ASTRA - Advanced Space Tracking and Reconnaissance Array
Version: I01
Reviewed by: Mathieu Udriot, Marnix Verkammen, Stephan Hellmich, Andrew Price
Review date: 03/06/2025
Review status: ✅DONE (trajectory parts missing)
This study, conducted as part of the ENG-411 course at EPFL, addresses the critical challenge of Space Situational Awareness (SSA) in cislunar space (the region between Earth and the Moon). This study aims to design a sustainable, cost-effective space-based surveillance system capable of detecting and tracking objects larger than 1 meter. Recognizing the limitations of ground-based systems for continuous coverage, the mission proposes deploying a constellation of satellites at the Earth-Moon Lagrange points (L4 and L5), providing persistent monitoring of the Earth-Moon corridor. Through concurrent engineering, the team developed an architecture encompassing trajectory design, propulsion, payload, and subsystems, ensuring a 10-years mission lifetime within a budget of €250 million. The mission supports future lunar and deep-space operations by providing reliable SSA data to prevent conjunctions and promote responsible behavior in space.
The following contains all the relevant informating resulting from this study, from the context and mission objectives to lessons learned. For this edition, a space sustainability role has been added to the team.
This study was performed at eSpace Concurrent Design Facility by the following team:
Name | Affiliation | Role |
---|---|---|
Alexandre Rafael Aires Viegas | EPFL | Systems Engineering (SE) |
Aubin Louis Gérard Mercier | EPFL | Systems Engineering (SE) |
Alexandre Paul Corbaz | EPFL | Trajectory Analysis |
Jehan Névé Marc Corcelle | EPFL | Structure and Mechanisms |
Daniel Simon Christoph Gann | EPFL | Propulsion |
Aurélien Genin | EPFL | Configuration |
Adam Neale Antonin Lecroart | EPFL | Thermal subsystem |
Martin Jacques-Yves Lemaire | EPFL | Sustainability |
Maximilian Eduard Bonvin | EPFL | Power subsystem |
Samuel Arthur Wahba | EPFL | Communications & Data Handling (CDH) |
Jules Raphael Simon Streit | EPFL | Attitude & Orbit Control (AOC) |
Under the responsibility of:
Mathieu Udriot, EPFL Space Center, Study Coordinator
Marnix Verkammen, EPFL Space Center
With the technical support of:
Christian Cardinaux, EPFL Space Center, Systems Engineering Support
Stephan Hellmich, EPFL Space Center, Study acting customer
Andrew Price, EPFL Space Center, Study acting customer
Candice Norhadian, EPFL Space Center, Logistics & Admin Support
For a list of terms and acronyms often used, check the Glossary section. Additional acronyms specific to this study:
During the Spring semester of 2025, an interdisciplinary group of students took part in the third iteration of the concurrent engineering course, given through the Minor in Space technologies at EPFL. This course aims to teach graduate students the principles of concurrent design for space missions through a couple theoretical courses on concurrent engineering and five design sessions of 4 hours on a space mission.
With the increased interest in the moon and its resources, there will be more and more missions to this destination. This means more spacecraft will pass through the cislunar region to get there and thus there will be an increase in operations and debris in that region. There is thus a keen interest in observing and tracking objects in the cislunar region for Space Situational Awareness (SSA). This is the main objective of this mission, to track and characterize objects in this region to ensure safe passage of any spacecraft passing through this region, more specifically the Earth-Moon corridor.
The mission concept involves the deployment of a constellation of four identical satellites. Two satellites will be positioned near the Earth-Moon L4 Lagrange point, and two near the Earth-Moon L5 point. Together, they will provide continuous surveillance of the Earth-Moon corridor. The satellites will be equipped with instruments capable of detecting, tracking, and characterizing various types of objects. The system will deliver critical data for collision avoidance, debris monitoring, and long-term space traffic management in the cislunar domain.
The study focuses on the preliminary design of a constellation of four spacecraft dedicated to SSA in the cislunar region. With lunar missions becoming increasingly frequent, the Earth-Moon corridor is poised to become a congested and strategically vital space highway. To mitigate the risks associated with debris and uncontrolled objects in this region, the mission proposes deploying four identical spacecraft to the Earth-Moon Lagrange points L4 and L5, where they can provide persistent surveillance coverage.
Each spacecraft will be tasked with detecting, tracking, and characterizing objects in the cislunar domain, contributing to a real-time understanding of the dynamic space environment. The study aims to develop the preliminary mission architecture, including spacecraft subsystems, operational concepts, and budgets requirements, through a concurrent engineering process. The final design reflects a balance between performance, cost and reliability to evolving SSA needs.
The objective of this study is to do the preliminary design of the 4 spacecraft whose purpose is to observe the cislunar region.
Ref | Requirement |
---|---|
MIS-001 | The mission shall detect, track and characterize objects in the cislunar region |
MIS-002 | The mission shall deploy spacecraft to the L4 and L5 Lagrange points in the cislunar region to maintain stable positions for observation and monitoring |
MIS-003 | The mission shall have continuous monitoring of the Earth-Moon corridor |
MIS-004 | The mission’s lifetime shall last 10 years |
MIS-005 | The mission shall use the Ariane 62 as a launch vehicle |
MIS-006 | The mission cost shall not exceed 250 million euros |
MIS-007 | The minimum cis-lunar object size detected shall be 1m |
MIS-008 | The mission shall deploy 4 spacecrafts in total |
The main mission and system requirements design drivers were the mission objective and customer requirements. The spacecraft design is inspired by the heritage mission CHEOPS. As such, the spacecraft has a similar design and payload as both missions have a similar objective of observation. Furthermore, the main mission design driver was the “Acquisition of Objects in Cislunar Space with Small Spaceborne Telescope” study by Priedhorsky et al. (2024) which we based our mission on to allow continuous monitoring of objects in cislunar space.
The outcome of the study is the development of a robust and sustainable mission architecture for SSA in cislunar space. The proposed mission, ASTRA (Advanced Space Tracking and Reconnaissance Array), successfully fulfills the customer’s objectives by providing continuous surveillance of the Earth-Moon corridor and detecting objects larger than 1 meter.
General Architecture:
ConOps (Concept of Operation)
See figure below.
Scheduling
In the operational phase, the schedule of all 4 satellites is rythmed by the duration of a lunar month (29.5 days). During this period, half of the time is spent scanning the Earth-Moon corridor (60 deg large, 6 deg wide), with each section of the corridor scanned at least three times at a 1h frequency, to allow for initial orbit determination. Scanning the corridor in this linear fashion allows us to observe the regions with the optimal solar phase angle, maximizing the illumination and therefore the brightness of the objects observed. The schedule allows for more scans of each region of the corridor, or dedicated observations when an object is detected to better measure its orbit and characteristics if needed. When the Sun is on the opposite side of the corridor as the Lagrange point, the two satellites at that Lagrange point face away from the corridor to avoid being blinded by the Sun. During that time, they are available for secondary missions such as asteroid surveillance.
