the inception of a multi-planetary society
TRANSCRIPT
The Inception of a Multi-Planetary Society
Undergraduate Honors Thesis
Maximilian Y Plavcan
University of Florida
Fall 2019
2 Fall 2019
Faculty Advisors:
Dr. Anil Rao MAE
Dr. Steven Miller MAE
Dr. Oscar Crisalle ChE
3 Fall 2019
Abstract
With the technological advances currently being made to return humankind back to the Moon by
the year 2024 with NASA’s Artemis program, the goal of exploring and creating permanent
outposts on Mars has been postponed in the hopes that lessons are learned while colonizing Earth’s
nearest celestial body. In order to effectively colonize any celestial body outside Earth’s sphere of
influence, major challenges must be addressed to protect explorers from hazardous environments
and allow for sustainable living conditions. The report outlines a few of the key milestones that
must be accomplished in order to advance the human species to another planet and proposes
solutions to complex engineering challenges that the space agencies of the world could potentially
utilize when leaping into the vast expanses of space.
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Table of Contents
1 Introduction ........................................................................................................................................... 5
1.1 Reasoning for Human Exploration ............................................................................................... 5
2 Exploration Challenges ......................................................................................................................... 8
3 In-Situ Resource Utilization.................................................................................................................. 8
3.1 Regolith Utilization ....................................................................................................................... 8
3.2 Water Extraction and Utilization .................................................................................................. 9
4 Environment Overview ......................................................................................................................... 9
4.1 Martian Environment .................................................................................................................. 10
4.2 Potential Martian Habitation Sites .............................................................................................. 11
4.2.1 Habitation Site I - Planum Australe .................................................................................... 12
4.2.2 Habitation Site II - Pavonis Mons ....................................................................................... 14
4.2.3 Habitation Site III – Gale Crater ........................................................................................ 16
5 Oxyhydrogen Generation .................................................................................................................... 19
5.1 Chemistry Overview ................................................................................................................... 19
5.2 Engineering Prototype of Oxyhydrogen Generator .................................................................... 21
5.3 Experimental Setup and Prototype Results ................................................................................. 23
5.4 Prototype Improvements and Further Work ............................................................................... 24
5.5 Oxyhydrogen Generator Utilization ............................................................................................ 25
6 Orbital Dynamics ................................................................................................................................ 26
6.1 Characteristics of Simulated Orbit Transfers .............................................................................. 26
6.2 Approximations in Simulation .................................................................................................... 27
6.3 Orbit Fractioning ......................................................................................................................... 27
6.4 Transfer Orbit Simulation Results .............................................................................................. 28
6.4.1 Results Interpretation .......................................................................................................... 34
7 Additional Future Establishment- Sky Cities on Venus ..................................................................... 36
8 Afterthoughts ...................................................................................................................................... 38
9 Acknowledgments ............................................................................................................................... 39
10 Works Cited ......................................................................................................................................... 40
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1 Introduction Fifty years ago, Humanity committed itself to performing a great leap into the unknown by
successfully leaving Earth to set foot on another celestial object. From July 20th, 1969 to December
14th, 1972 twelve humans explored the face of the Moon, returning with Lunar samples effectively
giving humankind a glimpse into the formation of the Moon, Earth and Solar System. At the
conclusion of each mission many of the life support systems and other ground support equipment
that aided the astronauts heavily during their short visits were simply left behind, never to be used
again. With the successful return of Apollo 17 and its crew of three came the hopes of the Space
Shuttle Program as well as orbiting laboratories such as SkyLab and the International Space Station
(ISS). With the historic accomplishments that all successor programs achieved after the Apollo
program all had a single feature in common, each program confirmed human spaceflight again to
Low Earth Orbit (LEO) rather than look outward toward crewed interplanetary missions.
With upcoming human rated launch vehicles such as NASA’s Space Launch System (SLS) rocket
as well as SpaceX’s BFR and Blue Origin’s New Glenn rocket to name a few, the excitement of
the 1960’s space program is again a possibility for humankind to experience. This thesis is meant
to convey a broad overview of how humanity could potentially leave the confines of the Earth and
colonize, expand, and grow a civilization on the surface of Mars. Several celestial bodies within
the Solar system share features with Mars so the outcomes of the report do not exclusively apply
to a singular geological system. Additionally, the report is not all inclusive and does not address
all major challenges but rather outlines a select few. An artist representation of the SLS rocket that
will return humans back to the face of the Moon is displayed in Figure 1.1.
Figure 1.1 Artist Representation of the SLS Rocket During SRB Separation [1]
1.1 Reasoning for Human Exploration With the many hardships and struggles that humanity faces on Earth already it is a valid
question to ask why human exploration and expansion to other celestial bodies is necessary. With
space programs costing on the order of billions of dollars and with the constant risk of mid-flight
anomalies and unsuccessful missions, NASA and its contractors are constantly required to justify
mission purpose, priority and budget.
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Along with various others, there are three underlying reasons why humanity has an obligation to
strive towards becoming a multi-planetary society.
I. The first reason being the technological advancements that are a byproduct of the push to
expand humankind away from Earth. From the development of miniature electronics that
were initially driven by the need for mass reduction in spacecraft to advancements in
medical instrumentation that were driven by life support systems inside confined
spacecraft, the exploration of humankind to LEO and beyond creates constraints and
extenuating circumstances that would otherwise be nonexistent on Earth, thus facilitating
ingenuity and technological advancements in areas that would otherwise be unmodified
and be recognized as “good enough”.
II. The second reason is for the promotion of the longevity of the human species. With the
potential of nuclear warfare and fatal asteroid impacts, one option that could provide safety
to the existence of the human species is to occupy more than a single celestial object. In
the case of a global threat, human-induced or naturally occurring, humans will have the
ability to either escape or completely avoid global tragedies that are unavoidable.
III. The third and final reason is less tangible than the first two previous reasons but equally as
vital. Exploration from Earth inspires future generations as well as provides a means of
self-reflection for humans living on Earth. Within the short span of 13 years, starting in
1959 with NASA’s initial announcement of the Mercury 7 astronauts to 1972 when Apollo
17 and humans departed from the Moon, an entire generation of future explorers, and
dreamers were generated. As Apollo 11’s Lunar Module Pilot Edwin “Buzz” Aldrin said
“The biggest benefit of Apollo was the inspiration it gave to a growing generation to get
into science and aerospace” [2]. Heroes and legends were generated by these various space
missions, effectively providing subsequent generations with role models and liaisons to the
STEM field.
