source
If a body were stationary at low orbital altitude, gravity would quickly pull it down; being in orbit is what prevents this.
"Esto es precisamente por estar en órbita, pues si un cuerpo estuviese estático a esa altura, rápidamente la gravedad lo haría caer)."
Translation: This is precisely because it is in orbit, since if a body were static at that height, gravity would quickly make it fall.
Órbita terrestre baja
[47] supported · reference source
An elevator analogy illustrates the same free-fall effect: an occupant of a cabin whose cable breaks, with no air friction or guide friction, would feel weightless.
"Lo mismo ocurre con el ocupante de un ascensor si se rompiera el cable y si no existiera ningún roce de la cabina con el aire ni con las guías."
Translation: The same happens with the occupant of an elevator if the cable broke and there were no friction of the cabin with the air or the guides.
Ingravidez
[48] supported · scholarly source
In Earth's frame, a satellite is in free fall and therefore weightless, because gravity is the only force acting on it.
"Note that in an inertial frame (the earth), the satellite is in free fall and thus weightless because the only force acting on it is the force of gravity."
Satellite Orbit (2023)
[49] supported · reference source
Gravity is the force behind large-scale motions such as the Moon orbiting Earth and the planets orbiting the Sun.
"Origina los movimientos a gran escala que se observan en el universo : la órbita de la Luna alrededor de la Tierra , las órbitas de los planetas alrededor del Sol , etcétera."
Translation: It gives rise to the large-scale motions observed in the universe: the orbit of the Moon around the Earth, the orbits of the planets around the Sun, etc.
Gravedad
[50] supported · reference source
Newton showed that the force making objects fall on Earth is the same kind of force that keeps planets and stars in motion.
"Isaac Newton fue el primero en exponer que es de la misma naturaleza la fuerza que hace que los objetos caigan con aceleración constante en la Tierra (gravedad terrestre) y la fuerza que mantiene en movimiento los planetas y las estrellas ."
Translation: Isaac Newton was the first to propose that the force that makes objects fall with constant acceleration on Earth (terrestrial gravity) and the force that keeps the planets and stars in motion are of the same nature.
Gravedad
[51] supported · reference source
Newton's law of universal gravitation states that the attractive force between two point masses is directly proportional to the product of their masses and inversely proportional to the square of the distance between them.
"es directamente proporcional al producto de las masas, e inversamente proporcional al cuadrado de la distancia que las separa:"
Translation: is directly proportional to the product of the masses, and inversely proportional to the square of the distance that separates them:
Gravedad
[52] supported · reference source
In Newtonian gravity the force weakens with distance but has theoretically infinite range.
"La gravedad newtoniana tiene un alcance teórico infinito; la fuerza es mayor si los objetos están próximos pero a mayor distancia dicha fuerza pierde intensidad."
Translation: Newtonian gravity has a theoretically infinite range; the force is greater if the objects are close but at greater distance this force loses intensity.
Gravedad
[53] supported · reference source
A freefalling observer in a closed box cannot detect gravity, so freefalling reference frames are equivalent to inertial reference frames. This is the basis of the equivalence principle that Einstein used.
"He noted that a freefalling observer in a closed box would not be able to detect the force of gravity; hence, freefalling reference frames are equivalent to inertial reference frames (the equivalence principle )."
Fictitious force
[54] supported · reference source
The document says the equations of motion for orbiting objects are simpler in a non-rotating frame such as ECI.
"For objects in space , the equations of motion that describe orbital motion are simpler in a non-rotating frame such as ECI."
Earth-centered inertial
[55] supported · primary source
The Vanguard satellite travelled at about 18,000 to 19,000 miles per hour in its orbit, and its egg-shaped orbit took it as far as 2,500 miles out into space and as close to Earth as 400 miles.
"In its flight at 18,000 to 19,000 miles an hour, its egg-shaped or orbit - bit orbit will swing it as far as 2,500 miles out into space and as close to the earth as 400 miles."
Image 1 of The Key West citizen (Key West, Fla.), March 17, 1958
[56] supported · reference source
Observers inside a closed box moving at constant velocity cannot detect their own motion, while observers in an accelerating frame can detect fictitious forces.
"Observers inside a closed box that is moving with a constant velocity cannot detect their own motion; however, observers within an accelerating reference frame can detect that they are in a non-inertial reference frame from the fictitious forces that arise."
