Dragonfly: Thermal Design Overview
Transcript of Dragonfly: Thermal Design Overview
ICES-2020-160
Copyright © 2020 Johns Hopkins Applied Physics Laboratory and Lockheed Martin Space Systems Company
Dragonfly: Thermal Design Overview
G. Allan Holtzman1, Robert F. Coker2, Carl J. Ercol3 and Douglas S. Adams4
Johns Hopkins Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723
and
Loren C. Zumwalt5
Lockheed Martin Space Systems Company, 12257 S Wadsworth Blvd, Littleton, Colorado 80125
Dragonfly is a NASA New Frontiers mission that will send a rotorcraft lander to Titan,
Saturn’s largest moon. Titan has a dense atmosphere and low gravity, making flight an ideal
way to traverse its surface. Powered flight will be achieved by employing a battery charged
by a Multi-Mission Radioisotope Thermoelectric Generator (MMRTG). The temperature of
Titan at its surface is nearly constant but extremely cold at 94 K, so the lander’s thermal
control system (TCS) will retain the excess heat from the MMRTG and distribute it
throughout the lander body with a pumped fluid loop. During cruise to Titan, a cruise stage
with a second pumped fluid loop will maintain spacecraft components and the MMRTG
within allowable flight temperatures. The performance of the lander TCS as well as all
components exposed to the Titan environment will be verified with testing on Earth in a
Titan-relevant environment. This paper will provide an overview of the lander and cruise
stage still-evolving thermal design details with a discussion of the planned thermal testing
campaign.
Nomenclature
APL = Johns Hopkins Applied Physics Laboratory
AU = Astronomical Unit
CCHP = Constant Conductance Heat Pipe
CFC-11 = ChloroFluoroCarbon fluid, also known as freon-11
EDL = Entry Descent and Landing
EOM = End Of Mission
HGA = High Gain Antenna
I&T = Integration and Test
IMU = Intertial Measurement Unit
LIDAR = Laser Imaging, Detection, And Ranging
LM = Lockheed Martin Space Systems Company
MMRTG = Multi-Mission Radioisotope Thermoelectric Generator
MSL = Mars Science Laboratory
N2H4 = Hydrazine
PSU = Power Switching Unit or Penn State University
RCS = Reaction Control System
RF = Radio Frequency
TCM = Trajectory Correction Maneuver
TCS = Thermal Control System
TEL = Thermal Exterior Losses document
TVAC = Thermal VACuum
TWTA = Traveling Wave Tube Amplifier
1 Dragonfly Lead Thermal Engineer, Johns Hopkins Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723. 2 Dragonfly Instrument and Analysis Thermal Lead, Johns Hopkins Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723. 3 Dragonfly Lander Fluid Loop Thermal Lead, Johns Hopkins Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723. 4 Dragonfly Spacecraft System Engineer, The Johns Hopkins University Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723. 5 Dragonfly Cruise Thermal Lead, Lockheed Martin Space Systems Company, 12257 S Wadsworth Blvd, Littleton, Colorado 80125.
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I. Introduction
On Titan, the molecules that have been raining down like manna from heaven for the last 4 billion years might
still be there largely unaltered, deep-frozen, awaiting the chemists from Earth.
— Carl Sagan, Pale Blue Dot
Dragonfly will allow our Earth chemists to explore this organically rich, ocean world at multiple locations on
Titan’s surface by flying through its thick atmosphere (surface pressure = 1.5 bar), aided by the relatively low Titan
gravity (g = 1.35 m/s²). The Titan environment is extremely cold at 94 K (-179°C), and although the lander’s
thermal control system must take these harsh conditions into account, they are known and constant, changing very
little over diurnal or even seasonal cycles. A single MMRTG supplies not only the heat needed to survive the Titan
and cruise environments, but also all the electrical power for the lander and spacecraft throughout the mission
including spacecraft trajectory correction maneuvers and atmospheric flight on Titan, stored for use during these
transient events using a large lithium-ion battery.
Figure 1. Dragonfly rotorcraft lander, surface configuration with HGA deployed.