The act of self-reflection driven by leaving the Earth can best be illustrated by the aftermath
of the Earthrise image taken by Apollo 8’s Lunar Module Pilot Bill Anders in 1968. The
impact is best summarized through the words of astrophysicist Neil DeGrasse Tyson:
“In this image, which is one of the most recognizable images ever obtained, we see Earth as nature intended
it to be viewed: the ocean, land, clouds. There are no countries in that image. There are no national
boundaries or state borders. By 1970, the Environmental Protection Agency was founded under a Republican
president. Leaded gas was banned. The catalytic converter was introduced. The Comprehensive Clear Air
Act was passed. The Comprehensive Clean Water Act was passed. The Endangered Species Act was updated.
Earth Day was founded. Suddenly, we were thinking of Earth as a system; Earth as a collective home for all
of humanity. That happened while we were going to the Moon, and it was birthed by that photo. That photo
became part of our culture. We were different because of that photo.” [3]
The image of Earthrise is presented in Figure 1.2.
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Figure 1.2 Earthrise Taken by LMP Bill Anders in Lunar Orbit on Apollo 8 [3]
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2 Exploration Challenges
With the push to colonize Mars comes a collection of unique challenges that humanity has
never confronted at such scales. With the many challenges that must be accounted for, three critical
areas that are expanded upon within this report include Mars resource utilization, environmental
conditions and orbital mechanics of planetary arrival.
3 In-Situ Resource Utilization
With limited launch vehicle payload volume and high launch costs, materials and
instrumentation brought to initial interplanetary colonies must be minimal as well as self-
sustainable. Common habitation operations as basic as waste disposal must be calculated and must
focus on minimal resource waste to promote colony longevity. Due to launch constraints, In-Situ
resource utilization will play a key role in the success of future colonies on foreign bodies. In-Situ
Resource Utilization (ISRU) relates to the use and manipulating of local materials in order to
support mission exploration [32]. With the seemingly desolate environment that a planet such as
Mars may portray comes a multitude of hidden resources that can be uncovered through careful
planning and exact science. The two major resources that can be utilized on a planet such as Mars
are the surface regolith and water found within regolith and subsurface lakes/glaciers.
3.1 Regolith Utilization The first mentioned resource, and possibly the most abundant on Mars is the regolith present
on the surface and subsurface level of Mars’ environment. Martian regolith is rich in silica and
metallic oxides which would in turn provide a useful material in which to build infrastructure [18].
Utilizing granular body forming processes such as sintering through thermal treatments would
allow for the forming and hardening of the copious amount of soil found on the planet into useful
resources and infrastructure. One such use of Martian regolith is the sintering of the soil to provide
environmental shielding on habitations, effectively providing protective roofing used to help
hinder cosmic radiation exposure within habitation sites and protect against micrometeorite
impacts. Examples of such a habitation site can be found in Figure 3.1.
Figure 3.1 An Artist's Representation of a Possible Habitation Igloo on Mars. Note the habitat striations present due to
manufacturing [33]
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Through initial interplanetary colonization missions, either an autonomous system or astronaut can
build up the igloo-type habitation mounds simply through heat treatment processes applied to the
local soil in the habitation region. The build-up process would include overlaying soil onto a
habitation module and applying heat to sinter the overlaid granular material into a coherent layer
of material. Repeating this process of heating and building up layer-by-layer will mimic the
additive manufacturing techniques typically used with plastics on Earth.
3.2 Water Extraction and Utilization Water is a vital resource for any colony and will be the most valuable resource for human
exploration when leaving Earth. As a result of this necessity, the extraction and utilization of the
resource is of upmost priority in a mission. Within a system such as Mars, water is primarily
located in polar regions, subsurface cavities or dissolved within salts in the soil. The utilization of
water in the form of ice and liquid found in polar and subsurface regions on Mars is somewhat
straightforward and would require plumbing and filtration systems to extract and utilize the
resource. Due to the likelihood of colonization within Martian equatorial regions, the extraction of
water from soil will likely be the primary method of obtaining water from a planet like Mars. In
regions such as Gale Crater within the Martian equatorial region it has been proven through
spectral analysis by the Mars Science Laboratory (MSL) Curiosity that the soil contains 2% water
by weight [13]. Such a finding results in the ability to extract approximately 1 liter of water from
every 0.03 cubic meters of Martian soil [13]. Through thermal heating of the regolith, water vapor
will be synthesized and thus will be able to be stored and used for various purposes. Furthermore,
water extraction from soil can be coupled with the regolith utilization methods mentioned
previously. As regolith is heated in preparation for sintering of habitation construction, water vapor
can concurrently be extracted, providing two resources simultaneously.
As stated previously, the access to water is essential for the success of remote colonies on celestial
bodies. Not only is water essential for the biological sustainability of exploration crews but can
also be utilized in more non-traditional methods. The electrolysis of water into its elemental forms
of hydrogen and oxygen provides a means of utilizing water as a fuel and heat source. Hydrogen
and oxygen are a typical fuel-oxidizer combination used for propulsion systems on liquid rocket
engines. Thus, by separating water into its basic elements, fuel and oxidizer generation for rocket
propulsion systems on Mars will be possible. Along with uses as rocket fuel, electrolysis of water
can be used for habitations. Through the combustion of the hydrogen, heat produced by the
reaction can be used for environmental control systems within habitations. Additionally, the main
product of the combustion of hydrogen is water vapor so hydrogen combustion can also be used
as a tool to humidify greenhouses within habitation modules to promote plant and crop growth.
The electrolysis of water and its potential are expanded upon in section 5.
4 Environment Overview
The first consideration that must be determined when deciding to colonize the face of another
body in our Solar System is deciding on landing and habitation locations for the explorers arriving.
