Alpbach Summer School 2012 URANUS SYSTEM EXPLORER USE 2/08/2012 GREEN TEAM 1 Mission Summary Study the Uranian system with a focus on the interior, atmosphere and magnetosphere in order to better constrain the solar formation model and to understand how the icy giants formed and evolved. www.planeten.ch We will achieve this with an orbiter and an atmospheric probe. Hubble Space Trelescope / NASA 2 2 ESA Cosmic Vision 2015-2025 What are the conditions for Planet Formation and the Emergence of Life? Observations of Uranus will help to improve existing models of planetary system formation Understand icy giant planets (exoplanets) How does the Solar System Work? What is the structure and dynamics of the icy giants? How do they interact with their space environment? 3 3 Outline [1] Scientific Rationale [2] Baseline design [3] Mission analysis [5] Spacecraft and ground segment design Voyager 2 / NASA [7] Conclusion 4 Basic facts of Uranus URANUS Interior Voyager 2 Magnetosphere Atmosphere One of the 4 giant planets Distance: 19 AU Rotation Period: 17h Orbit Period: 84 years Only visited by Voyager 2 in 1986 Hubble Space Trelescope / NASA 5 5 Atmosphere of Uranus Composition ? Drivers of atmospheric chemistry ? Dynamics (transport of heat) 6 6 Magnetosphere of Uranus Field Intensity @ 1.4 Ru Rotation axis tilt 98° Dipole axis tilt by 59° Large quadrupole moment Voyager 2 Source: Nicholas et al., AGU, 2011 How and where is the intrinsic field generated? A new class of dynamo? 7 7 Magnetosphere of Uranus How does the magnetosphere interact with solar wind? Voyager 2 How is plasma transported in the Uranian magnetosphere? Rotation axis tilt 98° Dipole axis tilt by 59° Large quadrupole moment Is there a significant internal plasma source on Uranus? Insight into Earth’s magnetosphere during magnetic reversals LASP, University of Colorado, Boulder 8 8 Interior of Uranus Rel. low heat flux Molecular H2 Molecular H2 Helium + Ices Inhomogeneous Metallic H Ices mixed with Rocks? Rocks? Uranus Ices + Rocks Core? Jupiter 9 Interior of Uranus Why is the heat flux lower than expected? Implications for the interior Molecular H2 Molecular H2 and thermal evolution of the planet? Rel. low heat flux Helium + Ices Why does Uranus have such a strong intrinsic magnetic field? How do its Ices mixed with characteristics constrainRocks? the interior? Inhomogeneous Metallic H Is there a rocky silicate core? Implications Rocks? for solar system formation? Uranus Ices + Rocks Core? Jupiter 10 Outline [1] Scientific Rationale [2] Baseline design [3] Mission analysis [5] Spacecraft and ground segment design Voyager 2 / NASA [7] Conclusion 11 Mission Payload Orbiter Atmospheric Probe Imaging Camera (CAM) Visible and Infrared Spectrometer (VIR-V & VIR-I) Remote Thermal IR Spectrometer (TIR) UV-Specrtometer (UVS) Microwave Radiometer (MR) Electron and ion spectrometer (EIS) Scalar and Vector Magnetometer (SCM & MAG) In situ Energetic Particle Detector (EPD) Radio and Plasma Wave Instrument (RPWI) Ion composition instrument (ICI) Mass Spectrometer (ASS & GCMS) Nephelometer (NEP) Doppler wind instrument (DWI) Atmosphere Physical Properties Package (AP3) 12 12 Orbiter Payload Imaging camera - New Horizons / Lorri Study the cloud motion and winds of Uranus Range: 0.35 – 0.85 μm ; FOV: 0,29 x 0,29 deg Visible and Infrared Spectrometer - Dawn / VIR Study chemical composition of the atmosphere Range: 0.25 – 1.05 μm ; FOV: 3,67 x 3,67 deg Range: 1.0 – 5.0 μm ; FOV: 0,22 x 0,22 arcmin Thermal IR Spectrometer - Cassini / CIRS Heat flux at different points to constrain models of the interior and thermal evolution Range: 7.67 – 1000 µm ; Spectral Resolution 0.5 – 20/cm UV Spectrometer - New Horizons Morphology and source of Uranus auroral emission Range: 52 – 187 nm ; Spectral Resolution < 3nm ; spatial res < 500 km 13 13 Orbiter Payload Electron and ion spectrometer – Rosetta/EIS Measures electrons and ions Range: 1-22 keV Ion composition instrument – Rosetta / ICA Voyager detections Measure magnetospheric plasma particles in order to study plasma composition and distribution Range: 1eV/e to 22 keV/e ; Resolution: dE/E = 0.04 Energetic Particle Detector - New Horizons / PEPPSI Energetic charged particles that can be used to characterize and locate radiation belts Range: 15 keV – 30 MeV ; energy resolution: 8 keV 14 14 Orbiter Payload Magnetometer - Juno globally measure the magnetic field from low altitude to constrain the dynamics of the field generation layer resolution < 1nT in range of 0.1 – 120000 nT Radio Wave and Plasma Instrument - Cassini Measure plasma waves range: kHz – MHz We resolve the upper hybrid frequency < 1 MHz Microwave Radiometer - Juno / MWR atmospheric and terrestrial radiation, air temperature, total amount of water vapor and total amount of liquid water range: 1.3 – 50 cm High gain antenna Space craft tracking to make gravity field measurements 15 15 Probe Payload Aerosol sampling system / Gas Chromatograph & Mass Spectrometer Galileo sample aerosols during descent and a gas chromatograph and measure heavy elements, noble gas abundances, key isotope ratios range: 1 – 150 amu/e Nephelometer - Galileo studies dust particles in the clouds of Uranus' upper atmosphere Doppler Wind Instrument - Huygens / DWE height profile of Uranus zonal wind velocity resolution: 1 m/s Atmosphere Physical Properties Package - Huygens / HASI measure the physical characteristics of the atmosphere temperature sensor pressure sensor 3 axis accelerometer electric field sensor 16 16 Traceability Matrix - Interior Instrument Intrinsic magnetic field / dynamo Mass distribution in the interior Heat flux MAG TIR RAD What is the origin of the intrinsic magnetic field? Is there secular variation in the Uranian magnetic field? Extent of mass of Si core Are there different layers with different composition, states of matter? Is it uniform / Are there hotspots ? Heat transport mechanisms ? 17 17 Mission Requirements Science Phase I Interior (Gravity) HGA visible from Earth Low altitude Period ~11 days 15 Ru 40 Ru Sun Magnetosphere Globally probe magnetosphere Cross magnetopause 1.5 Ru Atmosphere Global coverage on day- and nightside Occultation 18 25 Mission Requirements Science Phase II and III Interior (Magnetic Field) Global coverage with low altitude Period 4.3 days 10 Ru 20 Ru 1.5-1.05 Ru Interior (Gravity) HGA visible from Earth Low altitude Atmosphere Global coverage on day- and nightside 19 26 Mission requirements Gravity and magnetic field Higher orders can only be resolved at lower altitudes Here: 2.5 Ru for degree 11 Signal decays exponentially with altitude Higher orders decay more efficiently 20 20 Outline [1] Scientific