In order for Dragonfly to soar majestically through the Titan atmosphere, it must first get to Titan. During cruise,
and on the launch pad once the MMRTG is installed, a pumped fluid loop that runs parallel to the lander’s internal
loop (intended only for surface operations) manages heat dissipation from the MMRTG, which is near 2000 W at the
beginning of the mission. The pump assembly, which is similar to the lander pumps, runs at a constant power, while
passive mixing valves on the cruise stage radiator segments adjust for thermal variations. The cruise stage fluid loop
attaches to a heat exchanger port on the MMRTG to maintain the fin root temperature near its optimum power
generation value. This heat dissipation will thermally control all cruise and entry vehicle components, such as the
tanks, valves, and electronics, as well as the aeroshell that surrounds the lander. Electrical heater power is not
required in normal operations and is minimized for transient events by this design approach. The radiator will have
two zones to allow the system to adjust to changing environmental conditions as the spacecraft travels through the
inner solar system and then outward to Titan and still maintain constant MMRTG and propellant tank temperatures.
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Figure 2. Cruise stage thermal block diagram.
Similar to the cruise stage thermal control system, the lander’s thermal control system harvests heat from the
MMRTG and distributes it throughout the body of the lander using a pumped fluid loop, but is completely separate
from the cruise stage fluid loop, which will have been jettisoned with the rest of the cruise stage on arrival to Titan.
The fixed amount of heat provided by the MMRTG used protect the lander’s internal components from the cold
Titan thermal environment will be preserved by carefully designing the level of thermal isolation between the lander
interior and its environment. External components on the lander will be designed to have survival temperatures < 94
K, such that they will not require survival heaters during hibernation. The performance of the lander TCS as well as
all components directly exposed to the Titan environment will be verified with testing on Earth in a Titan-relevant
environment.
Figure 3. Lander thermal block diagram.
II. Lander Thermal Control System
The heart of the thermal control system for the lander is the MMRTG. Heat generated by the MMRTG is
distributed throughout the lander body using a pumped fluid loop to maintain a typical thermal environment for its
internal components. An insulating layer of Rohacell™ foam protects the interior of the lander from the cryogenic
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and convective Titan environment by fully enclosing the MMRTG, battery, electronics and most science
instruments. Structural attachments, such as the mobility motor arms, landing legs, wires, camera and LIDAR
windows, and other penetrations to the insulating foam layer, are designed to minimize the heat leak from the lander
interior to the external environment. Some components, such as the mobility and sampling system motors, are
outside the lander interior and are designed and tested to survive in the Titan environment, with preheaters (in some
cases) to reach their minimum operational temperatures.
The thermal insulation for the lander is a 5-cm-thick layer of Rohacell™ 31 HF foam, which is a closed-cell
rigid foam based on polymethacrylimide chemistry with an approximate density of 31 kg/m3 and extremely low
dielectric constants with particularly favorable RF transmission properties at high frequencies. The effective thermal
conductivity through a 5-cm-thick layer of foam from 0°C (approximate lander interior) to −179°C (approximate
Titan ambient) is ≤0.035 W/m/K, verified by testing at the Johns Hopkins Applied Physics Laboratory (APL) in a
flight-relevant environment. The thermal conductivity of the foam is less than the datasheet value for this application
due to the decrease in material thermal conductivity with decreasing temperature. The external surface temperature
of the lander, including the outside of the MMRTG enclosure, is greatly attenuated by the foam insulation, resulting
in lander skin temperatures only 10–15°C above ambient (worst-case hot condition assuming no wind). A thin skin
of aluminized Kapton will be bonded to the outer surface of the foam for grounding during Titan surface operations
and handling during lander integration and testing (I&T).