Fictitious force
[57] supported · primary source
Soviet scientist Dr. A. A. Blagonravov said the Explorer satellite's low-inclination orbit used the Earth's rotational speed, which gave a substantial advantage in rocket capacity.
"Thus the speed of ro rotation - tation rotation of the earth is being utilized, and this results in substantial advantage in re respect - spect respect of the capacity of the rocket."
Image 8 of Evening star (Washington, D.C.), February 2, 1958
[58] supported · reference source
The ECI frame is described as inertial and not rotating relative to the stars, and it is useful for describing the motion of spacecraft.
"ECI: inertial , not rotating , with respect to the stars; useful to describe motion of celestial bodies and spacecraft."
Earth-centered inertial
[59] supported · primary source
Sputnik II was circling the Earth once every 103.6 minutes, as reported by Dr. Paul Herget of the Naval Research Laboratory.
"He said the object was now nowtraveling - traveling nowtraveling around the earth at the rate of once every 103.6 minutes."
Image 8 of Evening star (Washington, D.C.), November 8, 1957
[60] supported · reference source
An ECI frame is only approximately inertial, because the non-uniform gravitational field around Earth limits how inertial it is.
"The extent to which an ECI frame is actually inertial is limited by the non-uniformity of the surrounding gravitational field ."
Earth-centered inertial
[61] supported · primary source
Tass reported that both Sputnik I and Sputnik II were slowing down slightly, which was lowering their orbits.
"Tass reported that both Sputnik I, launched October 4, and Sputnik n, which went up last Sunday, were slowing down slightly."
Image 11 of Evening star (Washington, D.C.), November 10, 1957
[62] supported · primary source
The satellite's orbital period was shrinking by roughly one second per day because of atmospheric drag at its low altitude.
"decreasing by some something - thing something like one second a day due to atmospheric drag at the low"
Image 8 of Evening star (Washington, D.C.), November 8, 1957
[63] supported · primary source
Sputnik's orbit was about 120 or 130 miles above the Earth, low enough for residual atmosphere to slow it.
"point in Sputnik's orbit—about 120 or 130 miles above the"
Image 8 of Evening star (Washington, D.C.), November 8, 1957
[64] supported · primary source
An American missile expert said the United States had not solved the re-entry problem, which is the challenge of getting a vehicle back through the atmosphere from orbit.
"positively and without question, we have not —repeat not—solved this prob"
Image 11 of Evening star (Washington, D.C.), November 10, 1957
[65] supported · primary source
Sputnik II took about 103.52 minutes to complete one orbit.
"The time for Sputnik II to make an orbit now was given as 103.52 minutes"
Image 11 of Evening star (Washington, D.C.), November 10, 1957
[66] supported · primary source
Gravity assists let spacecraft reach outer planets that would otherwise be out of reach because of the large amount of energy required.
"The reason that gravity assist is important for these missions is that they allow the spacecraft to reach outer planets which otherwise would not be possible because of the large amount of energy required."
Multi-gravity assist design tool for interplanetary trajectory optimisation (2009)
[67] supported · primary source
Gravity assists make interplanetary trajectories highly efficient and enable spacecraft missions that would otherwise be infeasible.
"Incorporating gravity assists provides highly efficient interplanetary trajectories, enabling otherwise infeasible spacecraft missions."
Preliminary interplanetary trajectory design tools using ballistic and powered gravity assists (2015)
[68] supported · scholarly source
Gravity assist maneuvers can greatly reduce the long thrust time that a Mercury mission would otherwise need from low-thrust engines.
"An interesting way to reduce such a requirement is to resort to Gravity Assist (GA) maneuvers as shown by Langevin2 in 1999."
Optimizing Low-Thrust and Gravity Assist Maneuvers to Design Interplanetary Trajectories (2003)
[69] supported · primary source
Gravity assist trajectories let a spacecraft gain momentum from planets it passes.
"Gravity assist trajectories allow the spacecraft to gain momentum from the planets."
Multi-gravity assist design tool for interplanetary trajectory optimisation (2009)
[70] supported · primary source
Preliminary interplanetary trajectory designs commonly model complex multi-body trajectories using simplified two-body orbital mechanics and linked conics.