The following figure shows the scheduling in the operation phase, based on the lunar month duration.
Usually takes care of (from ESA CEC 2022, "Mission Overview and Requirements"):
- Define the orbit and transfers of the spacecraft
- Define delta v over lifetime
- Calculate ground station contact time
- Calculate eclipse duration
- (End of life)
Requirements:
Before talking about the different methods to achieve the requirements, I would like to give some background concerning Lagrange points. Lagrange points arise as equilibrium points in the earth-moon-satellite system where the mass of the satellite is considered as negligible compared to those of the two primaries. This kind of system is frequently called the restricted 3 body problem (R3BP). In theory, a satellite positioned at those points would stay there forever but in reality, objects aren’t exactly located at the precise lagrange points but appear to orbit around those points when viewed from a synodic frame of reference (a.k.a. a frame of reference where the two primary bodies appear stationary).
An example of a family of orbits around L4 is depicted in Fig. Traj. 2. These particular orbits are in the same plane as the lunar orbit plane but other kinds of orbits also exist in three dimensions. The key point here is to understand that “orbits” around lagrange points become apparent when viewed under the synodic frame of reference.
Fig. Traj. 1 - Satellite in the Earth-Moon synodic reference frame In this frame of reference only the satellite moves
[Tradeoffs]
Missing from report
[Justifications]
Missing from report
[Results]
Missing from report
Usually takes care of (from ESA CEC 2022, "Mission Overview and Requirements"):
- Create the configuration of the spacecraft
- Define the location of the equipment in the satellite
- Determine the MoI and CoG
Requirements:
[Design]
The configuration of the ASTRA spacecrafts is based on the ESA satellite CHEOPS. This small satellite of 1.5x1.5x1.5 m hosts a telescope with similar characteristics as the one required for ASTRA (see Payload). The main advantage of this architecture is that it uses fixed solar arrays and fixed antennas, reducing the number of mechanisms and therefore the number of possible failure points and complex parts.
Having fixed solar arrays is also justified by the fact that the telescope will have to always face away from the Sun ( 90 deg) to avoid being blinded by it. It is therefore meaningful to install the solar arrays on the opposite side of the telescope. Moreover, the use of a hexagonal-shaped structure enables to cover three faces with solar arrays, increasing the pointing range of the telescope while keeping a minimal power production (detailed in Power).
It has been decided to use fixed antennas for communication. This impacts the operation as it requires to halt the observations to point the antennas towards Earth to downlink data. This is completely compatible with the operation schedule, which provides enough time for communication. Because the satellites will be positioned at L4 and L5, the Earth is fixed from each satellite point of view. However, the Sun rotates around it in one lunar month. To be able to communicate with the Earth and still have the solar arrays illuminated, no matter the position of the Sun, two sets of antennas are used: one the +X face and one on the -Y face. They are moreover angled relative to these faces so that the telescope will not see the Earth (risk of blinding) when the antennas are facing the Earth.
[Results]
The figure below shows a simple CAD model of the ASTRA spacecraft. The telescope is shown with its shutter opened. It is placed on top of the satellite platform. On the three opposite faces are the solar arrays. The two sets of antennas are placed on the bottom of the +X and -X faces. The thrusters are positioned on the -Z face, with the launcher adapter.
The following figure shows the inside of the spacecraft by opening the different faces of the platform. The bi-propellant tank is positioned at the center and serves as a structural support. Each face can hold a volume of 500x700x240mm, where each subsystem’s components are positioned. Their placement is made to minimize harness (for example the batteries close to the solar arrays), to fulfill their requirements (two sets of reaction wheels on different faces to allow for attitude control) and to balance the satellite (according to REQ-CON-003). With the final configuration, the center of mass is located at (-0.049m, 0.004m, 0.65m) with the origin being at the center of the launch adapter (on the -Z face of the satellite). The satellite’s moments of inertia around the center of mass, and along the three axes, are (29.5kg.m, 13.2kg.m, 36.3kg.m). These values are used for dimensioning the AOCS.
The two figures below show how the four spacecrafts fit inside the fairing of the Ariane 62 launcher. The spacecrafts are placed side-by-side on a custom launch adapter. This solution was preferred to stacking them to avoid having to oversize the structure of the satellites to hold the weight of up to three other satellites during launch (around the equivalent of 5t given the maximum acceleration of the launcher). The satellites are released sequentially to avoid collisions.
Requirements:
[Design]
The payload for the ASTRA mission is an optical telescope observing in the visible spectrum. It is largely inspired from the payload of the ESA CHEOPS satellite. Some modifications were made to have a larger field of view, while ensuring a minimal resolution (according to REQ-PL-002 and REQ-PL-006).
The MIS-003 requirement requires that the satellite shall observe the full Earth-Moon corridor. It is defined as a 60 deg large and 6 deg wide arc. Given the 0.75 arcsec resolution chosen, this gives 8300 Gpx for the full image of the corridor, at a depth larger than 21 mag.
To fulfill these needs, while not generating an amount of data impossible to transmit (according to REQ-PL-005), the payload has been sized according to the table below.
Parameter | Value |
---|---|
Focal length | 1000 mm |
Diameter | 350 mm |
Field of view | 0.77 deg |
Sensor size | 20x20 mm |
Resolution | 0.75 arcsec |
Image size | 4096x4096 px |
Quantization | 16 bits/px |
The performance of this telescope would enable it to perform some really interesting astronomy studies (e.g. asteroid survey/follow-up observations) during the two weeks per month during which the satellites can’t observe the corridor.
Requirements:
[Tradeoffs]
The main factors that affect the satellite in terms of structure is the reliability against external events as shocks and the use of a
This trade off can be assessed by comparing the specific stiffness (E/rho) and yield strength/density ratio of different materials.
For the structural parts, three classical space-craft materials are compared : Aluminium alloy (Al 7075-T6) , Titanium alloy (Ti-6Al-4V) and Steel alloy (highly alloyed Cr-Ni).
In terms of specific stiffness, they are all really similar (around 0,0224 GPa·m³/kg), but in terms of tensile strength, Titanium has a great advantage, as seen in the table below.