The lander pumped fluid loop distributes the MMRTG heat, which is predicted to be 1670 W EOM, to
components within the lander body. The loop consists of a 1-cm inner diameter metal tube that runs along the length
of the lander, up to the lander top deck, and back, attaching to most boxes and the battery with flanges on the tube,
typically at the base of each box to simplify I&T (particularly for the battery). The heritage working fluid for
previous MMRTG missions is CFC-11 at 2 L/min, and a design trade is currently in progress for Dragonfly to
determine the optimum fluid and fluid loop architecture, for flight and for testing, for the lander and cruise stage,
that takes into account thermal performance, temperature limits, pump power, fluid availability, safety, government
regulations, reliability, radiation susceptibility, etc. The lander fluid loop will use one of the heat exchanger ports of
the MMRTG, as done on Mars Science Laboratory (MSL) [Paris et al., 2004; Bhandari et al., 2013]. This approach
will maintain the MMRTG fin root temperature near its optimum level.
Thermal trim devices, located one on each side of the lander near its aft end, will provide a Vernier-style
adjustment of the lander internal temperature, allowing for precise control of the MMRTG fin root temperature on
Titan. The thermal trim devices conceptually consist of an aluminum sheet metal, covered with a 5-cm-thick layer of
Rohacell™ foam, which opens using a linear actuator to expose the outside of the lander interior wall directly to the
Titan environment. The pumped fluid loop will be routed to the lander interior wall at these locations to maximize
the heat rejection capability of the device while physically separating the lander interior from the Titan atmosphere.
Because one trim device is at the fluid input to the MMRTG and the other is at the MMRTG output (and at the input
to the battery), the devices can be offset from one another to bias the MMRTG temperature warmer or colder
relative to the battery, in addition to biasing the lander internal bulk temperature warmer or colder. The trim devices
will be designed to leak only a minimal amount of heat to the external environment when fully closed. The size and
heat rejection capability of the trim devices will be determined during the typical detailed design process going
forward, and will be verified with component and lander level thermal testing.
The battery assembly is attached to flanges on the fluid loop to keep the battery above 0°C during cold survival
conditions and provide cooling for scenarios during which the battery dissipates only a moderate amount of heat.
The high thermal capacitance of the battery keeps its bulk temperature below its upper operational temperature limit
of 35°C during transient high heat dissipation cases, which only occur during atmospheric flight on Titan. The
battery bulk temperature only rises by 10°C during 30 min of powered flight, during which many lander internal
component heat dissipations (including the battery discharge) are at a maximum. To control temperature gradients
across the battery cells during these events, aluminum fin extrusions are placed between the cell stacks, with small
tube-axial fans envisioned to reject the heat to the lander interior, using the atmosphere that Titan generously
provides. The fans would operate only on the surface and only during atmospheric flight, and can be commanded to
turn on before the flight begins to precool the battery if needed (keeping in mind that the battery cannot be charging
if its temperature drops below 0°C).
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Most internal electronic boxes in the lander are mounted to the internal structure and dissipate heat to the
structure as well as the internal atmosphere (at Titan atmospheric composition but lower density due to the higher
temperature). Some higher heat dissipating boxes, such as the power switching unit (PSU) and inertial measurement
units (IMUs), are attached in close proximity to the fluid loop to maintain their cold survival and hot operational
temperatures within limits. The mobility rotor drive electronics will also have aluminum fin extrusions and fans to
limit their temperature during flight operations. A few internal items, such as the X-Band traveling-wave tube
amplifiers (TWTAs), are mounted directly to the lander interior top deck and dissipate heat to the wall by
conduction and to the interior fluid by convection (with one leg of the cruise stage fluid loop going to the top deck,
which passes through the lander and MMRTG, to limit the maximum operational temperatures of the TWTs during
cruise, during which fans will not be used).
The internal portion of the high gain antenna (HGA) gimbal assembly is thermally connected to the fluid loop,
either by the loop going across the top deck or by using constant conductance heat pipes (CCHPs) to make the
thermal connection (on Titan, the orientation of the pipes are conveniently appropriate for reflux operation). The
portion of the gimbal assembly that extends above the lander top deck is insulated with a 5-cm dome of Rohacell™
foam. The insulated dome is designed to allow the HGA dish to articulate in azimuth and elevation, and the
attachment between the HGA gimbal assembly and the dish is thermally isolated to limit the heat leak across that
interface. Conduction through the HGA gimbal stack, along with natural convection, keeps both HGA gimbals well
above their cold survival temperature limit of −100°C. A small 10-W preheater is used for 15 min to raise the
gimbal actuator temperature to ≥-40°C before operation and can drop to 5 W to hold that temperature during HGA
operation.