Rationale [2] Baseline design [3] Mission analysis [5] Spacecraft and ground segment design Voyager 2 / NASA [7] Conclusion 21 Outline [1] Scientific Rationale [2] Baseline design [3] Mission analysis [5] Spacecraft and ground segment design Voyager 2 / NASA [7] Conclusion 22 Mission Baseline SCIENCE PHASE CRUISE PHASE Nov 2049 UOI Jun 2033 Earth GA Mar 2030 Venus GA Feb 2031 Earth GA 2029-Oct 2031-Feb 08 Oct 2029 Launch May-Nov 2052 Science phase 3 Mar 2036 Jupiter GA Sep 2049 Probe release Nov 2049- Sep 2050 Science phase 1 2036-Mar May 2051-May 2052 Science phase 2 2052 26 Nov 2052 End of nominal mission 23 23 Launch and Cruise phase 2029 2030 2031 2033 2036 2049 Launch 8 Oct 2029 02:18:41 Ariane 5 launch. 𝑉𝑒𝑠𝑐 = 3.56 km/s (C3=12.67) Total Mass available: 4185.1 kg -> Launch driven by mass maximization. Total time cruise phase: 20.139 years 24 24 Launch and Cruise phase 2029 2030 2031 2033 2036 2049 Launch 8 Oct 2029 02:18:41 Gravity Assist sequence: Venus-Earth-Earth-Jupiter. Total ΔV = 0.21 km/s 5% Margin and 25m/s maintenance for the 5 legs applied. The mission is classified category II (COSPAR Planetary Protection). Total time cruise phase: 20.139 years 25 25 Orbit insertion in Uranus 2029 2030 2031 2033 2036 2049 Orbit insertion in Uranus: 19 Nov 2049 13:33:00 Uranus Orbit Insertion: 19 Nov 2049 with ΔV = 0.60 km/s burn. Velocity at Uranus arrival: 3.36 km/s Final orbit Inclination set to 90° at arrival. 26 26 Probe insertion and descent 2029 2030 2031 2033 2036 2049 • Probe release: Probe released 19 Sep 2049, 2 months before orbit insertion. Release maneuver ΔV = 0.001 km/s burn. • Probe insertion Entry at the atmosphere at 23 km/s. Arrival at latitude of 20 deg. Dayside arrival. • Probe descent 27 27 Probe insertion and descent 0 Probe Entry, t = 0 min Δt ≈ 5 min Pressure (bar) Drogue Parachute Drogue Parachute Release Δt ≈ 2 min Top Cover Removed 0.1 Heat Shield Drops Off 100 Probe Mission Terminates t = 90 min 28 28 Insertion Science Phase Profile 10 months 6 months Science Phase 1 Nov 2049 12 months Science Phase 2 Sep 2050 6 months Science Phase 3 May 2051 May 2052 End of nominal mission Nov 2052 Total science phase duration: 34 months 29 29 Science Phase 1 Orbits 10 months Nov 2049 Sep 2050 125 orbits Highly elliptical polar orbit. Eccentricity 0.93 - Inclination 90 ° Arg. of perigee 280.39 ° Apogee radius 996803.63 km Perigee radius 38338.58 (1.5 Ru) km Period 11.67 days Large apoapsis to sample magnetosphere and cross magnetopause. Low periapsis for gravity field measurements. Dayside/Nightside global coverage. [3] Mission analysis 30 30 Science Phase 2 Orbits 6 months Sep 2050 12 months May 2051 84 orbits May 2052 30 orbits Orbit circularization lowering the apoapsis in 4 steps: 1.40-1.35-1.30-1.25-1.20 Ru 10 orbits at each step, 84 at last orbit. Total ΔV = 0.55 km/s Eccentricity 0.86 - Inclination 90 ° Arg of perigee ° Apogee radius 511215.10 (20 Ru) km Perigee radius 37331.12 (1.05 Ru) km Period 4.34 days Detailed magnetosphere sampling at different Ru. 31 31 6 months Science Phase 3 Orbits May 2052 42 orbits Nov 2052 Highly elliptical polar orbit with low periapsis. Argument of perigee gain of 10 deg. Avoiding dust hazards from the rings. Eccentricity 0.90 - Inclination 90 ° Arg. of perigee 297.176-307.16 ° Apogee radius 510334 (20 Ru) km Perigee radius 26837 (1.05 Ru) km Period 4.51 days Internal gravity field sampling. Enhanced magnetic field sampling. Untargeted Uranian satellites fly-bys. END OF MISSION: deorbiting maneuver at apoapsis of ΔV = 0.04 km/s to deliberately crash the orbiter to Uranus (avoiding satellite contamination). 32 32 Extended mission orbits ? months Nov 2052 ?orbits ?????? Highly elliptical polar orbit with low periapsis. Argument of perigee gain (20 deg per year). Eccentricity 0.90 - Inclination 90 ° Arg. of perigee 297.176-307.16 ° Apogee radius 510334 (20 Ru) km Perigee radius 26837 (1.05 Ru) km Period 4.51 days Enhanced magnetic field sampling. Untargeted Uranian satellites fly-bys. Aerobraking. • END OF MISSION?: Remaining ΔV or aerobraking 33 33 ΔV and fuel budget - Cruise ID Total Mass ΔV [km/s] [kg] Maneuver Used Remaining fuel Fuel [kg] [kg] 1 Initial State 3.56 4185.1 2095.1 2 Venus-Earth DSM 0.04 4093.86 57.80 2003.86 3 Earth-Earth DSM 0.04 4010.78 50.37 1920.78 4 Earth-Jupiter DSM 0.00 3978.74 0.00 1888.74 5 6 Jupiter-Uranus DSM Probe release maneuver 0.00 0.00 3946.95 3607.42 0.00 1856.95 307.99 1517.42 Total ΔV = 0.21 km/s (includes 5% margin and 25m/s maintenance ) 1 2029 2 3 4 2030 2031 2033 5 6 2036 34 2049 34 ΔV and fuel budget – Science Phase ID Maneuver Used fuel [kg] ΔV [km/s] Remaining Total Mass Fuel [kg] [kg] 1 Orbit Insertion 0.6343 664.37 853.05 2943.05 2 Apo 40Ru-35Ru 0.0994 92.37 760.67 2850.67 3 Apo 35Ru-30Ru 0.0603 54.61 706.07 2796.07 4 Apo 30Ru-25Ru 0.0833 73.75 632.31 2722.31 5 Apo 25Ru-20Ru 0.1228 105.15 527.16 2617.16 6 Per 1.5Ru-1.05Ru 0.1875 152.79 374.37 2464.37 7 De-orbit 0.0443 34.79 339.59 2429.59 • Total ΔV = 1.23 km/s Mission total ΔV = 1.44 km/s Insertion Remaining 10 months 6 months ΔV = 0.47 km/s 12 months 6 months 1 2 3 Nov 2049 Sep 2050 4 5 May 2051 6 May 2052 35 7 End of nominal mission Nov 2052 35 Science operations 6 kpbs / Downlink time 25% / Dedicated & normal modes 36 36 Outline [1] Scientific Rationale [2] Baseline design [3] Mission analysis [5] Spacecraft and ground segment design Voyager 2 / NASA [7] Conclusion 37 Payload Configuration Payload panel 1: Remote Sensing Boom: Magnetometers Payload panel 2 and 3 (opposite sides): Plasma package 38 38 Subsystems Configuration ASRGs: 3 ASRGs 90° apart. Back panel: Probe Sides panels: Radiators Low gain antennas 39 39 Launcher Ariane 5 ECA launcher Total launch = 4185 kg Fairing Maximum diameter = 4570 m Maximum height = 15589 mm Adapted from Ariane V user manual Adapted from Ariane V user manual 40 40 Propulsion Main engine: Leros-1b by AMPAC™ (JUNO Heritage) Bipropellant engine: NTO-Hydrazins Specific Impulse = 318 s Nominal Thrust = 645 N Status: Flight Proven Adapted from AMPAC™ website 41 41 Probe layout Probe configuration during cruise phase Elements of the probe: 42 42 Attitude Control The AACS provides accurate dynamic control of the satellite in both rotation and translation. Required Pointing Accuracies angle (degrees) Comms. 0,107 Probe Relay 0,107 Remote Sensing 0,061086524 Pointing Stability (1sec) 0,001396263 Pointing Stability (1h) 0,048869219 Payload • • • • • 4 x Reaction Wheels 4 xThrusters Clusters 2 x Star Trackers 2 x Sun Sensors 3 x MIMU 43 43 Attitude phases: Possible + Z spinning during cruise. It is required to protect sensors, pointing HGA antenna to the Sun. AACS is automated with coarse Sun sensors. 3-axis stability when approaching with RWA, compensation the realease of the proabe with thrusters; During nominal phase, 3-axis attitude control is done with reaction wheels. The largest reaction torque is 0.13 Nm. Angular momenta less than 34 Nms (approx.: 2000 rpm); fast maneuvers or accelerations must be achieved with less precise but faster thrusters (RCS); Inertia Tensors calculated before and after probe releasing. In both cases the values are inferior to those in Cassini which uses the same actuators. Sensors' Resolution IRU - uncalibrated < 0.5 deg/h IRU - calibrated < 0.05 deg/h Sun Sensors < 0.01 deg Star Trackers < 0.001 deg Achievable Pointing Accuracies - angle (degrees) Attitude Typical Accuracy Maneuverability Thrusters RWA Spinning 0,2 Fast, least accurate 0,01 Slow, very accurate from new horizons 0,027 heritage 44 44 Q & A – Inertia Calculations -> 1 N thrusters -> 0.13 Nm Inertia Matrix w/ Probe Ix 5458,0 Kg.m2 Iy 4828,7 Kg.m2 Iz 1590,4 Kg.m2 Good maneuverability ! Inertia Matrix w/o Probe Ix 3137,8 Kg.m2 Iy 2203,6 Kg.m2 Iz 1285,5 Kg.m2 Change in the CM 45 45 Communication Overview HGA for Orbiter-Earth communications Ka-band downlink (35 GHz) X-band uplink (7.2 GHz) MGA for Orbiter-Earth communications near Venus X-band downlink (8.1 GHz) X-band uplink (7.2 GHz) LGA for LEOPS S-band downlink (2.2 GHz) S-band uplink (2.1 GHz) UHF for Probe-Orbiter communications UHF (400/420 MHz) dual uplink 46 High Gain Antenna 4m Cassini-derived HGA HGA for Earth comms to ESTRACK 35m network. Ka Band downlink (35GHz) X-band uplink (7.2Ghz) Ultrastable oscillator (HGA used for radio science) 47 High gain antenna link budget HGA Downlink Uplink Waveband Ka (35 GHz) X (7.2 GHz) Transmitter power 20 dBW (100 W) - Transmitter line Loss -0.458 dB Antenna pointing Loss -1.33 dB Transmission losses -315 dB -301 dB EIRP 80.3 dBW 92 dBW Receiver G/T 62.8 dBi/K 23.1 dBi/K Carrier-to-noise C/N0 55.2 dB Hz 42.3 dB Hz Coding BPSK/RS Viterbi DPSK Required Eb/N0 2.7 dB 12 dB Data rate 6 kbps 70 bps Implementation loss -2 dB -2 dB Rain attenuation -3 dB -10 dB Link margin 3.17 dB (>3 dB) 6.04 dB (>6 dB) 48 Medium Gain Antenna Medium gain antenna for communications with orbiter near Venus when HGA used as sun shield. Communications over Xband with Kourou. 0.8m diameter steerable antenna. Rosetta heritage. MGA 49 ESA Medium gain antenna link budget MGA Downlink Uplink Waveband X (8.1 GHz) X (7.2 GHz) Transmitter power 20 dBW (50 W) - Transmitter line Loss -0.458 dB - Antenna pointing Loss -0.286 dB - Transmission losses -281 dB -301 dB EIRP 50.6 dBW 92 dBW Receiver G/T 41.0 dBi/K 9.14 dBi/K Carrier-to-noise C/N0 39.3 dB Hz 38.6 dB Hz Coding BPSK/RS Viterbi DPSK Required Eb/N0 2.7 dB 12 dB Data rate 500 bps 30 bps Implementation loss -2 dB -2 dB Rain attenuation -3 dB -3 dB Link margin 3.81 dB (>3 dB) 6.03 dB (>6 dB) 50 Low Gain Antenna Low gain antenna for communications during NEOP. LGA Communications over LGA S-band with Kourou. Low mass and power patch antenna. 