Material | Yield Strength (MPa) | Density (kg/m³) | Specific Yield Strength (MPa·m³/kg) |
---|---|---|---|
Aluminium alloy | 448 | 2800 | 0.160 |
Titanium alloy | 830 | 4500 | 0.184 |
Steel alloy | 900 | 7900 | 0.114 |
This means that Titanium alloy is ideal for critical load paths where weight and strength matter, where Al alloy offers a great trade-off with lightness and decently strong. Steel, while been really strong, is too heavy so used in high.load points if critical.
It is possible to create a Trade-off chart from a Trade-off table to clarify the best material for our use.
While Aluminium alloy has a better score with the addition of weight factors, the titanium alloy will also be selected in case of problematic loads.
For walls, honeycomb structure is chosen as it is the mainly used material for this application as in the Cheops mission. It will drastically reduce the weight and handle every subsystem as it is possible to fix with screws in it.
For the two platforms, carbon fiber composite (CFRP) is selected as it has the unique property to optimize the force distribution with the orientation of the different stacked layers of long fibers with only 5 to layers.
[Results]
According to the Ariane 6 User's Manual (Issue 2 Revision 0), the maximal compressive load in the Ariane 6.2 during the launch and release phase is 3.1 g (ESR Jettisoning) and the maximum of traction stress is around 6 g (at ESR End of Flight). From this, the loads on each critical part is derived :
The FAP (Flat adapter Port) experience 15,000 N in compression and 59,000 N in tension. These values are derived by applying the launch acceleration to the total mass of all four satellites mounted on the platform.
The SCA (Separation Clamp Adapter) endures up to 2,430 N in compression and 12,262 N in tension, based on the mass of a single satellite subjected to the same acceleration loads.
Each Stringer needs to support 1,962 N in compression and 817.5 N in tension, under the assumption of uniform distribution of the total payload mass and upper structure across six stringers.
The critical load ( Pcrit ) at which a slender, ideal column will buckle is given by:
Where:
We have a maximum buckling of Pcrit = 2’004 N for Aluminium and Pcrit = 3’246 N for Titanium, considering 1 cm by 1.5 cm section and 80 cm length.
It is preferred to have a security factor of 1.5 to certify the integrity of the structure, the Titanium is chosen to stay at a pretty small section area, diminishing the mass.
Moreover, in terms of diminishing thermal expansion, critical to avoid movement of the Payload, a 80 cm stringer will expand by 13 mm for an Al alloy and 4 mm for a Ti alloy (DeltaT = 320°C)
To reduce bending moment, vibrations and compression of the x,y plane, the composite structure is chosen to be a [0,-45,45,90,45,-45,0] quasi-isotropic layup for an average height of 1mm. The honeycomb structure is an aluminium space-grade sandwich.
Finally the total mass calculated is 55.91 Kg with the sum of 6 honeycomb panels, 2 small stringers (80cm), 4 large stringers (150cm), 1 full composite plate and 1 half composite plate.
By adding the 25% of the structure mass for the bild, screws and fixations systems and another 10% of the mass for a safety factor, it appears the structure weighs 75.48 Kg.
In terms of mechanisms, the selected adapters are sourced directly from established manufacturers to ensure safety and reliability, as their components are backed by detailed datasheets and flight heritage, confirming their ability to withstand the calculated mechanical loads. The FAP is sourced from Moog with a tailored features of 4 clamp band fixation rather than 2 and the SCA are the (SAURON) 15” - from UAR X.
To ensure reliable operation during the opening phase of the shutter mission sequence, a brushless motor with a mass of 0.5 kg has been selected. The motor need to deliver a torque of 0.0013 N·m and achieves a rotation speed of 10°/s, values that are basics for brushless motors.
The shutter itself, made of aluminium and weighing 1.5 kg, is designed to be open smoothly after deployment, thereby minimizing the risk of contamination or damage at ground. It is also designed to close if necessary to avoid any cell damage by sun exposition or debris damage during orientation and displacement sequences.
To design an efficient and reliable propulsion system for the satellite, a systems engineering approach was chosen. The following chapter begins by defining the requirements given by the customers for the propulsion system. Based on these requirements, a trade-off analysis is conducted using various evaluation criteria relevant to the mission. These criteria were developed in collaboration with other departments.
Following the trade-off analysis, the propulsion system is designed at the component level. This includes decisions on the propulsion type, propellant selection, and the sizing of thrusters, tanks, and piping. These design decisions are discussed in detail in the chapter Justifications. The report concludes with an overview of the mass and power budget, as well as an estimate of the total cost for the propulsion subsystem.
Considering all the requirements, we can now dive deeper into the system design and start with the decision for an electrical or chemical system. This choice significantly influences the overall development and sizing of both the propulsion system and the satellite itself.
To identify the most suitable system for the mission, discussions were held with the trajectory team, the systems engineers, the power subsystem, and the configuration department. The interfaces between propulsion and these subsystems made it necessary to involve all of the mentioned departments.
The selection process followed this structure:
Criteria Definition and Weighting:
All relevant criteria for the propulsion system were first identified and assigned a weighting based on their importance for the mission. The weighting scheme is the following: Reliability > Mass > Electrical Power Consumption = Thrust > Cost
System Evaluation:
Next, the main propulsion options, monopropellant, bipropellant, and electric propulsion, were assessed against each criterion. Points were awarded based on how well each option satisfied the weighted requirements. This can be seen in the following figure.
Final Decision:
Based on the final scores and the applied weightings, a decision was made. The selected solution is a bipropellant system using monomethylhydrazine (MMH) as fuel and dinitrogen tetroxide (NTO) as oxidizer.
Total Score Electrical Propulsion: 6
Total Score Monopropellant: 6
Total Score Bipropellant: 7
With the final propulsion type selected, the system development can now proceed at the component level. This chapter focuses on the detailed design of the individual subsystems that make up the propulsion system.
Propellant Mass
One of the most critical parameters for the overall satellite system is the required propellant mass. It was determined through several iterative loops, with increasing accuracy in each step.
The final deltaV requirement for the mission was given by the Trajectory and Sustainability departments. The total deltaV needed for the mission is 511 m/s.
Given this requirement, along with:
a specific impulse of Isp = 320 s (given by the propellant MMH/NTO),
the gravitational constant g0,
and the current total mass of the satellite,
the dry mass of the satellite, and thus the required propellant mass, can be calculated using the Tsiolkovsky rocket equation:
From the calculations above, the required propellant mass was determined to be m_fuel=65.49 kg. However, to ensure adequate system reliability and redundancy, a margin of 10% was applied. This results in a total propellant requirement of 72.05 kg.