The lander has eight body-mounted cameras, which require holes in the insulation for transparent windows. The
survival temperature for these cameras is −135°C, so the heat leak associated with each one will be minimized by
isolating the cameras from the lander interior with a 2.5-cm-thick covering of Rohacell™ foam. The conduction
from the cameras to the lander exterior surface will be tuned such that the resulting camera hibernation temperature
is just above their survival limit, thereby minimizing the resulting heat leak to the Titan ambient. Thermal analysis
indicates that a single window pane is optimal for this configuration, which has been confirmed by preliminary
component-level testing. Each camera will have a 35 W preheater to raise the camera temperature before operation.
Most cameras, once preheated, will maintain acceptable temperatures due to their internal operational heat
dissipation, and the others will need a small amount of preheat to remain applied during operation.
Two panorama cameras are mounted to the structure of the high gain antenna, with the window of each camera
resting on the external surface of the lander’s top deck when the antenna is stowed. The side and back of the
cameras’ packaging will be insulated with a 5-cm-thick layer of Rohacell™ foam, with a thermally-isolated
structural attachment to the antenna. Thermal isolation through the lander’s top deck foam insulation at these
locations will be decreased by just enough to allow the right amount of heat to leak into the cameras to keep them
above their minimum survival temperature of −135°C during lander hibernation. The cameras will require a small
amount of heat when deployed to maintain their minimum operational temperatures when in use, and their minimum
survival temperatures if not in use but still deployed.
The lander thermal control design exposes a limited number of components directly to the Titan environment,
including the mobility motors, sampler drills and blowers, and landing gear. Special design and operational
considerations have been made for these components. Thermal modeling shows external components, such as the
landing struts, reach equilibrium with the Titan environment before initial landing, which will be verified with
component and lander level thermal testing.
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Figure 4. Lander external (left, cold survival) and internal (right, cold survival and hot operation)
temperatures on Titan.
The lander’s mobility motors are designed to survive in the Titan environment and require no survival heater
power. The motor bearings will be preheated with ~90 W each for 5 min before operation to a temperature of
−65°C. The heaters are located near the center of the motor, directly adjacent to the bearings. The internal structure
of the motor is largely titanium, so the windings will be colder, but this is desirable to limit the internal resistance of
the motor. During flight, the motor can dissipate up to 300W of heat but the temperature remains very cold, just
above the motor minimum operational temperature limit, depending on the exact motor operational profile. Unlike
motors of this type used in terrestrial applications, the Dragonfly mobility motors have no cooling fins. The cold
survival, preheating, and hot operational performance of the motor have been verified with preliminary thermal
testing in a Titan-relevant environment at APL and Penn State University (PSU), and the design of the mobility
motor will be evolved during Phase B and verified with testing.
III. Cruise Stage Thermal Control System
The Dragonfly spacecraft thermal design builds on concepts proposed by Lockheed Martin (LM) and APL in the
NASA New Frontiers Step 1 & 2 mission design architectures. The cruise stage fluid loop relies on MMRTG waste
heat to regulate cruise stage, lander avionics, and aeroshell while maintaining MMRTG temperature throughout
cruise period. The cruise stage design employs curved radiators and multi-layer insulation closeouts to provide
efficient entry system solar shading over the mission extremes of 0.615–9.07 AU. Figure 5 depicts the integrated
Dragonfly spacecraft thermal model which incorporates an APL Step 1 lander model that has been modified for
cruise simulations to assess hardware margins and set initial thermal conditions for the EDL assembly and lander.
No electrical power except fluid loop pump power is permitted or required by the cruise stage thermal subsystem
except for the reaction control system (RCS)/trajectory correction maneuver (TCM) propulsion and telecom
hardware elements to support TCM and telecom transients.
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Figure 5. Integrated thermal model is being used to validate configuration and CONOPS.