A compromise is required between the landing and habitation sites because spacecraft landing
locations typically require flat, desolate expanses that allow for unobstructed lander descent and
ascent while habitation locations can often be beneficial near craters and subsurface caves. This
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section explores three geological locations on the Martian surface and details the available
resources at each justifying the feasibility of habitation at each location.
4.1 Martian Environment Mars is the fourth planet from the Sun and the second smallest in size in the Solar System.
Mars orbits the Sun at an orbit with an eccentricity of 0.0934, resulting in a difference of aphelion
and perihelion of 0.285 AU [19]. One Martian sidereal year is the equivalent to 687 days on Earth
[19]. The difference between aphelion and perihelion contributes to the seasonal heating and
cooling of Mars as a result of the cyclic distance fluctuation from the Sun. The surface temperature
on Mars varies greatly by geological location and orbit location. The average temperature on Mars
is -60 ⁰C (-80 ⁰F). Near the equator, during a Martian summer the temperature can range from 20⁰C
(70⁰F) to -73⁰C (-100⁰F) while in polar regions during the winter can see temperatures as low as -
125⁰C (-195⁰F) [9]. Mars has an average surface gravity that is 38% of that experienced on Earth
with an average gravitational acceleration constant of 3.72 m/s2 [36].
The frigid temperatures experienced on the Martian surface are due partly to the atmospheric
conditions. The atmospheric density on the Martian surface is approximately 0.020 kg/m3 making
it approximately two orders of magnitude thinner than Earth’s atmosphere [20]. At the Martian
surface the average atmospheric pressure is approximately 0.00627 atm or 0.63% that of Earth’s
pressure at sea level. Even though Mars’ atmosphere is comprised up of 95% carbon dioxide (per
volume) the low density of the atmosphere does not allow the planet to retain the thermal
irradiation received from the Sun which results in a tundra-like environment.
Martian soil, or regolith is composed up of mainly silicon dioxide, iron oxide and various metal
alloys. Due to the thin atmosphere, much of the water found on Mars is in the form of frozen
glaciers that exist in subsurface layers under regolith. There have been discoveries of subsurface
liquid water currently present on Mars near the polar regions of the planet, but these discoveries
have been rare [7]. Along with water, traces of perchlorates have been discovered by various Mars
landers in weight percentages ranging from 0.5%-1% [22]. Perchlorates are significant due to their
potential as a source of fuel but pose a hazard to humans due to their toxicity to the human thyroid
gland system [23].
Mars lacks an interior dynamo that would otherwise generate a powerful protective magnetic field
to protect its surface from harmful radiation. The lack of convection of molten iron within Mars’
outer core is the primary theory of why Mars has a weak and almost non-existent magnetosphere
[25]. Mars is bombarded primarily with two types of radiation, low-energy protons from solar
flares and high-energy atomic nuclei known as Galactic Cosmic Rays (GCR) [24]. Solar flares are
low-energy, intermittent and can easily be shielded using conventional metals or organic polymers.
Conversely, GCRs are high energy nuclei that can damage DNA and can penetrate many
conventional radiation shields.
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4.2 Potential Martian Habitation Sites With the help of satellites such as NASA’s Mars Reconnaissance Orbiter and ESA’s Mars
Express Orbiter, topographic and detailed imagery of the Martian surface have been obtained and
made available to the public. Realistically, there are on the order of hundreds to thousands of sites
on Mars that have the potential to be suitable habitation zones but for all intense and purposes
three of the most promising and potentially scientifically rich locations were identified and
analyzed in this report. Along with geological landmarks and historical lander locations the
locations of the three potential “Habitation Sites” are marked in red on Figure 4.1.
Figure 4.1 Potential Martian Landing Sites [4] [6]
OLYMPUS MONS
NORTHERN LOWLANDS
SOUTHERN HIGHLANDS
HABITATION SITE II
HABITATION SITE I
HELLAS BASIN
ELYSIUM MONS
HABITATION SITE III
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4.2.1 Habitation Site I - Planum Australe (Coordinates: 81° S, 193° E)
Figure 4.2 Location of Subsurface Liquid Water Found at Planum Australe [8]. The subsurface liquid waterbed is shown as the
blue triangle in the image.
The first of the habitation sites is situated in the Southern Highlands of Mars near the
Southern Pole. The area of interest within Planum Australe is roughly 12 miles in width. The
region gained interest in 2018 when Italian physicists announced evidence of subsurface liquid
water in the region found using radar data produced by MARSIS, a low-frequency radar instrument
flown on the European Space Agency’s Mars Express orbiter mission [7]. The 12-mile wide patch
of Martian land is a flat plain with few topographical variations, making descent and ascent to and
from the location ideal. Due to the minimal topographical features, the location provides little
naturally occurring shelter and protection from micrometeorites and radiation. Due to the
subsurface lake location near a polar region, sunlight is limited to the area during a portion of the
Martian sidereal year. Partly as a result of the limited sunlight, temperatures in the polar region
can plummet to -195⁰F (-125⁰C) making living conditions harsh and frigid [9]. Due to the limited
sunlight in the region, alternatives to solar energy must be provided if habitation is considered.
Energy alternatives in the region could include thermonuclear or geothermal. One way to provide
shelter and insulation for habitats within the region is to burrow into the Martian regolith,
effectively creating subsurface habitats. A proposed habitation layout is presented in Figure 4.3.
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Figure 4.3 Habitation Site I With Habitation Details Outlined [6]
Situating the liquid waterbed in between the ascent/descent region and habituation area would
allow astronauts access to ample pre-liquified water for applications such as biological
consumption, fuel for energy utilization and launch vehicle fuel and oxidizer. The ascent/descent
region is an ellipse that is situated in an orientation that aligns with the orbital mechanics analysis
performed in a subsequent section. In order to arrive at the habitation site from cis-Martian space,
a terminal polar orbit would be required with an orbital inclination aligned with the latitude that
passes through the habituation site. To provide landing tolerance, the ascent/ descent region is an
ellipse of approximately 25 miles in major axis.
Habitation Site
Perimeter
Living Region
Ascent/ Descent
Region
Liquid Water
Source
50 miles
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4.2.2 Habitation Site II - Pavonis Mons (Coordinates: 4.70°N, 247°E)
Figure 4.4 Artist Representation of Pavonis Mons [10]. Habitation Zone II is Highlighted in Red.
The second habitation site is located in the Tharsis Montes region near the Martian equator
within Pavonis Mons. Pavonis Mons is one of three inactive volcanic mountains in the Tharsis
Montes region. The habitation zone selected is situated directly above a region of subsurface
glaciers within Pavonis Mons. The region was once home to volcanic activity so subsurface lava
tubes are inevitable. With pre-existing caves and lava tubes, astronauts can use the natural
phenomenon as protection from micrometeorite collisions and cosmic radiation. The location is
situated near Mars’ equator so sunlight is available to the region throughout the entire Martian
sidereal year. The region experiences a warmer climate when compared to polar regions with a
temperature upper and lower bound of 20⁰C to -73⁰C [9]. Due to the constant sunlight, solar energy
could be the primary source of energy production in the region. Due to the seasonal dust storms
that block sunlight exposure on Mars, secondary energy sources such as radioisotope
thermoelectric generators (RTG) should also be considered. The water glaciers that exist within
the volcano would provide astronauts with consumable water, a fuel source and rocket fuel and
oxidizer. The habitation zone’s location near the Martian equator is beneficial because it will allow
spacecraft rendezvous to Low Mars Orbit to use less fuel due to the effective “delta V” provided
by the larger rotational speeds achieved at the equator. The proposed habitation location within
Pavonis Mons along with landing zone is presented in Figure 4.5.
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Figure 4.5 Habitation Site II on Pavonis Mons [11] [6].
Figure 4.5 depicts the proposed habitation site at Pavonis Mons. Both the living and the
ascent/descent regions are situated directly above the subsurface glacier, allowing both regions
direct access to frozen water. The ascent/ descent elliptic region is situated in a way that is aligned
with the orbital mechanics analysis preformed in a subsequent section. When arriving to the
habitation site a craft would be in an orbit with minimal inclination, so having a landing site aligned
with the velocity vector direction of the craft would allow landing location tolerancing. The
location of the subsurface glacier found within Pavonis Mons is shown in the top right region of
Figure 4.6.
Figure 4.6 Elevation Map of Pavonis Mons and Arsia Mons Along with Predicted Glacier Sites [17]
30 Miles
Ascent/Descent
Region
Mountain
Perimeter
Living Region
Habitation Site
Perimeter
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4.2.3 Habitation Site III – Gale Crater (Coordinates: 4.58°S, 137.44°E)
Figure 4.7 Gale Crater with Proposed Habitation Site Identified in Red [15].
The third habitation site is Gale Crater. The habitation region highlighted in Figure 4.7 is
located within an region of flat, semi-uniform land within Gale Crater. The flatness of the region
is advantageous and would allow for habitation and launch locations to be in the vicinity of one
another. The crater is best known as the location of the 2012 landing of the Mars Science
Laboratory (MSL) Curiosity rover. The crater is located near Mars’ equator and is approximately
96 miles in diameter and encircles the 3.4-mile-high Aeolis Mons [12]. Due to the crater’s location,
it will experience temperature fluctuations like those of Habitation Site II. The primary sources of
energy would likely be solar due to the areas ample sun exposure year-round but would require
contingency energy production methods such as RTGs or geothermal utilization. The location does
not have an abundance of subsurface caves and lava tubes so protection and shelter from natural
elements would likely require human manipulation of the region. Gale Crater is of interest due to
its soil surface composition which was confirmed in 2013 to contain 2% water by weight [14]. As
a result of the soil composition it would be feasible to extract approximately 1 liter of water from
every 0.03 cubic meters of Martian soil [13]. The soil analysis performed by the Sample Analysis
at Mars (SAM) instrument on the MSL is presented in Figure 4.8. From the analysis, the four most
prevalent chemical components (by an order of magnitude of 2) were water, carbon dioxide,
oxygen and sulfur dioxide, with water being the most abundant of the four. The highest counts per
second for water was obtained when each sample was heated to a temperature of approximately
250 degrees Celsius (Figure 4.8).
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Figure 4.8 Soil Analysis Conducted by SAM Within the MSL Curiosity Rover [14]
The proposed habitation site layout is presented in Figure 4.9. The habitation region is in the same
area in which the water observed by the Curiosity rover was found, giving future habitants access
to water through a heating process similar to that performed by SAM. The ascent/ descent elliptic
region is situated in a way that the semi major axis is parallel to Mars’ lines of latitude. When
arriving to the habitation site a craft would be in an orbit with minimal inclination so having a
landing site aligned with the velocity vector direction of the craft would allow landing tolerances
as previously described in habitation site II.
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Figure 4.9 Gale Crater Habitation Site III [16]
Habitation Site
Perimeter
Ascent/Descent
Region
Living Region
15 Miles
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5 Oxyhydrogen Generation
With the need for energy production on Mars, one form can be found within the subsurface
lakebeds and permafrost entrenched in the Martian regolith. The reminisces of water on Mars has
become a known fact within the scientific community, which in turn has created a discussion on
its potential utilization by future explorers to the planet. As stated in previous sections, water has
the potential to be utilized not only as a biological consumable but also as a source of energy. For
example, cryogenic hydrogen is often used as a fuel for liquid rocket engines while standard
gaseous hydrogen can be used as a heat source for astronaut living quarters and green houses.
Furthermore, if hydrogen is used for biological sustainability purposes, when hydrogen undergoes
a combustion reaction, the main byproduct of the reaction is liquid water which then has the
potential to either be recycled within a system or be used as a biological consumable.
Water is composed up of hydrogen and oxygen molecules, two elements that prove highly useful
in human spaceflight and sustainability. In order to utilize both elements, the electrolysis of water
can be utilized to split the water molecules into their respective elemental states. To split water
molecules within an electrolytic cell, an electrical current can be run through electrolyzed liquid
water and as a result hydrogen gas will be produced at the cathode and oxygen gas at the anode.
An electrolyte is mixed within the water to promote water conductivity and thus the flow of
electricity through the system.