The deltaV distribution across the individual maneuvers, along with the corresponding propellant consumption for each, is summarized in the following table:
Maneuver | Needed DeltaV [m/s] | Needed Propellant [kg] |
---|---|---|
L2_dep | 50 | 6.89 |
L4/L5_injection | 100 | 13.45 |
Station keeping (10 years) | 300 | 37.88 |
EOL Maneuver | 61 | 7.27 |
Total | 511 | 65.49 |
Table with needed deltaVs]
Propellant Tanks
Once the required propellant mass was calculated, the sizing of the propellant tanks could begin. Due to the limited available space within the satellite, titanium tanks were selected. Titanium offers an excellent balance of low weight and high structural strength, making it well-suited for this application. Given the mixture ratio of 1:1.65 (MMH:NTO), the individual masses of fuel and oxidizer were calculated. Based on these values, we could get the total tank volume. Finally, the tank’s structural mass was calculated.
With a wall thickness of 1.5mm the total weight of the empty tank is m_Tank=6.04kg.
Thruster
To maneuver the satellite, a dual-thruster system is used, consisting of two Inconel nozzles, each providing 200N of thrust. This setup ensures increased reliability through system redundancy. Both thrusters are mounted on the underside of the satellite.
Due to the compact size of the nozzles, as seen below, the satellite can continue maneuvering if one thruster fails, since both are aligned to act through the center of mass.
The following parameters were calculated:
Propellant Pipes
To transport the propellant from the tank to the engine, propellant pipes are needed. The selected material for the pipes is titanium. This enables the pipes to be lightweight while also ensuring safe transport of the propellant to the engines. Based on the engine’s mass flow rate and the pipe diameter and length, a total mass of 0.04 kg was calculated.
The final propulsion system is based on a bipropellant configuration using MMH/NTO. The goal was to design a reliable propulsion system that operates effectively throughout the satellite's entire lifecycle. The resulting configuration delivers sufficient thrust while meeting all customer-defined requirements. The key system parameters for the propulsion subsystem are as follows:
Thruster: 2x 200N inconel thruster
Propellant: MMH/NTO
Tanks: Spherical titanium tanks
Total Power Consumption: 240W (40W Controls, 80W Pumps, 120W Heating)
Total Mass Propulsion System: 79,65kg (7,6kg dry mass / 72,05kg propellant mass)
Total Cost Propulsion System: 425.568 EUR
Requirements:
[Tradeoffs]
FACTOR 1 : ACTUATORS/SENSORS selection (theory)
The first step was to make a selection of sensors and actuators which would allow us to control the full attitude of our satellites. This part will detail everything for one single satellite. Here is the final choice :
SENSORS
Sun sensor: One on each of the eight external faces of the satellite
Gyroscope: One unit, inside the satellite, placed on one of the six ‘petals’
Star tracker: Two units, theoretically only one is necessary => redundancy
ACTUATORS
Reaction Wheels: Three units, one on each axis + one for redundancy
Gas thruster: Six units, to desaturate reaction wheels
Once it was done, I could start to search for existing datasheets in order to have first values to set in COMET for a first iteration.
FACTOR 2 : TORQUES : Available vs Required
Then I started to derive both the required torques and available torques on each axis with the previous selection of actuators. Results were good. The required torques to operate a rotation of and angle theta [rad] around each axis were calculated with the following math :
FACTOR 3: Mass&Dimensions available
From this point, we did a second iteration on COMET and I considered my first constraints coming from other subsystems.
FACTOR 4: POWER CONSUMPTION
I did get a proper ‘available power’ value from the power subsystem but I kept trying to minimize it as much as possible.
As the iterations kept going, I had to change my selection, doing a tradeoff between mass & dimensions and torques needed, always taking long reliability as first priority and minimizing power consumption.
Torques needed, and mass available kept changing over the weeks due to variations of the total mass and moment of inertia.
[Justifications]
As mentioned above, the actuators-sensors package was constantly changing. I wanted to add as much redundancy as possible but I was limited by my available mass and the power consumption. Some additional elements have also been considered like an Earth sensor but later cancelled because of its inefficiency that far from Earth. A controlled moment gyroscope was also part of the first selection but was the most heavy (~15kg) and the most power consuming (~25W) element above all. I noticed during my calculations of torques that other actuators were sufficient.
We chose to put a sun sensor on each face of the satellite as an insurance, it would maybe not be necessary to have that much but these devices are light and low consuming.
While reaction wheels and gyroscope are located inside the satellite, on one of the six ‘petals’ (see Configuration subsystem). Most of the sensors and actuators are located on the external faces of the satellite. Locations and thrust directions of gas thrusters have been determined to allow the three rotations (around x,y and z axis) while not interfering with telescope and star tracker FOV.
GasThrustersLocation]
[Results]
Component | Quantity | Mass [kg] (per unit / total) | Mean Power [W] (per unit / total) | Peak Power [W] (per unit / total) |
---|---|---|---|---|
SENSORS | ||||
Sun Sensor | 8 | 0.65 (5.2) | 0.3 (2.4) | 0.4 (3.2) |
Gyroscope | 1 | 4.6 (4.6) | 25 (25) | 32 (32) |
Star Tracker | 2 | 2 (4) | 10 (20) | 12 (24) |
Sensors Subtotal | 13.8 kg | 47.4 W | 59.2 W | |
ACTUATORS | ||||
Reaction Wheels | 4 | 5 (20) | 5 (20) | 8 (32) |
Gas Thrusters | 6 | 0.6 (3.6) | 5 (30) | 5 (30) |
Actuators Subtotal | 23.6 kg | 50 W | 62 W | |
TOTAL | 37.4 kg | 97.4 W | 121.2 W |
This resumes all the torques available for rotations around the x,y and z axis passing through the center of mass. One main assumption has been made : the center of mass is on the z axis shown above.
Component | Torque [Nm] x axis | Torque [Nm] y axis | Torque [Nm] z axis |
---|---|---|---|
Thruster 1 | 0.065 | 0.135 | 0.15 |
Thruster 2 | 0.065 | 0.135 | 0.15 |
Thruster 3 | 0.065 | 0.135 | 0.15 |
Thruster 4 | 0.065 | 0.135 | 0.15 |
Thruster 5 | 0.15 | 0 | 0.15 |
Thruster 6 | 0.15 | 0 | 0.15 |
Reaction Wheels | 0.2 | 0.2 | 0.2 |
Total torque available | 0.76 | 0.74 | 1.1 |
To face available torques, I computed required torques to rotate the satellite by an angle of alpha [rad] at different fixed times. Here are the plots:
Since we don’t have explicit requirements about it in the documentation we had, we can only try to derive a torque from the technical notes:
180 × (60s integration + slew time) ≤ 86,400s
→ Maximum slew time per pointing ≈ 20s
On our 3 plots we can determine what torque would be necessary to do such a rotation around each axis from different slew times:
Temps \ Axe | Torque X (Nm) | Torque Y (Nm) | Torque Z (Nm) |
---|---|---|---|
5s | 0.32 | 0.30 | 0.50 |
10s | 0.05 | 0.17 | 0.13 |
20s | 0.019 | 0.018 | 0.032 |
All these values of torques are available with our design.