51 Low gain antenna link budget LGA Downlink Uplink Waveband S (2.2 GHz) S (2.1 GHz) Transmitter power 10 W - Transmitter Antenna Losses -0.458 dB Antenna pointing Loss -19.8 dB Transmission losses -197.3 dB -197 dB EIRP 14.4 dBW 74.7 dBW Receiver G/T 29.1 dBi/K -19.6 dBi/K Carrier-to-noise C/N0 55.0 dB Hz 86.6 dB Hz Coding BPSK/RS Viterbi DPSK Required Eb/N0 2.7 dB 12 dB Data rate 500 bps 500 bps Implementation loss -2 dB -2 dB Rain attenuation -3 dB -3 dB Link margin 19.5 dB (>3 dB) 41.8 dB (>6 dB) 52 Probe UHF link budget LGA Uplink #1 (Coast) Uplink #1 (100 bar) Waveband UHF (400 MHz) UHF (400 MHz) Antenna Patch LGA on Aeroshell Quad helix on Probe Transmitter power 10 W 150W Transmitter line loss -0.45 dB -0.45 dB Antenna pointing Loss -11.81dB -9.33dB Transmission losses -182 dB -197 dB EIRP 24.18 dB 21.89 dB Receiver G/T -3.55 dB -3.55 dB Carrier-to-noise C/N0 40.57 dB 40.70 dB Coding BPSK/RS Viterbi BPSK/RS Viterbi Required Eb/N0 2.7 dB 2.7 dB Data rate 2.25 kbps 2.32 kbps Implementation loss -3 dB -3 dB Atmospheric attenuation 0 dB -15 dB Link margin 2.7 dB 2.7 dB 53 53 Unit mass [kg] Qty Mass (CBE) [kg] DMM Mass (CBE+DMM) [kg] HGA 100 1 100 5% 105 X/Ka band Rx/Tx 5.05 2 10.1 20% (average) 11.8 MGA 10.4 1 10.4 30% 13.6 X band transponder /filters 5.3 2 10.6 10% 11.7 LGA 0.08 2 0.16 20% 0.19 S-band transponder 2.6 2 5.2 10% 5.72 2 3.704 10% 4.07 Communications system mass UHF receiver 1.852 Total 152 kg 54 Communications system power budget DMM Uplink (CBE) [W] Uplink (CBE+DMM) [W] Downlink (CBE) [W] Downlink (CBE+DMM) [W] High gain (averages) 20% 25 32.5 140 158 Medium gain 10% 20 22 50 55 Low gain 10% 5 5.5 20 22 Probe UHF 10% 6 6.6 0 0 Uplink power consumption scaled from downlink using typical numbers from SMAD. Probe UHF system values are from Mars Odessey. Power consumption for TWTA (40W) comes from WFI CDF study report. 55 Command & Data Handling GNC and CDH Flight computers redundant Mass storage: Two High Speed Solid State Data recorders 4 Gbyte (4x1 Gbyte DRAM) Redundant storage – recorders operate in parallel Primary data bus (MIL-1553) Spacewire to high data rate instruments (ORS), SSDRs and communications system. 56 Ground Segment ESTRACK MOC 35-m antennas Mission Operation Center 15-m antenna for LEO SOC Science Operation Center PGS Probe Ground Segment MOC monitoring and control of the complete mission generation and provision of the complete raw-data sets SOC scientific mission planning support creation of pre-processed scientific data PGS supports operations of the Probe coordinates scientific mission planning 57 57 Radiometric Tracking Meas. Type Precision Tracking schedule range-rate ~0.1mm/s cruise once per week range ~1m ang. pos. (VLBI) ~0.03mas1 (s/c) ~2.43mas2 (probe) some months before UOI until end of science phase once per day at pericenter passage probe descent continuous 10.03mas translates to 0.4 km at the mean distance of Uranus (35GHz freq.) 22.43mas translates to 34 km at the mean distance of Uranus (400MHz freq.) POD during science phase: ranges, range-rates Position accuracy of the s/c in the cruise phase: 10-20km science phase: km range VLBI can be used to improve Uranus’ ephemeris Position accuracy of the probe: 34km 58 58 Thermal control – Hot case Venus Solar backscattering from Venus (but high altitude) 2649.7 W/m² 178.4*(Rv/Rorbit)² payload panel Antenna towards sun for critical hot case Avoid payload panel towards Venus Radiators top, bottom or towards zenith ARSGs shadowed by antenna 59 59 Thermal control – Cold case 0.55*(Rv/Rorbit)² Uranus Eclipse 158W electrical power for payload (assume 10% dissipation) Critical => heat load needed for cold case for balance Possibility to use ASRG waste heat load in addition to decrease need of heaters (15W for New Horizons) Heat pipes for better transport to critical components (tanks, batteries) Classic solution: louvers VCHP? Heat switch? 