Figure 5.1 Example of Electrolysis Process of Hydrogen and Oxygen Separation from Water [28]
5.1 Chemistry Overview The electrolysis of water as described within the report occurs within an electrolytic cell. An
electrolytic cell utilizes electrical current in order to drive a nonspontaneous reduction-oxidation
(redox) reaction, as opposed to a galvanic cell which generates energy through a spontaneous redox
reaction [34]. The ideal half reactions that occur within the electrolytic cell for the electrolysis of
water are presented within equations 1 and 2.
Equation 1 represents the half reaction that occurs at the anode of the electrolytic cell. Water within
the cell is stripped of electrons due to the electric potential difference driven by the application of
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an external power source. The positive terminal of the power source is connected directly with the
anode, allowing for the transfer of electrons from the anode. The process of electron stripping is
known as oxidation. As water molecules oxidize, they produce oxygen gas and hydrogen cations.
2𝐻2𝑂(𝑙) → 𝑂2(𝑔) + 4𝐻+(𝑎𝑞) + 4𝑒− (1)
As oxidation occurs, electrons transfer from the anode to the opposite end of the cell at a location
known as the cathode. The cathode is opposite to the anode and receives electrons driven from the
anode by the power supply. The cathode is the site where the cell receives electrons or where
reduction occurs. As hydrogen cations combine with electrons, hydrogen gas is produced as shown
in equation 2.
4𝐻+(𝑎𝑞) + 4𝑒− → 2𝐻2(𝑔) (2)
Combining the two half reactions produces the overall chemical reaction accounting for both
reduction and oxidation. The overall equation is presented in equation 3.
2𝐻2𝑂(𝑙) → 2𝐻2(𝑔) + 𝑂2(𝑔) (3)
The cell potential of the electrolytic cell is -1.23 Volts, which represents that the cell utilizes a
non-spontaneous chemical process, requiring applied potential. The cell potential is an idealization
and does not account for losses such as contact resistance and undesired side reaction so an
overpotential was required to drive the reaction within the experimental setup.
The selection of the electrolyte used within the cell is of importance due to the various competing
side reactions that occur as a result of the driven chemical process. With the use of sodium chloride
as an electrolyte within distilled water, the danger of producing chlorine gas was identified and
thus the salt should not be considered if the generator is located within a confined space or within
a “manned” area. More suitable electrolytes such as sodium hydroxide are often used due to their
ability to conduct well as well as produce relatively benign byproducts if side reactions do occur.
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5.2 Engineering Prototype of Oxyhydrogen Generator To aid with the previous discussion of the potential that hydrogen production has on the
development and sustainability of a colony located on a foreign body, an oxyhydrogen generator
was designed built and manufactured to demonstrate a proof of concept of the mentioned chemical
process. Solidworks Computer Aided Design software was utilized to create a 3D model of the cell
to aid in manufacturing and clearance verifications. A side-by-side comparison of the CAD model
to the actual manufactured cell is presented within Figure 5.2.
Figure 5.2 Side-by-side comparison of the oxyhydrogen generator CAD model to the actual engineering proof of concept.
The oxyhydrogen generator is composed up of three major subcomponents: the main reservoir, the
anode & cathode plate arrays and the bubbler. An image detailing the physical representation of
each subassembly is presented within Figure 5.3.
Figure 5.3 Overview of the subcomponents of the oxyhydrogen generator built for the report
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The oxyhydrogen reservoir is the location in which distilled water and electrolyte were stored
during testing. Ionized water could have also been utilized for testing, but distilled water was used
to hinder undesired side reactions as well as reduce corrosion buildup on anode and cathode plate
arrays. Sodium hydroxide was utilized as the cell electrolyte due to its desirable conductivity
properties within water as well as its tendency to not produce toxic gases when oxidized.
The anode and cathode arrays were composed up of alloy aluminum flashing used for housing roof
applications. When aluminum is exposed to a solution of sodium hydroxide, hydrogen gas and
aqueous sodium aluminate forms causing metal dissolving. Due to this undesired phenomenon,
low molarity solutions of sodium hydroxide were utilized during testing to reduce plate corrosion.
Stainless steel washers, nuts and bolts were utilized to constrain both the anode and cathode plate
arrays. During testing the bolts housing each plate array were the regions in which the power
source was interfaced directly with. As mentioned previously, the cathode is the region in which
reduction occurs and hydrogen forms while the anode is the region where oxidation occurs and
oxygen forms.
The third subassembly within the oxyhydrogen generator is the bubbler assembly. It was
anticipated prior to manufacturing that match tests would be performed. A match test consists of
holding a match to the outlet hose of the cell in order to verify hydrogen production through
combustion. The bubbler was installed into the cell as a safety measure, to hinder the phenomenon
of “flashback” during testing. Flashback is the propagation of a combustion reaction in a reverse
direction as intended, effectively causing a flame to creep into the main reservoir of a fuel cell. Of
course, this phenomenon is highly undesirable and dangerous so adding a bubbler adds an
additional inert barrier between the ignition source and the main reservoir such that if flashback
occurred it would only occur in a small volume in comparison to the main reservoir.
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5.3 Experimental Setup and Prototype Results Experimental performance testing of the manufactured engineering prototype was
completed in order to characterize and quantify the capabilities of the electrolytic cell. Distilled
water mixed with sodium hydroxide to produce a low molarity solution was poured into the main
reservoir of the oxyhydrogen generator in preparation of testing. Additionally, untreated tap water
was poured into the bubbler since no chemical processes occur within its reservoir. Utilizing an
Eventek KPS3010D Variable Switching Regulated Digital Power Supply, alligator clip leads were
attached directly to the anode and cathode of the electrolytic cell, with the positive terminal
interfacing with the anode plate array and the negative terminal interfacing with the cathode plate
array. A depiction of the experimental setup is presented within Figure 5.4.
Figure 5.4 Depiction of the experiential setup used to characterize the engineering prototype performance.
While operating the power supply at approximately 3.8 Volts and 9.6 Amps, experimental tests
were performed for 3-minute intervals. The short interval duration was chosen due to the formation
of undesired side reactions as a result of prolonged plate oxidation. Due to the limitations of the
experimental setup hydrogen production was quantified through visual inspection of the bubble
formation rate of the cell. As the cell was operated, approximations of bubble formation average
size as well as rate at which bubbles formed within the bubbler were documented and extrapolated
for longer time periods. It was calculated that the engineering prototype had the ability to produce
approximate 1.45 L/hr of hydrogen and oxygen when supplied with the aforementioned power
from a DC power supply. A depiction of hydrogen and oxygen formation within the cell during
testing is presented within Figure 5.5.
