Satellite Subsystems —  Study Notes

ECE 521E — Radar & Satellite Engineering
School of Engineering, Masinde Muliro University of Science and Technology (MMUST)
5th Year Undergraduate · Electrical & Communication Engineering

Full Lecture-Style Notes · Bus & Payload · With Worked Examples

Section 1

1. Overview of a Satellite System

1.1 The Two Halves of Every Satellite

Any satellite, whether a 1U CubeSat or a 6-tonne GEO communications spacecraft, divides into two functional halves:

Design principle

The payload is designed first (mission requirements → payload sizing), and the bus is then sized to carry and support the payload. Bus mass and power typically scale with payload mass and power through simple fractions: on GEO comsats the bus is roughly 25–40% of launch mass; power subsystem mass ≈ 2.5–4 kg per 100 W of generated power.

1.2 Classification of Satellites

ClassOrbit altitudePeriodTypical missions
LEO (Low Earth Orbit)300 – 1,500 km~90 – 110 minEarth observation, SAR, ISS, imaging, CubeSats, LEO broadband constellations
MEO (Medium Earth Orbit)~8,000 – 20,000 km~6 – 12 hGPS/GNSS (20,200 km), navigation
GEO (Geostationary)35,786 km (equatorial)23 h 56 min (sideral)Fixed comms, weather imaging, broadcast
HEO / ellipticalperigee ~500 km, apogee ~40,000 kmvaries (e.g., 12 h Molniya)High-latitude communications (Molniya), early-warning
Sun-synchronous LEO~600 – 800 km, retrograde, i ≈ 98°~100 minMapping, radar altimetry — constant local solar time (e.g., 10:30 AM descending node)

1.3 The Subsystem Map

Standard satellite engineering recognizes these bus subsystems:

  1. Mechanical structure and mechanisms
  2. Attitude Determination and Control Subsystem (ADCS)
  3. Propulsion subsystem
  4. Electrical Power Subsystem (EPS)
  5. Thermal Control Subsystem (TCS)
  6. Telemetry, Tracking and Command (TT&C)
  7. Command and Data Handling (C&DH)
  8. Payload(s) with their dedicated antennas/sensors

Sections 2–8 treat the bus subsystems in detail; Sections 9–10 treat communication and radar payloads; Section 11 covers reliability engineering; Section 12 the ground segment.

1.4 The Space Environment (Why Subsystems Exist)

Section 2

2. Mechanical Structure and Mechanisms

2.1 Functions

2.2 Construction

Mechanism design rule: mechanisms are among the highest-risk items (they must work exactly once, after months in space). Design practice demands redundancy of release initiators, generous margins, ground testing in vacuum/thermal-vacuum, and where possible "test as you fly" on the flight unit.

Section 3

3. Attitude Determination and Control Subsystem (ADCS)

3.1 Mission of the ADCS

The ADCS keeps the satellite pointed (attitude control) and knows where it is pointing (attitude determination). Typical pointing requirements:

MissionPointing accuracyStability
GEO comsat antenna beam±0.05° – 0.1°0.001–0.005 °/s
Earth-imaging camera±0.01° – 0.1°very low jitter
SAR antenna±0.1° – 0.5°attitude knowledge drives image registration
Space telescope (e.g., JWST)milli-arcsecondsextreme stability
CubeSat (basic)±1° – 5°modest

3.2 Attitude Determination Sensors

SensorPrincipleAccuracyNotes
Earth horizon sensors (IR)Earth IR limb at 14–16 µm0.1° – 1°LEO standard; fails beyond GEO distance
Sun sensorsPhotodiode fine/course heads0.01° – 1°Cheap, robust; ambiguous axis along Sun line
Star trackersImage star field, pattern matcharcsecondsBest accuracy; occultation by Sun/Earth/Moon; radiation upsets
MagnetometersMeasure local B field0.5° – 2°Needs accurate field model (IGRF); LEO only (strong field)
Gyroscopes (rate sensors)Momentum / optical (FOG, RLGs)rate: 0.001°/h – 1°/h driftPropagate attitude between fixes; MEMS for CubeSats
GPS receiverCarrier phase / codeposition m-level; attitude with multi-antennaLEO mainly; increasingly used for orbit determination

Standard practice: gyros propagate the attitude between absolute fixes (star tracker / Earth sensor / Sun sensor) — a complementary filter (Kalman filter) merges them, estimating gyro bias.