If I were to continue the project, I would focus on finding more efficient ways to control the rotations by studying the thrust curve documentation. So far, I’ve simply assumed it was feasible, given that our gas thrusters can produce thrust in multiple directions to counter each rotation.
The Command and Data Handling System shall provide the satellites with the necessary infrastructure to process, store and exchange information — such as commands and data — with the ground segment.
This mission statement was further refined as the sources of information were readily identified in the form of the satellite itself — hereinafter referred to as the Telemetry, Tracking and Command (TT&C) — and the payload. The C&DH system therefore needed to be designed so as to accommodate both pipelines simultaneously.
Standards and regulations applying to the present scenario were taken into account in the design of the C&DH System. Most importantly for this project, standardized margins of safety are provided in [CDH_REF_01]. Furthermore, the available ground infrastructures were assumed to be limited to the ESTEC’s network of ground emitters and receivers, a list of which is provided in [CDH_REF_02]. Knowledge of the ground segment was taken into account and included into the system’s link budget.
For the purpose of this project, the design was simplified by strictly limiting the selection of components to pre-existing commercial off-the-shelf (COTS) options.
Finally, other subsystems, particularly the Power Subsystem and Configuration Subsystem, will impose lower-level design constraints, which were taken into account within the technical specifications of the subsystem.
Figures of Merit (FoM) were used to facilitate trade-offs by providing objective and quantifiable elements of comparison between various design options. Moreover, by defining a set of FoMs, one obtains the core components used in high-level requirements elicitation.
ID | Name | Type | Metric | Range |
---|---|---|---|---|
CDH_FOM_01 | Mean Time between Full Transmission | Minimization | Duration [h] | [0;+∞[ |
CDH_FOM_02 | Mean Spatial Resolution Loss | Minimization | 1 - \frac{\text{Data Size Transmitted}}{\text{Data Size from Payload}} | [0;1] |
CDH_FOM_03 | Mean Path Redundancy | Maximization | number of path available to transmit data from source to destination | [1;+∞[ |
CDH_FOM_04 | Modularity | Maximization | [1;+∞[ |
The design process was centered around the establishment of a link budget. Beyond providing direct insight into the feasibility of each option, it also provides a quick and efficient way to extract the values of the aforementioned FoMs. The equations driving the models can be found in [CDH_REF_03].
The first step in designing the Command and Data Handling (C&DH) system was selecting an overarching architecture—determining how to structure the various functionalities into distinct components. Guided by the chosen set of Figures of Merit (FoMs), a bus-modular architecture centered around a centralized on-board computer (OBC) was adopted. This approach offered a balanced trade-off between performance and modularity, with the added benefit of simplified reliability mechanisms through the integration of multiple redundant units onto the bus.
However, a key limitation of this architecture is the single point of failure (SPoF) introduced by the central bus, specifically the OBC. To address this vulnerability, enhanced redundancy mechanisms were incorporated into the bus design.
The S-Band and X-Band were selected for the TT&C and Payload Downlink, respectively. These frequency bands are commonly employed in space missions and are well-suited to ESTEC’s ground infrastructure. It is also important to note that, while the Payload Downlink operates over a single RF channel, the TT&C subsystem requires full duplex communications to accommodate both uplink and downlink operations.
Together, the previously discussed constraints, selected Figures of Merit, and the high-level architectural and design decisions formed a comprehensive foundation for the system’s technical specifications. As a result, the subsequent lower-level design was reduced to finding the best-fitting combination of COTS components.
Mean Spatial Resolution Loss
The final CD&H System design directly follows from the above system architecture, for a total mass of 22.73 kg. The system’s components are listed in the following tables:
Name | Quantity | Band | Mass | Peak Gain |
---|---|---|---|---|
Anywaves S-Band TTC Antenna | 2 | S-Band | 0.59 kg | 6.5 dBm |
Anywaves High Gain X-Band Downlink Antenna | 2 | X-Band | 0.98 kg | 15.5 dBm |
Name | Quantity | Band | Mass | Power Draw | Tx Power | Data Rate |
---|---|---|---|---|---|---|
RocketLab Frontier-S | 1 | S-Band | 0.59 kg | 6.8 W | 28.5 dBm | 20 Mb/s |
LL3Harris CXS-1000 | 2 | X-Band | 5 kg | 12 W | 40 dBm | 400 Mb/s |
The chosen configuration — two X-Band transceivers and one S-Band transceiver — is a direct consequence of the capabilities of both transceivers. Firstly, the Frontier-S have two redundant channels per direction (i.e. two Tx and two Rx channels). Secondly, should the Frontier-S fail, the capabilities of the CXS-1000 would allow for the entire TT&C traffic to be passed through the X-Band channels without much impact on the Payload Downlink operations.
Name | Quantity | Mass | Power Draw | Storage Capacity |
---|---|---|---|---|
Beyond Gravity Next-Gen OBC | 1 | 9 kg | 38 W | 789 Gb |
Beyond Gravity’s Next-Gen OBC was chosen as it not only has sufficient storage capacity to support the Paylaod’s operations but also incorporates two redundant units — as if there were two identical OBC.
The modes of operations are not within the scope of the C&DH subsystem. The system’s design and configuration instead ensures that any potential operational needs could be fulfilled. The power needs for said operations were handled by the Configuration and Power subsystems.
The link budgets for each RF channel were constructed around the SNR per bit (), which are then compared against the margins specified in the requirements. Each budget takes the emitter, the receiver and the ‘path’ — the distance traveled in free space. As the chosen frequency bands were of small-enough frequency, the effects of the atmosphere, especially rain fade, could be neglected.
These are the simplified calculations used to compute the budgets for each RF channel. Note that the antenna pointing losses are negligible and thusly omitted from this index. The minimum , against which the margin is computed, is set to 10.5 dB as per [CDH_REF_02]
Effective radiated power: Total power emitted at the transmitting antenna
Symbol | Name | Units |
---|---|---|
P_ | Transmitter Power | dBm |
G_ | Transmitter Antenna Gain | dBi |
L_ | Tx-side Lines Losses | dB |
Free Space Losses: Lost power as the wave travels through free space
Symbol | Name | Units |
---|---|---|
Distance travelled in Free Space | km | |
Frequency | GHz |
SNR per bit: Normalized signal-to-noise ratio w.r.t to the frequency bandwidth
Symbol | Name | Units |
---|---|---|
T_ | Rx-Side Noise Temperature | K |
Data Rate | b/s |
The Electrical Power Subsystem (EPS) was tasked with providing reliable and autonomous power generation, storage, and distribution over a mission duration of ten years. The system was constrained to operate solely on solar energy and required to support critical mission modes including continuous observation and multiple daily communication sessions.