24 Fall 2019
Figure 5.5 Depiction of hydrogen and oxygen bubble production within the oxyhydrogen generator
As mentioned previously, a match test was performed to verify the formation of hydrogen and
oxygen within the oxyhydrogen generator. The test was performed in a well-ventilated
environment to mitigate the buildup of explosive gases. Images of the match test are presented
within Figure 5.6
Figure 5.6 Images of a match test performed during testing to verify hydrogen and oxygen production within the electrolytic cell
5.4 Prototype Improvements and Further Work Due to the fast-paced design, manufacturing and testing phases performed for the
oxyhydrogen generator, several areas of improvement can be performed to advance further
versions of the hydrogen generator. During testing it was observed that local regions of electrolysis
formed as a result of the overlapping anode and cathode plate arrays. Localized electrolysis greatly
hindered the bubble production of the hydrogen and oxygen because only a fraction of each plate
area was utilized as a result (see Figure 5.5). Additionally, alternative plate materials should be
utilized in further iterations of the design to allow for higher molarity solutions of sodium
hydroxide to be utilized. Materials such as stainless steel and platinum could be considered within
25 Fall 2019
this material selection process. The number of contacts within each plate array should also be
minimized in further iterations to lower losses associated with contact resistance between surfaces.
It was also observed that bubble trapping occurred due to the orientation of the cell, future
iterations should orient the arrays of the cathode and anode to mitigate such phenomenon.
5.5 Oxyhydrogen Generator Utilization The potential uses of a hydrogen-oxygen generator were discussed briefly in previous
sections and included uses such as: fuel production for spacecraft, a biological consumable for
explorers and fuel for habitations. A key concept that is required in order to promote sustainable
living on another celestial body is the ability of a species to produce food for biological
consumption. A hydrogen-oxygen generator has the ability to be utilized as a humidifier used to
promote the growth of planet life grown on Mars. An overview of one method in which explores
could efficiently farm on another celestial body is presented within Figure 5.7.
Figure 5.7 Concept of space farming utilizing an oxyhydrogen generator as a central humidifier and heat source.
As hydrogen and oxygen are produced by a generator, the produced gas can be combusted to
produce water vapor as well as heat, due to the exothermic nature of the reaction. Situating the
humidifying hydrogen generator within the center of a farming unit could allow humidification as
well as warming of the surrounding environment, effectively promoting plant growth. To “close
the system” of the farming technique a polymer lining can be applied to the walls of the farming
unit to allow for water vapor condensation to form. With condensation forming, water can be
recycled by forcing the condensed water to settle within a water collection reservoir underneath
the system. The water in the reservoir can then be recirculated into the hydrogen generator to be
separated and combusted again.
26 Fall 2019
6 Orbital Dynamics
In section 4.2 of the report three potential habitation sites on Mars were proposed: Planum
Australe, Pavonis Mons and Gale Crater. The first mentioned is situated in the southern region of
Mars in the vicinity of the South pole while the second two are situated within 5 degrees north and
south of the Martian equator. To further investigate the feasibility of arriving to each habitation
site, on-orbit dynamics scenarios were simulated using MATLAB computer software. The purpose
of the simulation was to generate estimates of required spacecraft impulse maneuvers that would
be performed to transfer a vehicle from an inclined large circular orbit to a smaller circular orbit
of different inclination and longitude of ascending node. The final orbital inclination of each
simulation is directly dependent on habitation site location.
For the orbit transfers within the simulations, two-impulse Hohmann transfers of non-coplanar
circular orbits were performed. For simplification, within the simulation all orbit circularizations
were performed at the periapsis of each elliptic transfer orbits while all plane changes were
performed at the apoapsis of each transfer orbit.
Figure 6.1 Two-impulse Hohmann transfer of two non-coplanar circular orbits, transferring from a small circular orbit to a larger
circular orbit [37]
6.1 Characteristics of Simulated Orbit Transfers The initial orbit for all scenarios simulated a spacecraft within a circular orbit (e =0), 1000
kilometers from the surface of Mars with an orbital inclination of 25.19⁰ and longitude of
ascending node of 0⁰. The initial orbit inclination was chosen because Mars has an orbital tilt of
approximately 25.19⁰ [20] so any spacecraft arriving to Mars from a transfer orbit within the
ecliptic plane would appear to have an inclination equal to the planetary tilt when viewed within a
27 Fall 2019
Mars Centered Mars Fixed coordinate system (MCMF). The initial and final longitudes of
ascending nodes were 0⁰ and 90⁰. The values of the initial and final longitude of ascending nodes
were chosen arbitrarily and kept constant for all scenarios. The longitude of ascending node was
varied from initial to final orbit to simulate the variation in impulse maneuver locations that could
occur within a “real-life” orbit transfer scenario.
The final orbits in each simulation have altitudes of 230 kilometers, which was chosen due to the
altitude being the theoretical beginning of the Martian exosphere [36]. It was assumed that landing
to all three locations would endure similar reentry/descent regimes once in a low orbit, 230
kilometers about their targets so energy required for orbital transfer to each final orbit was only
considered when comparing habitation sites.
6.2 Approximations in Simulation As stated previously, the simulation performed in MATLAB approximated the impulses
required to perform an orbital transfer from an initial circular orbit with altitude of 1000 km ,
inclination of 25.19⁰ and longitude of ascending node of 0⁰ to three different orbits that correlated
with the three previously mentioned proposed habitation sites. In order to simplify calculations for
the simulations performed, various approximations were implemented. The largest simplification
made was the modeling of on-orbit maneuvers as scaled Dirac delta functions, or better known as
impulsive thrust approximation [37]. The approximation assumes that that an infinite thrust force
is applied instantaneously due to the thrust’s magnitude being extremely large in comparison to its
application duration. In reality, burn durations associated with on-orbit plane changes and
circularization maneuvers would likely not be negligible in comparison to the thrust produced by
vacuum optimized engines so the approximation was performed purely for simplicity. The
simulation also assumed uniform gravity distribution within Cis-Martian space.
6.3 Orbit Fractioning Within the simulation, a method of orbit fractioning was employed. Orbit fractioning is a
method of splitting up an orbit transfer into a series of thrust maneuvers that would otherwise be
performed as singular events. For example, in the case of a two-impulse Hohmann transfer
simulated within the report, orbit fractioning would allow for N number of apoapsis-periapsis on-
orbit maneuvers effectively allowing for splitting of large orbit circularization and plane change
burns into smaller achievable maneuvers. The mathematical representation of orbit fractioning is
represented within equation (4).
[
𝑟𝑛
𝛺𝑛
𝑖𝑛
] = [
𝑟0
𝛺0
𝑖0
] +𝑛
𝑁[
𝑟𝑓 − 𝑟0
𝛺𝑓 − 𝛺0
𝑖𝑓 − 𝑖0
] , (𝑛 = 1,2,3 … 𝑁) [38] (4)
Where rn is the incremental radius of each transfer orbit, Ωn is the incremental longitude of
ascending node and in is the incremental inclination of each transfer orbit.
28 Fall 2019
6.4 Transfer Orbit Simulation Results As stated previously, MATLAB simulations were performed for all three habitation sites.
Each simulation produced plots of incremental “delta V” for impulse maneuvers performed at the
transfer orbit apoapsis and periapsis as well total “delta V” and total time required.
Planum Australe
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Apoapsis
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Periapsis
Total Orbit Fraction Number (N) vs Total Delta V Required
Total Orbit Fraction Number (N) vs Total Transfer Time
Required
Table 1 Planum Austale simulation results
29 Fall 2019
The instance in which the total orbit fraction number was equal to four was analyzed to provide
additional orbit transfer analysis. For N=4, the total impulse required to transfer from the ecliptic
plane to Planum Australe was found to be 5.1 km/s. The 3D simulation results are presented in
Table 2.
Table 2 Planum Austale 3D simulation results. The top image depicts an isometric view of the entire orbit transfer, where the light
blue orbit represents the initial orbit and the orange orbit, with approximately 90 degrees of inclination, represents the final orbit.
The bottom image highlights the final orbit’s placement over Habitation Site I, Planum Australe.
30 Fall 2019
Pavonis Mons
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Apoapsis
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Periapsis
Total Orbit Fraction Number (N) vs Total Delta V Required
Total Orbit Fraction Number (N) vs Total Transfer Time
Required
Table 3 Pavonis Mons simulation results
31 Fall 2019
The instance in which the total orbit fraction number was equal to four was analyzed to provide
additional orbit transfer analysis. For N=4, the total impulse required to transfer from the ecliptic
plane to Pavonis Mons was found to be 1.9 km/s. The 3D simulation results are presented in Table
4.
Table 4 Pavonis Mons 3D simulation results. The top image depicts an isometric view of the entire orbit transfer, where the light
blue orbit represents the initial orbit and the orange orbit represents the final orbit. The bottom image highlights the final orbit’s
placement over Habitation Site II, Pavonis Mons.
32 Fall 2019
Gale Crater
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Apoapsis
Maneuver Number (n) vs Impulse Maneuvers Performed at
Transfer Orbit Periapsis
Total Orbit Fraction Number (N) vs Total Delta V Required
Total Orbit Fraction Number (N) vs Total Transfer Time
Required
Table 5 Gale Crater simulation results
33 Fall 2019
The instance in which the total orbit fraction number was equal to four was analyzed to provide
additional orbit transfer analysis. For N=4, the total impulse required to transfer from the ecliptic
plane to Gale Crater was found to be 2.1 km/s. The 3D simulation results are presented in Table
6.
Table 6 Gale Crater 3D simulation results. The top image depicts an isometric view of the entire orbit transfer, where the light blue
orbit represents the initial orbit and the orange orbit represents the final orbit. The bottom image highlights the final orbit’s
placement over Habitation Site III, Gale Crater.
34 Fall 2019
6.4.1 Results Interpretation Presented in the results section above are various key outcomes that were obtained for each
habitation site using the orbit transfer simulation within the report. The results show that the total energy
required when transferring to each location was directly related to the magnitude of cranking angle required
to perform each orbit transfer. As a result of this relation, it was found that performing an orbit transfer to
Planum Austale, located within the Mars southern pole, required the largest amount of energy (delta V) of
the three locations and exhibited asymptotic behavior approaching 5.2 km/s when factoring number was
incrementally increased. This key finding intuitively makes sense since transferring to a polar orbit from
the plane of the ecliptic would require more than 50⁰ of cranking angle, while the other two equatorial
locations would require cranking angles of approximately 20⁰-30⁰. The habitation site that required the least
total energy to arrive to from the plane of the ecliptic was Pavonis Mons with asymptotic behavior with
incremental fractioning increase towards 1.95 km/s. Gale Crater required slightly more total energy with
asymptotic behavior towards 2.2 km/s. It is also valuable to note that the plane change impulse maneuvers
performed at the apoapsis of each transfer orbit were all an order of magnitude larger than their transfer
orbit periapsis impulse maneuver pair. This phenomenon is largely due to the direction of impulse
application and extent of the maneuver. The impulse maneuver performed at the apoapsis of each elliptic
transfer orbit provided an orbital plane change and also produced an elliptic transfer orbit from an initially
circular orbit while the periapsis maneuvers simply circularized each orbit. Due to the nature of the
simulation performed, all habitation site transfers followed similar linear time requirements with increased
total transfers. This phenomenon can be explained due to each simulation trajectory following similar
overall trajectories but differing in orientation.
When analyzing the three habitation sites, an apoapsis impulse reduction phenomenon was observed when
cranking to habitation sites of low overall required cranking angle (e.g. Pavonis Mons & Gale Crater). A
depiction of the phenomenon is presented within Table 7.
Table 7 Visualization of apoapsis energy reduction phenomenon observed for low inclination change orbit transfers. if represents
the angle of inclination of the terminal orbit with respect to the initial inclination of 25.19°. For example, if represents an inclination
of 19.19° within MCMF. Longitude of ascending node was held constant for each simulation.