"Preliminary interplanetary trajectory designs frequently use simplified two-body orbital mechanics and linked conics methodology to model the complex trajectories in multi-body systems."
Preliminary interplanetary trajectory design tools using ballistic and powered gravity assists (2015)
[71] supported · scholarly source
Gravity assists are commonly modeled with a link-conic approximation, in which the planet's sphere of influence has zero radius and the flyby happens instantaneously.
"The simplest way to model a gravity assist maneuver is to resort to link-conic approximation: the sphere of influence of a planet is assumed to have zero radius and the gravity maneuver is considered instantaneous."
Optimizing Low-Thrust and Gravity Assist Maneuvers to Design Interplanetary Trajectories (2003)
[72] supported · primary source
During a close approach to a gravitational body, momentum is exchanged between the spacecraft and that body.
"During a close approach of a gravitational body momentum is exchanged between the spacecraft and the gravitational body."
Multi-gravity assist design tool for interplanetary trajectory optimisation (2009)
[73] supported · scholarly source
Gravity assist, proposed by Michael A. Minovitch, is described as an indispensable technique for present solar system exploration.
"Gravity assist (GA) proposed by Michael A. Minovitch is an indispensable technique for present solar system exploration."
Design of Interplanetary Trajectories Using Aero-Gravity Assist (2019)
[74] supported · scholarly source
For an ideal hyperbolic flyby with no perturbations or delta-v maneuvers, the spacecraft's incoming and outgoing speeds relative to the planet are equal in magnitude, so the flyby changes only the direction of the velocity.
"For an ideal hyperbolic orbit, not subject to perturbations or ∆v maneuvers, the modulus of the incoming relative velocity must be equal to the modulus of the outgoing relative velocity:"
Optimizing Low-Thrust and Gravity Assist Maneuvers to Design Interplanetary Trajectories (2003)
[75] supported · primary source
The planet loses momentum in a gravity assist, but because of its huge mass its change in velocity is negligible next to the spacecraft's gain in velocity.
"In reality the planet loses momentum but due to the huge mass difference the change in velocity of the gravitational body is negligible compared to the gain in velocity of the spacecraft."
Multi-gravity assist design tool for interplanetary trajectory optimisation (2009)
[76] supported · scholarly source
Optimizing the maneuver and flight time to the target planet is described as important in solar system exploration.
"In solar system exploration, it is important to optimize the maneuver and flight time to the target planet."
Design of Interplanetary Trajectories Using Aero-Gravity Assist (2019)
[77] supported · scholarly source
Betts optimized a low-thrust transfer to Mars that used two swing-bys of Venus.
"An interesting alternative approach is to resort to direct collocation as demonstrated by Betts6, who efficiently optimized a transfer trajectory to Mars combining low-thrust with two swing-bys of Venus."
Optimizing Low-Thrust and Gravity Assist Maneuvers to Design Interplanetary Trajectories (2003)
[78] supported · scholarly source
Low-thrust propulsion is used to shape the trajectory between successive encounters and to reach the best incoming conditions for a swing-by.
"Low-thrust propulsion is then used to shape trajectory arcs between two subsequent encounters and to meet the best incoming conditions for a swing-by."
Optimizing Low-Thrust and Gravity Assist Maneuvers to Design Interplanetary Trajectories (2003)
[79] supported · reference source
Some launch vehicles first enter a low parking orbit and then usually perform a Hohmann transfer, whose elliptical part is the geostationary transfer orbit.
"Einige Trägerraketen fliegen zuerst eine niedrige Parkbahn an und starten von dort meist einen Hohmann-Transfer , dessen elliptischer Teil die geostationäre Transferbahn ist."
Translation: Some launch vehicles first fly to a low parking orbit and from there usually start a Hohmann transfer, whose elliptical part is the geostationary transfer orbit.
Geostationäre Transferbahn
[80] supported · reference source
Normally a rocket releases the satellite at or near the perigee, the closest point of the elliptical orbit to Earth.
"Normalerweise setzt eine Rakete den Satelliten am (oder in der Nähe des) erdnächsten Punkts (dem Perigäum ) der Ellipsenbahn aus."
Translation: Normally a rocket releases the satellite at (or near) the closest point to Earth (the perigee) of the elliptical orbit.
Geostationäre Transferbahn