The design philosophy adopted for the EPS prioritized mechanical simplicity and robustness. As such, the solar arrays were dimensioned first, based on fixed-side panel mounting, and the energy storage system was then sized to compensate for illumination variability. This approach allowed early integration with configuration and thermal teams, and simplified the interface with AOCS by avoiding deployable or steerable panels.
A late-stage update from the CDHS team led to a significant design shift: instead of assuming one communication session per day, the satellite was expected to perform up to six. Given available mass margins, the battery system was scaled accordingly through modular replication rather than reworking the entire energy model, ensuring feasibility within the project timeline.
The EPS was structured into three core functions:
Functional Requirements:
Performance Requirements:
Assumptions:
Design Approach and Assumptions
The sizing of the solar arrays was the starting point for the EPS design. The strategy adopted was to first fix the surface available for solar energy collection based on the spacecraft’s external geometry and thermal constraints. Battery storage was then sized to compensate for energy shortfalls during periods of low illumination. This design sequence ensured early compatibility with the configuration and thermal teams and allowed the elimination of deployable or steerable panels.
Three lateral faces of the satellite were assigned to fixed solar panels. Each face provided approximately 0.8 m², for a total active area of 2.4 m². This layout allowed for at least one panel to maintain a favorable orientation to the Sun throughout most operational phases.
According to the trajectory and operations teams, observation phases occur under near-optimal Sun incidence, enabling maximum power generation. Communication windows, on the other hand, coincide with constrained spacecraft orientations and result in the worst illumination angles (27°, with respect to the most illuminated side panel), representing the power minimum.
Given the stable orbital configuration and the mission’s predictable scheduling (see Operations), a more detailed, time-resolved power mode analysis was not deemed necessary. The power subsystem was therefore dimensioned based on two bounding cases—DAY and ECL—which represent the best and worst illumination scenarios respectively. This approximation was validated in coordination with the CDHS and AOCS teams and ensures robustness across all intermediate states.
Environmental and Cell Characteristics
Parameter | Value | Units |
---|---|---|
Solar constant (lunar distance) | 1360 | W/m² |
Worst-case sun angle (communication) | 27 | degrees |
Mission duration | 10 | years |
Solar cell technology | GaAs CTJ30 | – |
Ideal efficiency (BOL) | 29.0 | % |
Derating due to temp, transmission, angle | 64.8 | % |
Yearly degradation | 3.0 | % |
Cumulative degradation over mission | 0.737 | factor |
The effective BOL and EOL power densities were computed as:
Power Generation Performance
Power generation was evaluated in two distinct modes:
Scenario | Power BOL | Power EOL | Units |
---|---|---|---|
Observation (DAY) | 388.7 | 286.7 | W |
Communication (ECL) | 88.2 | 65.1 | W |
Total power was computed from the surface area and power densities:
Mass Breakdown
Component | Value | Units |
---|---|---|
Cell surface density | 0.9 | kg/m² |
Structural layer + frame | 4.5 | kg/m² |
Total panel surface (3 panels) | 2.535 | m² |
Solar cell mass | 2.28 | kg |
Support structure + integration mass | 11.4 | kg |
Total solar array mass | 13.7 | kg |
Each panel contributes approximately 4.56 kg to the system. The integration mass estimate includes substrate, interconnects, and framing. Values were coordinated with the configuration and thermal teams to ensure mechanical compatibility.
Technology Selection
The CTJ30 solar cells selected for the mission are fully qualified according to ECSS-E-ST-20-08C and offer a BOL efficiency of 29.5% under AM0 conditions. Their high radiation resistance and stable output over time justified the assumption of a 3% annual degradation rate. Full specifications are provided by the manufacturer (CESI, 2020).
Power Budget and Energy Requirement
Battery sizing was driven by the need to cover power deficits during 1-hour communication sessions, which occur under worst-case illumination (ECL mode). The CDHS team confirmed late in the study that up to 6 such sessions per day were feasible. To preserve the integrity of the design timeline, the battery system was scaled by replication—one pack per session—without redesigning for this new regime.
Power demand per subsystem was estimated for both operational extremes:
Subsystem | High Illumination | Low Illumination (ECL) |
---|---|---|
CDHS | 68.8 W | 68.8 W |
AOCS | 97.4 W | 97.4 W |
Payload | 60.0 W | 2.4 W |
Other subsystems | 0.0 W | 0.0 W |
Total | 226.2 W | 168.6 W |
The solar arrays generate only 65.1 W under ECL conditions at EOL, resulting in a net deficit:
This shortfall must be supplied by the battery over a 1-hour communication session.
Battery Sizing
Battery capacity was calculated using the standard formula from the course:
Where:
Plugging in:
Each pack must thus provide at least 207 Wh usable energy.
Pack Design and COTS Technology
The chosen technology is the EaglePicher LP33037 Li-ion NMC cell, with the following characteristics:
Parameter | Value | Unit |
---|---|---|
Nominal voltage | 3.6 | V |
Capacity per cell | 60 | Ah |
Energy per cell | 216 | Wh |
Mass per cell | 1.6 | kg |
Specific energy (datasheet) | 160 | Wh/kg |
Temperature range | -20 to 60 | °C |
Each battery pack contains 4 LP33037 cells in parallel:
This provides over 2× the required session energy, offering redundancy through overcapacity rather than duplication.
System Sizing and Architecture
System Parameter | Value | Unit |
---|---|---|
Energy required per session | 103.5 | Wh |
Usable capacity per pack | 432 | Wh |
Packs used per day | 6 | – |
Number of cells per pack | 4 | – |
Mass per pack (est.) | ~6.8 | kg |
Total battery mass | ~40.8 | kg |
The modular architecture simplifies power management, tolerates partial degradation, and ensures each session can be powered independently.
Technology Selection
The LP33037 cell was selected for its high energy density, space-qualified stainless-steel enclosure, and thermal robustness. Its cycle life and electrical characteristics exceed mission needs. Over-sizing via modular replication ensured rapid integration after late mission requirement updates.