35 Fall 2019
Specifically within Table 7 it can be observed that at low overall cranking angles that the required impulses
with increasing fractioning number actually decreases. The phenomenon is counter-intuitive because one
would imagine increased required impulses with subsequent fractioning due to increased orbital speeds
reached within incrementally lower orbits. The apoapsis impulse reduction phenomenon reaches a critical
inflection point at approximately 20° of overall cranking angle where the reduction behavior diminishes,
and the impulses required at the transfer orbit apoapsides increase with increasing fraction increment as
expected. The reduction behavior for low overall cranking angles can be attributed to the geometry of the
impulsive plane changes applied at each elliptic transfer orbit apoapsis. For each plane change maneuver,
a law of cosines relation was applied to obtain the magnitude of the required plane change as presented
within equation (2).
‖∆𝑣‖ = √(𝑣−)2 + (𝑣+)2 − 2𝑣−𝑣+ cos(𝜃) (2)
Where Δv is the required delta V for the burn, v- is the orbital speed before the impulse and v+ is the orbital
speed after the burn and θ is the cranking angle. It can be observed that for transfer orbit maneuvers with
generally low overall cranking angles, that fractioning reduces the crank angle per maneuver even further
such that the small angle approximation can be utilized. Specifically, for a very small angle the
trigonometric function approaches 1 so the first two terms will be reduced increasing amounts as the v+ and
v- terms increase with fractioning. Conversely with large cranking angles the trigonometric term will be
fractioned causing the first two terms to be subtracted by a relatively small number in comparison, thus
causing increased impulse with increased orbit fractioning number. For completeness, equation (3) was
provided to show the implementation of the Vis-Viva equations implemented into the law of cosines
expression within equation (2).
‖∆𝑣‖ = √(√𝜇
𝑟)
2
+ (√2𝜇
𝑟−
𝜇
𝑎)
2
− 2 (√𝜇
𝑟) (√
2𝜇
𝑟−
𝜇
𝑎) cos(𝜃) (3)
Where μ is a gravitational parameter of a planet, r is the location of a spacecraft within an orbit and a is
the semi-major axis of an elliptic transfer orbit.
36 Fall 2019
7 Additional Future Establishment - Sky Cities on Venus As stated in previous sections, the report is not unique to a single celestial body. Many geological
locations within the Solar System share commonalities and thus the approaches to in-situ resource
utilization, human factors and orbital dynamics can be translated to fit differing exploration missions. There
are a few instances of “unique cases” in which the approaches described in the report do not apply and non-
traditional modes of colonization must be applied. One such scenario is the case of colonizing Venus. With
Venus’ surface pressure 96 times that of Earth’ the development of alternative habitations are required.
The planet Venus has an orbit that situates it approximately 40% closer (at closest approach) than the orbit
of Mars, making it the closest planet to Earth in the solar system. With its “close” proximity with Earth one
may wonder why space agencies haven’t announced major plans of Venus colonization. It is not until one
examines the geological environment of Venus that this colonization hesitancy can be realized. Underneath
the seemingly benign façade of Venus’ outer surface lies a hostile wasteland. The surface temperature of
Venus ranges from 461 ⁰C (861 ⁰F) to 701 ⁰C (1293 ⁰F) with an atmospheric pressure of 96 Bar (1300 PSI)
along with an atmosphere composed primarily of carbon dioxide, nitrogen and sulfuric acid [29].
Conversely, if one were to examine the thermodynamic properties of the atmosphere simply 50 kilometers
above the harsh surface, Earth-like conditions are present. This has driven scientists and engineers to
propose potential colonies capable of floating high within Venus’ upper atmosphere, quite literally creating
floating sky cities.
At an attitude of 50 kilometers Venus’ environment mimics that of Earth with 90% of Earth’s gravity and
a temperature range of 0⁰C (32⁰F) to 50⁰C (122⁰F) providing abundant to near constant exposure to solar
energy for energy production. Furthermore, due to the thick Venusian atmosphere “breathing air” of the
nitrogen-oxygen ratio of 80:20 can serve as a lifting gas (0.5 kg/m3) , effectively allowing the full interior
volume of an aerostat, as shown in Figure 7.1, to be utilized as living quarters.
Figure 7.1 Artist Concept of Venus Sky Cities [30]
With the endless possibilities that habitations within the Venusian atmosphere appear to bring come major
challenges that require ingenuity and approaching problems never before seen on Earth. Some of the
37 Fall 2019
challenges that humanity will be faced to address within these type of habitats include examples such as:
the development of lightweight structures for self-sustaining city sized colonies to be structurally sound
within confined thin walled balloons, the ability to resupply the floating habitats with resources, cosmic
ray/micrometeorite shielding of the habitat walls, methods of sulfuric acid contamination prevention within
the habitation and development of contingency evacuation options in the occurrence of worst case
scenarios.
38 Fall 2019
8 Afterthoughts With the excitement of interplanetary travel and the prospect of creating utopia-like
civilizations on other celestial bodies comes a key responsibility by the Earth-based humans
committing themselves to this outward expansion. Colonizing additional celestial bodies in the
Solar system is certainly exciting and vital to the human species but should not be taken as an
excuse to neglect the planet that all of humanity currently resides on. With the extensive research
I completed within the Fall 2019 semester came a realization of how challenging and unforgiving
the process of colonizing another celestial body will be when performed. The Earth is a fragile
system that has the potential to reach a similar demise achieved by planets such as Mars and Venus
if further neglect to the planet is applied. It is in my hopes that with an endeavor to return to the
Moon or exploration to Mars that humanity experiences a unanimous clarity of the magnitude of
our existence similar to the aftermath of Earthrise that sparks increased care and appreciation of
the pale blue dot that our species is currently confined on.
Figure 8.1 Pale Blue Dot image taken of Earth by Voyager 1 on February 14th 1990 from a distance of more than 6 billion kilometers [39].
39 Fall 2019
9 Acknowledgments I would like to thank all three of my faculty advisors for the incredible support that they have
given me throughout the honors thesis process. An abstract and ambitious topic of formulating a
paper that underlines the key requirements of colonizing another celestial body made it difficult to
find interested advisors, so the willingness and knowledge provided to me by all three of them was
greatly appreciated.
40 Fall 2019
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