60 60 Thermal control -Radiator α/ε << Teflon aluminized Teflon silvered OSR -Cryo-radiator for IR payload -Louvers Batteries MLI HGA α/ε << Teflon aluminized Teflon silvered OSR IR payload Payload MLI+Conductive insulation Tanks MLI ASRG Eff=28%, EOL electrical power=130W Heat load dissipated~334W Outer S/C cover MLI betacloth outer layer 61 61 Power budget We plan to use ASRGs (Am241, 27.8kg, 140W BOL, 130W EOL). Scaled from the Nasa plutonium ARSRGs, taking into account the lower activity level of Am241 (requires 5x more radioactive material). 20% margin applied. w/o margin w margin BUS (W) 129.5 142.9 PAYLOAD (W) 152.9 166.4 TOTAL (W) 282.4 309.30 390 312 3xASGs EOL (W) Assumption: peak load (without COMM subsystem) 62 62 Power budget: science orbit Occultation science ~158W COMM 63 63 Mass budget 13% 8% (kg) Total dry mass (excl. adaptator) With 20% system margin Propellant needed until after orbit insertion Propellant needed for attitude control Propellant needed for science orbit Total wet mass (excl. adaptator) Adaptator (incl. separation mechanism) Total CBE+DMM 2,115 62% 935 S/C BUS 158 S/C ORBITER PAYLOAD S/C BUS S/C ORBITER PAYLOAD 791 S/C PROBE 19% 31% S/C PROBE 4% S/C PROPELLANT (until insertion) 3,999 186 4185 S/C PROPELLANT (AOCS) 22% 4% 7% MASS MARGIN Launch capability = 4185kg 64 64 Risk management [5] Spacecraft design 65 65 Critical items Critical items Uranus rings plane hazards Thermal design (heat load variation) Probe (TPS, trajectory) Structure (FEA) [5] Spacecraft design 66 66 Development Timeline 67 Cost estimation Description M€ Sub-Total M€ % Launcher 175 175 9 1.450 74 230 12 100 100 5 Total 1.955 100 Main S/C Probe Operations PF 1.250 PL 200 PF 200 PL 30 68 Summary USE is equipped with sufficient instruments to carry out sufficient measurements to answer the scientific questions mass, power and cost budget allow the mission to be feasible technologies proposed use heritage from previous space missions and can be easily implemented for future space missions 69 Thank you! & USE IT! 70 70 Backup: Command & Data Handling GNC and CDH Flight computers: Leon3FT, 89 MIPS Secondary GNC/CDH computers Hardware watchdog timer based redundancy If Primary computer does not reset the timer, backups are brought online. Mass storage: Two High Speed Solid State Data recorders (derived from LRO-SSDR) 4 Gbyte (4x1 Gbyte DRAM) Redundant storage – recorders operate in parallel Primary data bus (MIL-1553) Spacewire to high data rate instruments (ORS), SSDRs and communications system. 71 Backup: Probe Mass Budget 72 72 Backup: Cruise phase science Take measurements of Venus and Jupiter during successive fly bys. Calibration of instruments during Earth fly-bys. During the Venus fly-by use the ‘Energetic Particle Detector’ and the ‘Radio and Plasma wave instrument’, to measure the interaction of Venus with the solar wind. During Jupiter flyby, we can use the newer instrumentation to obtain more, accurate, results then previous flybys. During the two flyby’s of Earth, the obiter's systems can be calibrated. Instruments shall be calibrated every year and engines tested. 