3.3 Attitude Control Actuators

ActuatorPrincipleTypical torqueUse
Reaction wheelsExchange momentum with body (wheel accelerates)0.01 – 5 N·mPrecision 3-axis control; limited by wheel saturation
Momentum wheelsSpin at biased speed for stiffness (gyroscopic)as reaction wheelsDual-spin GEO comsats, pitch momentum bias
Control Moment Gyros (CMGs)Gimballed spinning wheel redirects momentum50 – 500+ N·m per unitAgile large spacecraft (ISS, imaging sats)
Magnetic torquers (torque rods)Coil interacts with Earth's B field: τ = m × B0.001 – 1 N·mLEO momentum dumping, desaturation; no propellant
Thrusters (cold gas / chemical)Jet momentum0.01 – 20 NLarge slews, orbit corrections, wheel desaturation
Gravity-gradient boomTidal torque aligns long axis with nadirpassiveSimple LEO sats; accuracy ~1–5°

3.4 Control Modes and Disturbance Torques

Typical control modes: detumble after separation → acquisition (Sun, Earth) → nominal pointing → manoeuvre → safe mode (Sun-pointing, minimal activity, awaiting ground command).

Disturbance torques to be rejected (LEO example magnitudes for a 1 m³, 100 kg satellite at 500 km):

Torque sourceOrder of magnitudeCharacter
Gravity gradient10⁻⁵ – 10⁻³ N·mRestoring; used passively
Aerodynamic drag (VLEO)10⁻⁵ – 10⁻³ N·mPeaks at low perigee; variable
Solar radiation pressure10⁻⁷ – 10⁻⁵ N·mSteady; large for high area/mass
Magnetic residual dipole10⁻⁶ – 10⁻⁴ N·mInteracts with B field
Micrometeorite impactsimpulsive, rare~10⁻⁸ N·m average

3.5 Momentum Budget and Desaturation

Wheels absorb cyclic disturbance momentum (gravity-gradient, magnetic residuals) but secular disturbance (solar pressure on an asymmetric body) accumulates until wheels saturate. The momentum capacity needed over time T:

Hreq ≥ Tmax · T (worst-case disturbance torque × duration)

Desaturation ("unloading") options: magnetic torquers in LEO (τ = m × B with dipole m aligned to oppose wheel momentum), or thruster pairs. GEO spacecraft unload with thrusters every few days; LEO CubeSats use torque rods continuously.

Exam favourite: A reaction wheel can only exchange momentum — it cannot change the spacecraft's total angular momentum. External torques (thrusters, magnetic, gravity gradient) are mandatory for secular momentum management.

Section 4

4. Propulsion Subsystem

4.1 Functions of On-Board Propulsion

  1. Orbit acquisition: apogee/perigee raising, plane change (LEO→GEO GTO apogee burns; inclination change is famously expensive: Δv ≈ v·Δi for small angles).
  2. Orbit maintenance / station-keeping: GEO E-W (luni-solar ~1–2 m/s per year) and N-S (~40–55 m/s per year, i.e., inclination drift) corrections; LEO drag makeup (VLEO: up to 10+ m/s/day); constellation phasing.
  3. Attitude control: reaction control thrusters, momentum unloading.
  4. End-of-life disposal: GEO re-orbit to graveyard (+300 km, typically 3–11 m/s depending on area/mass); LEO passivation/de-orbit within 25 years (guideline).
  5. Collision avoidance: conjunction screening manoeuvres.