Subsystem Totals
Component | Mass (kg) | Notes |
---|---|---|
Solar arrays | 13.7 | Includes structural, support, and panel mass |
Batteries | 40.8 | 6 packs, each composed of 4 LP33037 cells |
Harness | 40.0 | Estimated as 10% of total satellite dry mass |
Total EPS | 94.5 | Compliant with system mass budget |
Remarks
Requirements:
[Tradeoffs]
[Justifications]
The next steps are is:
[Results]
Requirements:
[Tradeoffs]
There are 2 tradeoffs that are performed by the sustainability role. The other tasks purely serve a purpose of assessment. These two tradeoffs are the launcher selection and the end of life strategy. These are concurrently performed with the systems engineers. The objectives and alternatives for both are listed below:
Launcher Selection:
Objectives:
Alternatives: (European)
Decision support for the end-of-life strategy:
Objectives:
Alternatives:
[Justifications]
Launcher selection
From the information that we have, we establish an index for each of the propellants (See table 1). We are then able to tailor the assessment to any launch vehicle using its propellants composition and performing a weighted average (See equation 1). An implementation of the index can be observed on the figure 1 with the currently operational launchers and the future ones, where the index is re-normalized for the sake of the graph. We can clearly see that the selected launcher (Ariane 62) is currently the highest performing in terms of atmospheric impact.
Table 1: Atmospheric Impact of Typical Launch Vehicle Propellants. Data on atmospheric effects from “Space sustainability isn’t just about space debris: On the atmospheric impact of space launches” (Sirieys et al., 2022).
Equation 1: Index for the Evaluation of the Atmospheric Impact of a Launch Vehicle. Solely based on the Propellants of the Launch Vehicle.
Figure 1: Decision Support for the Selection of Launch Vehicle. Based on a tradeoff between sustainability and affordability. Sustainability Index normalised from Equation 1. Non European Launch Vehicle Displayed as Indication but Out-of-Scope for the Mission Requirements. Clusters found through k-means clustering with k=4 (SLS identified as outlier). All results normalized by MinMax. Own Figure. Data on future launch vehicles is indicative and uncertain.
End-of-Life Strategy:
The figure 2 shows the selection of the end-of-life strategy among the different alternatives. Uncertainties are identified and mitigated through additional propellant, enabling the definition of Real-Options to increase the flexibility of the strategy (See CONOPS in the results section, Figure 5).
Figure 2: Tradeoff Analysis for the Selection of the End-of-Life Strategy. Own Figure.
Then to establish the score of the end-of-life strategy, we use the following qualitative rationale:
High Level Life-Cycle Assessment:
To perform the high level life cycle assessment, we are going to use the following table as reference (See table 2). This table was AI-generated and deemed good enough for the sake of the course, enabling high level tradeoffs and selection of technologies.
Table 2: Carbon Footprint of the Different Technologies. Basis for the Assessment of the Environmental Impact of High-Level Tradeoffs performed by the most impactful subsystems.
Then from these values and the mass of the different components, we can perform an estimation of the total carbon footprint and normalize it by using the boundary values (See figure 3). This framework allows us to extract a score for each subsystem and one for the entire system.
Figure 3: Illustration of the Tradespaces for the most impactful subsystems in terms of the Carbon Footprint (Left). On the right is shown the tradespace for the entire system, based on typical mass proportions of satellites at different scales (e.g. no propulsion for smaller spacecrafts). Boundaries defined by the extrema of Table 2. Own Figure.
Assessment of the safety of the mission
We desire to assess the safety of the overall mission. We define hazards as all undesirable events that occur from within the system boundaries, like the failure of a subsystem. In this part we want to identify all the parts of the system that may fail or behave in a way that was not intended. Then we want to analyse the behavior of the system that is caused by such an issue.
After having identified the hazards that may arise within the system. We want to identify whether mitigations exist to counteract undesirable behaviors. These mostly take the form of redundancy when it comes to hardware but may also be planned modes transition in given circumstances. The state of the system after the mitigation must be assessed to ensure that it is an effective one and that it is sufficient to ensure the survival of the system.
We use the following qualitative rationale to evaluate the safety of the system:
In our case the main hazards are identified as follows, with the identified mitigations:
Assessment of the resilience of the mission
We define resilience as the capacity of a system to provide value under unexpected conditions. These conditions are defined by external forces, which themselves constitute the main source of uncertainty for any system. Hence we want to characterize a case of degraded conditions that is possible and evaluate the performance of the system under these circumstances. The difference of provided value between the expected scenario and the degraded scenario will characterize how resilient the system is.
To characterize the environment of the system, we start by identifying the external forces of the system. These external forces are all the factors that may impact the function of the system but are out of the boundaries of the system. In our case, the main external forces are the debris and the solar activity.
After having identified the external forces, we want to model them to accurately define a degraded scenario. We could produce stochastic models, especially for the debris, but given the time constraints that are inherent to the design sessions, we will limit ourselves to simple scenario planning. This gives us the following:
EXT_FORCE_01: Debris Population
EXT_FORCE_02: Solar Activity
Now that we have characterized the external forces of the system, we can provide a relevant description of degraded and critical cases for the system, and hence evaluate the outcomes of the system in these scenarios. Given the constraints imposed by the format of the project, we cannot quantitatively assess the outcomes of the system. Hence we will limit ourselves to a qualitative assessment as follows:
Normal Conditions
Degraded Conditions:
Critical Conditions:
We then evaluate the resilience of the system using the following qualitative rationale:
Mission Sustainability Score:
Finally, now that we have defined how we evaluate each aspect of the mission that is related to sustainability, we want to compute an overall score. Given that all previous scores are already between 0 and 1, we can perform a simple weighted sum to obtain a normalized score. The weights that were used are shown on figure 4.
Figure 4: Weights used for the Mission Sustainability Score. Weights are allocated to the initial objectives and then conveyed to their associated scores (Explicit through matching colors). These weights are defined as such for the project but shall be adapted to stakeholder expectations. Own Figure.
[Results]
CONOPS for End-of-Life strategy:
Figure 5: Concept of Operations for the End-of-Life Strategy of the mission. Real-Options are provided to recognize the uncertainty of this phase of the mission and how flexibility is integrated to ensure compliance with stakeholder expectations. Own Figure.
A 20% margin was added throughout the design sessions in the budget to account for unknown or future changes. This ensures a safety margin up to launch if any changes are to occur during the following design changes.
The composition of each subsystem mass was taken from Space Mission Engineering: The New SMAD to determine the top-down mass budget. Considering the Ariane launcher with capacity of 3500 kg for a TLI and with a Launch Vehicle adapter of 500 kg, the resulting top-down budget was calculated for the 4 spacecraft in total in the following table.