73 Backing: Calibrating instruments Using the Earth to calibrate the obiters instruments means that we can rely on ground based observations as well as satellite. This would lower error margins, and help to signify any problems the instruments may be having Orbiting the Earth twice will allow ground operations to check twice the working order of the instruments. Calibrating the magnetometer: as satellite passes through Earths Magnetic field, the reading it samples can be compared to the known value for the Earths magnetic field and the instruments can be calculated accordingly 74 Backup: Calibrating instruments Other instruments that rely on the interaction of the Earth’s magnetic field can be calibrated using the orbiting satellites and taking measurements around the earth. For example the ‘Energetic Particle Detector’ and the ‘Electron and Ion Spectrometer’ can be calculated using the current orbiting satellite’s data. Other instruments such as the imaging camera and visible and infrared Spectrometer need to take images of certain sections of the Earth of which the wavelengths are known. Using those previously obtained values and comparing our results, to see if they fall within the acceptable range, we can determine if and by how much the instruments need calibrating. Since Earth sends out a large number of radio waves, we can use these known radio waves to calibrate our radio instruments. 75 Backup: Planetary protection All mission is of Category II : Type of Mission Planet Category Flyby Venus II Jupiter* II Orbiter Uranus II Probe Uranus II * Case of Europa Category II: All types of missions to target bodies where there is significant interest relative to the process chemical evolution and the origin of life, but where there is only a remote chance that contamination carried by a spacecraft could compromise future investigations. 76 Backup: Planetary protection 77 Backup: Thermal control (hot case) Venus Solar backscattering from Venus (but high altitude) 2649.7 W/m² 178.4*(Rv/Rorbit)² payload panel HGA: α=0.1; ε=0.8; A=14,3 m² (teflon aluminized) Payload panel: α=0.5; ε=0.5; A=3.7*1.7 m² Side panels+Back panel: α=0.4; ε=0.9; A=3.7*1.7 m² (betacloth) Radiators not considered No critical power consumption for this case 78 78 Backup: Thermal control (hot case) Venus Solar backscattering from Venus (but high altitude) 2649.7 W/m² 178.4*(Rv/Rorbit)² payload panel 1 node S/C α_antenna*Qsun*A_antenna + εside*Qir*Aside + Qdiss= σ*ε_antenna*A_antenna*T^4 +σ*ε_payload_panel*A_payload_panel*T^4 +3*σ*ε_panel*A_panel*T^4 +σ*ε_bottom_panel*A_bottom_panel*T^4 (neglecting exchanges with area between antenna and top panel) (neglecting VF of the other panels than probe panel) 79 79 Backup: Thermal control (cold case) 0.55*(Rv/Rorbit)² Uranus Eclipse 158W electrical power for payload (assume 10% dissipation) ε_payload_panel*A_payload_panel*Qir + Qdiss= 4*σ*ε_panel*A_panel*T^4 +σ*ε_bottom_panel*A_bottom_panel*T^4 + σ*ε_antenna*A_antenna*T^4 (neglecting exchanges with area between antenna and top panel) (neglecting VF of the other panels than probe panel) 80 80 Backup: Thermal control (cold case) T° IR instrument Cryo-radiator ε_payload*A_aperture*Qir + Qdiss= σ*ε_payload*A_internal_surfaces*T^4 +GL*(T^4-T_cryo_radiator) GL*(T^4-T_cryo_radiator) = σ*ε_cryo_radiator*A_cryo_radiator*T_cryo_radiator^4 81 81