4.2 Thruster Types

TypePropellant / principleIsp (s)ThrustUse
Cold gasN₂, Ar, CO₂ stored pressurized50 – 75mN – NSimple RCS, CubeSats
Solid (Vernier)Once-only, e.g., apogee kick stage280 – 300kNAKM for GEO insertion
Monopropellant hydrazineN₂H₄ over catalyst bed220 – 2350.5 N – 22 N (0.9 lbf class)Workhorse station-keeping/RCS
Bipropellant (MMH/NTO)Hypergolic ignite on contact300 – 32510 N – 450 NApogee engines (490 N), larger manoeuvres
Electrothermal/resistojetHeated propellant300 – 350mNSmall Δv, long life
Electric propulsionHall thrusters, ion (gridded), PPT1,500 – 4,000+mN – 0.5 NHigh-Δv missions, orbit raising (all-electric GEO), station-keeping

4.3 The Rocket Equation (Tsiolkovsky)

Δv = g₀ · Isp · ln(m₀ / mf) = g₀ Isp · ln(1 + mp/mf)g₀ = 9.81 m/s²; m₀ = initial mass; mf = final (dry) mass; mp = propellant mass

Solving for propellant fraction:

mp/m₀ = 1 − exp(−Δv / (g₀ Isp))

Example: station-keeping a GEO comsat for 15 years needs Δv ≈ 550 m/s north-south + east-west. With Isp = 220 s (hydrazine): mp/m₀ = 1 − exp(−550/2158) ≈ 0.226 — nearly a quarter of launch mass is propellant. With Isp = 3000 s (electric): mp/m₀ = 1 − exp(−550/29,430) ≈ 0.019 — ~2% of mass. This single comparison explains the modern shift to electric orbit raising and station-keeping.

4.4 Propellant Storage and Feed

Section 5

5. Electrical Power Subsystem (EPS)

5.1 Architecture

The EPS generates, stores, regulates, and distributes electrical power:

  1. Generation: photovoltaic solar arrays (essentially universal for Earth-orbit satellites).
  2. Storage: rechargeable batteries for eclipse and peak loads.
  3. Power conditioning: regulation to unregulated or regulated bus voltages (28 V, 50 V, 100 V class), MPPT or direct-energy transfer, battery charge control.
  4. Distribution: switchgear, fusing, load shedding, power telemetry.

5.2 Solar Array Sizing

Solar cell efficiency (modern triple-junction GaInP/GaAs/Ge cells ≈ 29–32% BOL, degrading ~2–3% absolute over 15 years in GEO). Array power at beginning of life (BOL):

PBOL = Psun · ηcell · A · cos θ · KtempPsun ≈ 1361 W/m² solar constant; A = cell area; θ = Sun incidence angle; Ktemp ≈ 0.9 (temperature derating)

End-of-life (EOL) power after radiation degradation and contamination: PEOL = PBOL · (1 − d)N with yearly degradation d (0.5–1%/yr typical for triple-junction, more for Si). Arrays are sized for EOL conditions at worst Sun angle.

Array sizing example

A LEO satellite needs 500 W EOL at 600 km. Cells: η = 30%, degradation 1%/yr over 5 yr, worst-case Sun angle 23° off-normal (cos = 0.92), temp derate 0.9, packing factor 0.9.
PEOL = 1361 × 0.30 × A × 0.92 × 0.9 × 0.9 × (0.99)⁵ = 1361 × 0.30 × A × 0.92 × 0.9 × 0.9 × 0.951
Required: A = 500 / (1361×0.30×0.92×0.9×0.9×0.951) = 500 / 289 ≈ 1.73 m² of cell area — roughly 2 m² with engineering margin.

5.3 Batteries and Eclipse Design

C&DH link: the EPS is managed by the power control unit under C&H software commands: array pointing (if articulated), battery charge modes, load shedding priorities (payload first to shed, survival heaters last).

Section 6

6. Thermal Control Subsystem (TCS)

6.1 The Governing Physics

In vacuum the only heat transfer modes are conduction (within structure) and radiation (to space). Steady-state balance for each node:

α·S·Aproj + ε·σSB·A·Tenv⁴ + Qint = ε·σSB·A·T⁴ + Qcondα = solar absorptivity; ε = infrared emissivity; σSB = 5.67×10⁻⁸ W/m²K⁴; Qint = internal dissipation

Design targets are typically −10 °C to +50 °C for electronics, ~0–40 °C for batteries, and cryogenic or tightly stable temperatures for some sensors. The ratio α/ε is the master thermal design variable: low α/ε (white paint, optical solar reflectors) keeps equipment cool; high α/ε (black paint) keeps it warm.