Subsystem | Top-Down [%] | Total Mass [Kg] | Mass for single spacecraft [kg] |
---|---|---|---|
Payload | 35 | 910 | 227.5 |
AOCS | 6 | 156 | 39 |
Structure and mechanisms | 24 | 624 | 156 |
Propulsion (dry) | 7 | 182 | 45.5 |
Power (inc.harness) | 17 | 442 | 110.5 |
Thermal | 4 | 104 | 26 |
CDH | 7 | 182 | 45.5 |
With this composition, the final mass budget was distributed and calculated as per the following table for a single spacecraft.
Subsystem | Mass [kg] |
---|---|
Payload | 100.0 |
AOCS | 37.4 |
Structure and mechanisms | 55.9 |
Propulsion (dry) | 7.6 |
Power (inc.harness) | 92.6 |
Thermal | 2.2 |
CDH | 23.1 |
Dry mass | 318.8 |
Dry mass (20% margin) | 382.6 |
Propellant mass (20% margin) | 72.0 |
Wet mass | 454.6 |
LV Adapter | 500 |
Total Launch mass | 2318 |
As the Ariane 62 supports up to 3500 kg to a TLI, we are well within the available mass with a 33.8% margin.
Risk assessment was made by evaluating each subsystem and finding every failure point. Risks were identified and mitigation strategies were devised in the following table.
Probabilities go from 1 to 5 with 1 being the lowest and 5 being the most probable. Similarly, severity goes from 1 to 5, 1 being the least severe and 5 being the most severe. The risk is then calculated by multiplying both and color-coded to represent the scale of the risk.
Scale for the risk is as follows:
Costs were not taken into account during this study.
This study enabled the preliminary development of 4 satellites to fulfill the customers needs, i.e. to have an efficient object detection in Earth-Moon corridor system to support SSA in cislunar space. It was difficult to have a first draft and get every subsystem started, but once everyone had a better understanding of their goals, rapid iteration was possible. Every subsystem achieves a correct preliminary design, but future iterations shall consider the difference in progress made, as certain subsystems are more detailed than others, and the budget of mass for example differs sometimes a lot between the top-down and bottom-up approaches. A major trade-off made, impacting a lot of subsystems, was the type of propulsion used, mainly based on the trajectory needs. However, the trajectory was only decided using scientific publication and no simulation has been made yet.
A huge and recurrent lesson learned is the importance of good communication, as even with a good team communicating a lot, there were still some misunderstandings.
For general lessons learned about concurrent engineering, go to the useful_tips page (accessible to eSpace staff only).
[To complete during and at the end of the study: add below all technical lessons learned associated with the different disciplines/subsections]
Some technical parameters (or the information to calculate these parameters) were contained in the references provided by the customers to the team.
In this chapter, I want to share the key lessons I learned during the design phase of our satellite mission. Working on such a complex project brings a range of challenges, which provide good opportunities to learn from.
One important lesson I learned is that you should not be afraid to rethink your work, even if you are already several sessions into the project. If, through discussions with other experts (such as during the mid-term presentation) or with your teammates, you come to the conclusion that your current solution is no longer the best one, it’s okay to throw it out and start fresh.
In our case, for example, after many internal discussions, we revisited our decision to use an electric propulsion system and ultimately switched to a chemical one.
Another takeaway is the importance of clean documentation. Calculations, designs, and results should always be well-organized. Especially in a project like this, where many people rely on each other’s work. This is where a software like COMET can help since we only had five sessions. Still, it took some time for me to get confident with the tool.
Next, most of the processes in a complex system design are iterative like the calculation of the fuel mass. You often have to start with a rough estimate that can be far from the final value. But over time, as each subsystem is refined, the maturity of the overall mission increases.
Finally, perhaps the most important lesson I have learned is the importance of good team dynamics. I believe our team worked well together. Open communication, asking questions, taking ownership of your responsibilities, and sharing results quickly are all critical in a project involving many people from different backgrounds. A team that collaborates effectively makes all the difference and can determine the success or failure of a mission.
Tooling and Data Coordination
What I Would Do Differently
If I were to restart the project:
This experience also taught me that while the EPS is critical, its first-order behavior (especially in eclipse-free missions with good Sun exposure) can be addressed effectively without electronic detail, as long as physical and mission-level constraints are respected.
For future missions, it would be valuable to refine the EPS by incorporating more detailed electronic modeling (e.g. regulators, PCDUs, failure modes) and by exploring dynamic power profiles in more complex orbital environments or under stricter mass constraints.
If I had to do this again, here’s how I would do it:
Overall
The mission being a typical “old space” case reduced the challenge of integrating sustainability as a domain of expertise, which was good for a first test. Now that the role has been defined and iterated upon, it would be interesting to test it on a case of New Space (e.g. SATCOM Constellation) with a larger tradespace.
Team
On the team side, an important lesson is that this project is a course, and the students have very different backgrounds. Once a baseline design / set of parameters has been defined, these differences in background start to fade, but in the early design sessions, this creates a real bottleneck. Hence having a robust mitigation plan (e.g. predefined values, given in case of emergency) to make sure that the design’s first iteration does not get too long, or that students do not get stuck in the very early stages would probably allow to go much further in the last sessions (where real improvements arise system-wide).
Software
First Activity Browser was considered to perform the high level life cycle assessment but it had to be abandoned during the project for AI generated data. It was identified that Activity Browser is not adapted for rapid decision making and especially for high level tradeoffs. Hence a lesson that we can define is that a tool for technology choice should be created to enable an efficient and reliable decision. Currently, AI generated tools were effective and showed what kind of tools were needed, but the reliability of the data needs to be assessed.
Central Repository
COMET was hard to use in the context of the sustainability domain and most of the information that was needed was collected via oral interactions. Indeed, information like the selected technologies could not be collected (only values like mass), and other crucial parts like CONOPS were not available on COMET. Hence it would be interesting to explore tools that allow us to share more than simple values (images, diagrams, etc…). The main lesson learned in this case is that human interactions constitute a very important part of the concurrent engineering process and that an active effort should be made toward it.
Process
An important point that could be noted throughout the sessions is that although multiple pieces of information are required to perform some calculations, they do not come at the same time. Hence it is important to plan for these cases and perform educated guesses on possible values that will “fill the gaps” until more information. It is very important because some values come very late in the process and if no output is being produced from the sustainability until then, the impact on the system becomes very reduced. Therefore these “educated guesses” shall be planned in advance rather than on the go, like a risk assessment of the concurrent engineering process.
As a system engineer, it is important to keep an eye on the overall mission and not only look at each subsystem. Communication between subsystems is a key element to systems engineering and getting everyone on the same page with the same information is crucial.
Budgets:
Risk assessment: