Mars Cycler
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A Mars cycler (or Earth–Mars cycler) is a kind of spacecraft
trajectory A trajectory or flight path is the path that an object with mass in motion follows through space as a function of time. In classical mechanics, a trajectory is defined by Hamiltonian mechanics via canonical coordinates; hence, a complete tra ...
that encounters
Earth Earth is the third planet from the Sun and the only astronomical object known to harbor life. While large volumes of water can be found throughout the Solar System, only Earth sustains liquid surface water. About 71% of Earth's surfa ...
and
Mars Mars is the fourth planet from the Sun and the second-smallest planet in the Solar System, only being larger than Mercury. In the English language, Mars is named for the Roman god of war. Mars is a terrestrial planet with a thin at ...
regularly. The term Mars cycler may also refer to a spacecraft on a Mars cycler trajectory. The Aldrin cycler is an example of a Mars cycler. Cyclers are potentially useful for transporting people or materials between those bodies using minimal propellant (relying on gravity-assist flybys for most trajectory changes) and can carry heavy radiation shielding to protect people in transit from
cosmic ray Cosmic rays are high-energy particles or clusters of particles (primarily represented by protons or atomic nuclei) that move through space at nearly the speed of light. They originate from the Sun, from outside of the Solar System in our own ...
s and solar storms.


Earth–Mars cyclers

A cycler is a
trajectory A trajectory or flight path is the path that an object with mass in motion follows through space as a function of time. In classical mechanics, a trajectory is defined by Hamiltonian mechanics via canonical coordinates; hence, a complete tra ...
that encounters two or more bodies regularly. Once the orbit is established, no propulsion is required to shuttle between the two, although some minor corrections may be necessary due to small perturbations in the orbit. The use of cyclers was considered in 1969 by Walter M. Hollister, who examined the case of an Earth–Venus cycler. Hollister did not have any particular mission in mind, but posited their use for both regular communication between two planets, and for multi-planet flyby missions. A Martian year is 1.8808 Earth years, so Mars makes eight orbits of the Sun in about the same time as Earth makes 15. Cycler trajectories between Earth and Mars occur in whole-number multiples of the
synodic period The orbital period (also revolution period) is the amount of time a given astronomical object takes to complete one orbit around another object. In astronomy, it usually applies to planets or asteroids orbiting the Sun, moons orbiting planets, ...
between the two planets, which is about 2.135 Earth years. In 1985,
Buzz Aldrin Buzz Aldrin (; born Edwin Eugene Aldrin Jr.; January 20, 1930) is an American former astronaut, engineer and fighter pilot. He made three spacewalks as pilot of the 1966 Gemini 12 mission. As the Lunar Module ''Eagle'' pilot on the 1969 A ...
presented an extension of his earlier Lunar cycler work which identified a Mars cycler corresponding to a single synodic period. The Aldrin cycler (as it is now known) makes a single eccentric loop around the Sun. It travels from Earth to Mars in 146 days (4.8 months), spends the next 16 months beyond the orbit of Mars, and takes another 146 days going from the orbit of Mars back to the first crossing of Earth's orbit. The existence of the now-eponymous Aldrin Cycler was calculated and confirmed by scientists at
Jet Propulsion Laboratory The Jet Propulsion Laboratory (JPL) is a federally funded research and development center and NASA field center in the City of La Cañada Flintridge, California, United States. Founded in the 1930s by Caltech researchers, JPL is owned by NASA an ...
later that year, along with the VISIT-1 and VISIT-2 cyclers proposed by John Niehoff in 1985. For each Earth–Mars cycler that is not a multiple of 7 synodic periods, an outbound cycler intersects Mars on the way out from Earth while an inbound cycler intersects Mars on the way in to Earth. The only difference in these trajectories is the date in the synodic period in which the vehicle is launched from Earth. Earth–Mars cyclers with a multiple of 7 synodic periods return to Earth at nearly the same point in its orbit and may encounter Earth and/or Mars multiple times during each cycle. VISIT 1 encounters Earth 3 times and Mars 4 times in 15 years. VISIT 2 encounters Earth 5 times and Mars 2 times in 15 years. Some possible Earth–Mars cyclers include the following: A detailed survey of Earth–Mars cycler trajectories was conducted by Ryan Russell and Cesar Ocampo from the
University of Texas at Austin The University of Texas at Austin (UT Austin, UT, or Texas) is a public research university in Austin, Texas. It was founded in 1883 and is the oldest institution in the University of Texas System. With 40,916 undergraduate students, 11,07 ...
,
Texas Texas (, ; Spanish: ''Texas'', ''Tejas'') is a state in the South Central region of the United States. At 268,596 square miles (695,662 km2), and with more than 29.1 million residents in 2020, it is the second-largest U.S. state by ...
. They identified 24 Earth-Mars cyclers with periods of two to four synodic periods, and 92 cyclers with periods of five or six synodic periods. They also found hundreds of non-ballistic cyclers, ones which would require some powered maneuvers.


Physics

Earth orbits the Sun in one Earth year, Mars in 1.881. Neither orbit is perfectly circular; Earth has an orbital eccentricity of 0.0168, and Mars of 0.0934. The two orbits are not quite coplanar either, as the orbit of Mars is inclined by 1.85 degrees to that of Earth. The effect of the gravity of Mars on the cycler orbits is almost negligible, but that of the far more massive Earth needs to be considered. If we ignore these factors, and approximate Mars's orbital period as 1.875 Earth years, then 15 Earth years is 8 Martian years. In the diagram opposite, a spacecraft in an Aldrin cycler orbit that starts from Earth at point E1 will encounter Mars at M1. When it gets back to E1 just over two Earth years later, Earth will no longer be there, but it will encounter Earth again at E2, which is 51.4^\circ, of an Earth orbit, further round. The shape of the cycler orbit can be obtained from the conic equation: :r = a\frac Where r is 1
astronomical unit The astronomical unit (symbol: au, or or AU) is a unit of length, roughly the distance from Earth to the Sun and approximately equal to or 8.3 light-minutes. The actual distance from Earth to the Sun varies by about 3% as Earth orbits ...
, a is the semi-major axis, \epsilon is the orbital eccentricity and \theta=-25.7^\circ (half of -51.4^\circ). We can obtain a by solving Lambert's problem with 51.4^\circ as the initial and final transfer angle. This gives: :a = 1.60 Solving the
quadratic equation In algebra, a quadratic equation () is any equation that can be rearranged in standard form as ax^2 + bx + c = 0\,, where represents an unknown value, and , , and represent known numbers, where . (If and then the equation is linear, not q ...
gives: :\epsilon = 0.393 with an orbital period of 2.02 years. The angle at which the spacecraft flies past Earth, \gamma, is given by: :\tan \gamma = \frac Substituting the values given and derived above gives a value for \gamma of 7.18^\circ. We can calculate the
gravity assist In orbital mechanics and aerospace engineering, a gravitational slingshot, gravity assist maneuver, or swing-by is the use of the relative movement (e.g. orbit around the Sun) and gravity of a planet or other astronomical object to alter the p ...
from Earth: :\Delta V = 2 V \sin \gamma where V is the heliocentric flyby velocity. This can be calculated from: :V = V_E\sqrt where is the velocity of Earth, which is 29.8 km/s. Substituting gives us V = 34.9 km/s, and V = 8.73 km/s. The excess speed is given by: :V_\infty = \sqrt Which gives a value for of 6.54 km/s. The turn angle \delta can be calculated from: :\Delta V = 2 V_\infty \sin \delta Which gives \delta = 41.9^\circ, meaning that we have an 83.8^\circ turn. The radius of closest approach to Earth will be given by: :\sin \delta = \frac Where is the gravitational constant of the Earth. Substituting the values gives = , which is bad because the radius of the Earth is . A correction would therefore be required to comfortably avoid the planet.


Proposed use

Aldrin proposed a pair of Mars cycler vehicles providing regular transport between Earth and Mars. While astronauts can tolerate traveling to the Moon in relatively cramped spacecraft for a few days, a mission to Mars, lasting several months, would require much more habitable accommodations for the much longer journey: Astronauts would need a facility with ample living space, life support, and heavy radiation shielding. A 1999 NASA study estimated that a mission to Mars would require lifting about into space, of which was propellant. Aldrin proposed that the costs of Mars missions could be greatly reduced by use of large space stations in cyclic orbits called ''castles''. Once established in their orbits, they would make regular trips between Earth and Mars without requiring any propellant. Other than consumables, cargo would therefore only have to be launched once. Two ''castles'' would be used, an outbound one on an Aldrin ''cycler'' with a fast transfer to Mars and long trip back, and an inbound one with fast trip to Earth and long return to Mars, which Aldrin called ''up and down escalators''. The astronauts would meet up with the cycler in Earth orbit and later Mars orbit in specialised craft called ''taxis''. One cycler would travel an outbound route from Earth to Mars in about five months. Another Mars cycler in a complementary trajectory would travel from Mars to Earth, also in about five months. Taxi and cargo vehicles would attach to the cycler at one planet and detach upon reaching the other. The cycler concept would therefore provide for routine, safe, and economical transport between Earth and Mars. A significant drawback of the ''cycler'' concept was that the Aldrin cycler flies by both planets at high speed. A taxi would need to accelerate to around Earth, and near Mars. To get around this, Aldrin proposed what he called a ''semi-cycler'', in which the ''castle'' would slow down around Mars, orbiting it, and later resume the ''cycler'' orbit. This would require fuel to execute the braking and re-cycling maneuvers. The castles could be inserted into cycler orbits with considerable savings in fuel by performing a series of low thrust maneuvers: The castle would be placed into an interim orbit upon launch, and then use an Earth- swing-by maneuver to boost it into the final cycler orbit. Assuming the use of conventional fuels, it is possible to estimate the fuel required to establish a cycler orbit. In the case of the Aldrin cycler, use of a gravity assist reduces the fuel requirement by about , or 15 percent. Other cyclers showed less impressive improvement, due to the shape of their orbits, and when they encounter the Earth. In the case of the VISIT-1 cycler, the benefit would be around , less than one percent, which would hardly justify the additional three years required to establish the orbit.


See also

* Interstellar cycler * Lunar cycler


Notes


References


Additional references

* * * * } * * * {{Portal bar, Solar System, Physics, Spaceflight Spaceflight concepts Missions to Mars Buzz Aldrin