A detailed cruise stage fluid loop concept has been implemented in the Dragonfly system thermal model to
validate the zero-heater power cruise thermal control approach and efficient distribution of MMRTG waste to
protect cruise stage and lander hardware elements while maintaining the MMRTG within its required operating
temperature range from 0.615 to 9.07 AU. See Figure 6. The cruise stage pump assembly is currently located in an
open bay below the MMRTG to minimize fluid line losses and pressure drops. Two parallel fluid control zones are
split off from the pump assembly to regulate the fuel tank (blue) and open (green-magenta line) bays. Each of these
fluid control zones contains four parallel sub-circuits to provide uniform control temperatures for the hardware
elements within each zone. This is especially important as maintaining uniform temperatures across the four fuel
tanks promotes equal N2H4 propellant usage from each tank and principle axis alignment over the course of the
mission. Independent, passive mechanical fluid bypass switches are deployed on each radiator segment to
autonomously regulate fluid temperatures as solar loading, spacecraft loads, and MMRTG waste heat output
changes over the mission. The aeroshell radiator indicated in Figure 6 is used to warm aeroshell interior and
backshell interface above historical flight allowable limits. The 4-96% fluid bypass valve control range is employed
with a refrigerant pumping at 2L/min throughout the cruise period. To further trim fluid temperatures, the open bay
zone is disabled beyond 3.5AU; this may or may not be necessary in the final implementation. The defined fluid line
length in the two-zone series-parallel fluid network is just under 150 ft when both zones are enabled. Development
and optimization of this fluid network and associated hardware implementation is ongoing.
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Figure 6. Cruise stage cooling loop concept implemented in Dragonfly system thermal model.
Entry analysis mimics the changing flight configuration and environments illustrated in Figure 7. Event timing
and environmental inputs follow the approach successfully used by LM in support of the Mars Phoenix and InSight
missions with the substitution of a powered descent by the Dragonfly rotocraft lander in lieu of the propulsive
braking using the N2H4 descent engine burns on these Mars heritage missions. Aeroshell bondline temperature
profiles are provided by the LM and NASA Ames aerothermal team for the entry, descent, and landing (EDL)
trajectory and aeroshell thermal protection system (TPS) design baseline. These are combined with the aeroshell re-
pressurization and atmospheric convection effects to estimate aeroshell and lander temperatures from entry interface
through backshell separation. The Dragonfly thermal model organization by spacecraft element as shown in Figure 8
permits the seamless transition between physical configurations across the EDL phase boundaries.
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Figure 7. Entry and Descent simulation facilitated by Dragonfly system thermal model.
Figure 8. Integrated thermal model elements combined to simulate system configurations from launch to
powered descent.
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IV. Thermal Analysis and Test Campaign
System-level thermal models for the Dragonfly spacecraft and lander will be used to verify the thermal control
designs. Thermal analysis cases for the spacecraft thermal model include launch, low-AU cruise, high AU-cruise,
transient trajectory correction maneuvers, and Venus flybys. Thermal analysis cases for the lander include the Titan
surface hibernation survival (cold case) and transient surface operations (hot cases, which utilize the thermal
capacitance of the components within the lander as a heat sink). Preliminary thermal models for the spacecraft and
lander show positive thermal margins for all components.
A Thermal Exterior Losses (TEL) budget has been created for Dragonfly and is used to manage the heat leak
through all interfaces that penetrate the foam insulation, such as structural mounts, antennas, science instruments,
and camera windows. The lander on Titan will be immersed in a cryogenic, convective environment and special care
will be needed to account for all the ways heat can leak out of the system, and thermal engineers will need to be
there every time a hole, wire, window, or other leak is created in the protective foam layer, to assess the impact of
the design details. The amount of heat the lander has to stay alive is a fixed value, slowly decaying over time to such
a point (well after the primary mission) that the lander will reach a state of permanent non-operation (freeze to
death). During the early stage of the project, contingency is applied to the budgeted heat leaks, with additional
uncertainty factors applied to heat leaks that are determined by analysis (in some cases up to 80%), which will be
reduced as the design matures and heat leak values are informed by testing. The TEL manages this “death by a
thousand cuts” threat that Dragonfly faces, to ensure that the lander thermal control design will be robust enough to
survive the Titan environment.
The lander TCS can be tested before flight with high confidence, because the thermal aspects of the Titan
environment can be conservatively replicated on Earth in a full-scale lander thermal demonstration testbed that will
include all relevant interfaces. Natural convective effects within the lander interior are similar on Earth as compared
to Titan, with the changes to density and gravity largely canceling each other. Cold survival for the lander is
determined by external forced convection at the maximum Titan wind speed, which can be replicated with fans in a
high-pressure thermal chamber (currently being installed at APL) at the appropriate speed. The Titan thermal
environment is constant, changing very little during the course of a diurnal cycle or even seasonally, within ±2K
[Cottini et al., 2012; Jennings et al., 2016], and the heat output from the MMRTG is a known, predictable quantity
as a function of time. Final adjustment of the lander TCS will be made using planned changes in the effective foam
thickness to tune the lander internal temperatures to the desired level, which will be biased slightly warm, allowing
the trim devices to fine-tune the temperatures once on Titan. The trim devices could be fully closed late in the
mission to conserve the diminishing heat output of the MMRTG, offering the possibility of a mission extension.
MMRTG simulator thermal balance tests will be conducted at APL in summer 2020, and are extremely
important tests for Dragonfly. Both the cruise and lander thermal control designs hinge on the amount of heat
harvested from the MMRTG by a fluid loop, and so thermal balance tests will be used to verify the thermal model
predictions. An MMRTG simulator will be placed in a Rohacell™ foam enclosure, and run in a TVAC chamber
with a flight-equivalent fluid and flow rate, at a cold wall temperature similar to that of the cruise internal aeroshell
environment. Temperatures will be monitored for the entire system, including the inlet and outlet fluid temperatures,
and the resulting heat balance will be verified. The MMRTG simulator will then be placed in a Titan thermal
chamber and run at a range of pressures, up to 1.5 atm, to understand the MMRTG heat balance for the lander. The
amount of heat extracted from the MMRTG for both the cruise stage and the lander will then be verified, a critical
feature to put heat leaks per the TEL in context.
A lander full-scale engineering model will be constructed in Phase C that will host all critical heat leak
interfaces, such as the motor arms, insulation panels, HGA gimbal assembly, etc., so that each of these heat leaks
can be measured in context of a full-scale lander geometry and adjustments can be made as necessary to ensure a
robust thermal control design. Final testing with the flight lander will be conducted in a Titan-relevant environment,
with planned final adjustments being made to the insulating foam to achieve a precise thermal balance for the lander.
The Titan approach, entry and descent transient conditions with regards to the removal of the cruise radiators may be
examined in a Titan chamber by running a transient thermal case that bounds the expected timeline, to ensure that
the lander is robust to this scenario.
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System level thermal balance testing of the integrated spacecraft (cruise stage, entry system, and the Dragonfly
lander) will be completed in a representative cruise vacuum environment using an MMRTG simulator to
demonstrate the flight interfaces between the major system elements and generate the thermal performance data
required to correlate the system level model which will be used to perform many of the system thermal performance
requirements for spacecraft, cruise stage, and entry system. Test requirements, critical data elements, and thermal
performance limits are still under development.
V. Conclusion
Titan has been waiting a very long time for our chemists to arrive, and it’s high time we got them there. The
Titan environment is extreme, but is a known quantity (Titan is not like a box of chocolates – you know what you’re
going to get), and this, coupled with the deterministic nature of the MMRTG heat output and the testable, adjustable
nature of the Dragonfly thermal control design, gives high confidence that the mission will be successful. The solid
design concept will of course undergo the typical detailed design process going forward, and along the way will
avoid “death by a thousand cuts” by use of the TEL, which will account for and track each heat leak. Atmospheric
flight on another world is a very cool thing…
Dragonfly, the coolest mission ever flown!
Acknowledgments
The Dragonfly mission is supported by the NASA New Frontiers Program under contract to The Johns Hopkins
University Applied Physics Laboratory. The authors acknowledge NASA and the Dragonfly Project Team for
support in the preparation and presentation of this paper.
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