6.2 Passive Thermal Control

6.3 Active Thermal Control

Typical sizing calculation: a 300 W internal dissipation rejected from a 2 m² radiator at ε = 0.85 toward 3 K space: T = [300/(0.85×5.67e-8×2) + 3⁴]^¼ ≈ [3.11e9]^¼ ≈ 237 K (−36 °C) — comfortable margin above freezing for most electronics; add heater power for eclipse cold-soak cases.

Section 7

7. Telemetry, Tracking, and Command (TT&C)

7.1 The Three Functions

7.2 Frequencies and Link Budget

BandUplink (MHz)Downlink (MHz)Notes
VHF148 – 150137 – 138CubeSats, beacons; congested
UHF435 – 438400 – 402CubeSat command; AIS/ARGOS
L1,631.5 – 1,626.5 (LEO)1,525 – 1,559Mobile sat, GNSS; GPS L1 1575.42
S2,025 – 2,1202,200 – 2,290TT&C workhorse, NASA/ESA deep space (DSN S-band)
X7,145 – 7,2358,400 – 8,500Deep-space uplink/downlink; SAR payloads
Ku14.0 – 14.510.7 – 12.75FSS/VSAT; DTH broadcast downlink
Ka27.5 – 3117.7 – 21.2High-throughput beams, gateway links

7.3 Transponder (Bent-Pipe) Architecture

1RF front end: antenna (often a low-gain hemispherical/omni for TT&C plus medium-gain horn) → diplexer → low-noise amplifier (LNA) → down-converter (mixer + local oscillator).
2Channelization: input demultiplexer (IMUX) filter bank splits the wide receive band into transponder channels (36 MHz or 72 MHz typical for GEO comsats); each channel has automatic gain control and a linearized (TWTA or SSPA) high-power amplifier.
3Output: output multiplexer (OMUX) combines channels → high-power amplifier (HPA) → output filter (to suppress harmonics/out-of-band emissions) → transmit antenna via diplexer.

Regenerative (processing) transponders demodulate on board and re-modulate — enabling on-board switching (SS/TDMA), beam routing, and interference isolation at the cost of complexity.

7.4 Tracking Measurements

Section 8

8. Command and Data Handling (C&DH)

8.1 Role

The C&DH subsystem is the spacecraft's brain: it receives and validates commands, executes them autonomously, collects and formats telemetry, manages the onboard computer (OBC), mass memory, and the data buses, and implements autonomy (safe modes, fault detection, isolation and recovery — FDIR).

8.2 Typical Architecture

8.3 Telemetry and Command Standards

FDIR hierarchy: Level 1 — hardware watchdog and component retries; Level 2 — autonomous reconfiguration to redundant units (cross-strapping); Level 3 — safe mode (Sun acquisition, spinning or 3-axis, minimal power, await ground). Every fault path must be testable on the ground.

Section 9

9. Communication Payloads in Detail

9.1 Payload Elements

9.2 The Satellite Link Budget

The payload performance is expressed through EIRP (uplink: satellite receive G/T; downlink: satellite EIRP):

(C/N₀)downlink = EIRPsat − Lfs − Latm − Lpointing + (G/T)ground − k (all in dB)EIRP = Pt + Gt (dBW + dBi); Lfs = 92.45 + 20log f(GHz) + 20log R(km); k = −228.6 dBW/K/Hz

Overall link quality combines uplink, downlink, and intermodulation/interference:

(C/N₀)total−1 = (C/N₀)up−1 + (C/N₀)down−1 + (C/N₀)IM−1 + (C/I)−1 (powers in linear units)

Required C/N₀ from BER: e.g., QPSK with BER 10⁻⁵ needs Eb/N₀ ≈ 9.6 dB; C/N₀ = Eb/N₀ + 10log Rb. Add coding gain (Turbo/LDPC ≈ 5–7 dB at BER 10⁻⁵) and implementation margin (1–2 dB).

9.3 Multiple Access

TechniquePrincipleExample
FDMAChannels by frequencyClassic C-band transponders
TDMASlots in time, burst carriersIntelsat business service (120 Mbit/s)
CDMASpread codesGPS (CDMA), some LEO constellations
SDMASpatial beamsHTS spot-beam frequency reuse (4-color reuse)

Frequency reuse multiplies capacity: spot beams with orthogonal polarization/frequency reuse factor 4–8 give total throughput = per-beam throughput × reuse factor (beam isolation > ~16–20 dB required to keep C/I acceptable).

Section 10

10. Radar and Earth-Observation Payloads

10.1 Why Radar Payloads

Microwave radar provides day/night, all-weather imaging (cloud-penetrating at L/C-band), precision ranging (altimetry), and wide-swath ocean/ice monitoring — complementing passive optical sensors. Spaceborne radar must live within tight mass, power, and data-rate budgets; hence the heavy use of SAR (synthetic aperture radar) to achieve fine azimuth resolution without a physically long antenna.

10.2 Synthetic Aperture Radar (SAR) Payload

Key relationships

Azimuth resolution: δaz ≈ L/2 (independent of range — the SAR advantage)L = physical antenna length along track
Range resolution: δr = c / (2B·sin γ)B = chirp bandwidth; γ = incidence angle; pulse compression (chirp) achieves metres with μs pulses
Peak power need: Pt via the radar equation (two-way) with σ = σ⁰·δrδaz·(resolution cell)σ⁰ = normalized backscatter coefficient

Payload subsystems

  • RF front end: chirp generator (digital, DDS), up-conversion to L/C/X/Ku band, TWTA or GaN SSPA (hundreds of watts to a few kW peak, duty cycle 5–20%).
  • Antenna: planar phased array (active TR modules — e.g., TerraSAR-X: 384 T/R modules, X-band, 300 km swath StripMap), or reflector-fed for altimetry.
  • Receiver/data: low-noise receiver, ADC at IF/baseband, real-time raw-data buffering (multi-Gbit/s), onboard range compression sometimes, solid-state recorder for 100–1,000 km scenes.
  • Duty/power: SAR is power-hungry (1–4 kW payload power) — scheduling and thermal design must average over the orbit duty cycle.

Modes: StripMap (fixed pointing), ScanSAR (steered elevation bursts for wide swath, coarser azimuth), Spotlight (steered to dwell on target — sub-metre to decimetre resolution, e.g., ~25 cm commercial products).

10.3 Other Radar Payloads

PayloadPrincipleApplication
Radar altimeterNadir pulse timing: h = cτ/2; 1–2 cm precision with tracking gatesOcean topography (Jason/TOPEX), ice-sheet elevation
ScatterometerNormalized σ⁰ vs incidence angle at multiple azimuthsSea-surface wind speed/direction (ASCAT, QuikSCAT)
Cloud/rain radarW/Ka-band profiling of reflectivityCloudSat (94 GHz Cloud Profiling Radar), GPM DPR
GNSS reflectometryBistatic use of L1/L5 signals reflected off Earth's surfaceSoil moisture, ocean winds (CYGNSS)
Link to ECE 521E radar equation material: the SAR/altimeter sizing problems are direct applications of the two-way radar equation — received power ∝ R⁻⁴ forces kW-class peak powers, pulse compression for average-power reduction, and large antennas (T/R module count) for gain — the same trade-offs studied in the radar-equation notes.

Section 11

11. Reliability, Redundancy, and Parts Engineering

11.1 Quantitative Reliability

R(t) = exp(−λt)constant failure rate λ; reliability function (fraction surviving)
Ps(t) = Σ over redundant chains; for two parallel identical units: Ps = 1 − (1 − R)²

Mission requirement drives design: a GEO comsat needing 0.9 probability of 15-year life with inherently ~0.7 reliability demands redundancy in every long-life chain (TWTAs ×2 with loop/backup switching, receivers, computers, gyros ×4 in 2×2).

11.2 Redundancy Strategies

StrategyDescriptionPenalty
Cold (standby) spareSpare unpowered until neededSlower switchover; dormant-failure risk
Warm/hot redundancySpare powered, tracking, instant switchPower/mass; cross-strapping complexity
Cross-strappingAny unit to any function via switch matrixRelays/switches add their own failures
N-of-M votingMajority logic (e.g., 2-of-3 gyros)Extra mass; voter must be ultra-reliable

11.3 Parts, Materials, and Processes (PM&P)

Section 12

12. Ground Segment and Operations

12.1 Elements

12.2 Contact Geometry (LEO)

Pass duration and elevation determine link time: a 600 km orbit with a 5° minimum elevation gives ~8–10 min contacts and 2–4 passes/day from a single mid-latitude station; global coverage needs a relay constellation or multiple ground stations.

Max slant range at elevation E: Rmax = √( (Re+h)² − (Recos E)² ) − Re sin ERe = 6371 km; h = altitude; at E = 0°, Rmax ≈ √(2Reh) for small h

Section 13

13. Worked Design Examples

Example 1 — GEO comsat EIRP and G/T check

A Ku-band transponder: TWTA 120 W (20.8 dBW), antenna transmit gain 32 dBi, path 35,786 km at 11.95 GHz, ground station G/T = 30 dB/K. Downlink C/N₀ for C/T of −160 dBW/K/Hz?

EIRP = 20.8 + 32 = 52.8 dBW.
Lfs = 92.45 + 20log(11.95) + 20log(35786) = 92.45 + 21.55 + 91.07 = 205.1 dB.
C/N₀ = 52.8 − 205.1 − 0.5 (atmos) − 0.3 (pointing) + 30 − (−228.6) = 105.5 dBHz.
For a 36 MHz channel carrying 54 Mbit/s QPSK (27 MBaud), required C/N₀ = Eb/N₀ (9.6 + coding 5 ≈ 5 dB) + 10log(27×10⁶) = 10.6 + 74.3 = 84.9 dBHz → margin ≈ 20 dB. ✓ Comfortable.

Example 2 — Hydrazine vs electric station-keeping

15-year GEO life needs Δv = 550 m/s. Compare propellant mass fraction for Isp = 220 s vs 3000 s.

Hydrazine: 1 − exp(−550/(9.81×220)) = 1 − exp(−0.255) = 22.5%.
Electric: 1 − exp(−550/(9.81×3000)) = 1 − exp(−0.0187) = 1.85%.
A 3,000 kg GEO satellite saves ≈ 3,000 × (0.225 − 0.0185) ≈ 620 kg — traded against months of electric orbit-raising time.

Example 3 — Reaction wheel momentum sizing (LEO)

A 200 kg Earth-observation satellite suffers solar-pressure residual torque 2×10⁻⁴ N·m (LEO example exaggerated to include aero). Wheels must store one orbit of secular momentum (94 min) with 50% margin. Required wheel momentum?

H = τ·T = 2×10⁻⁴ × 5640 s = 1.13 N·m·s; with 50% margin: Hreq ≈ 1.7 N·m·s.
A single 2 N·m·s wheel saturates before one orbit → use 4 wheels in pyramid (2 N·m·s each, sharing 1.4 N·m·s total) and unload with torque rods every orbit. This is exactly how 10–15 kg CubeSats are also designed (scaled down).

Example 4 — Battery sizing for LEO

Payload+bus draw 350 W during 35 min eclipse at 28 V bus; allowed DoD 30%; discharge efficiency 0.95. Capacity?

Energy needed: E = P·t = 350 W × 0.583 h = 204 Wh.
C = E / (V·DoD·η) = 204 / (28 × 0.30 × 0.95) = 204 / 7.98 ≈ 25.6 Ah → a single 30 Ah Li-ion string (with cell balancing), or two 30 Ah strings for redundancy; BOL capacity margin ~15% covers aging over the mission life.

Example 5 — SAR payload power sanity check

StripMap SAR at 700 km, X-band (9.65 GHz), 40 MHz chirp bandwidth, antenna 4.8 m × 0.7 m (TerraSAR-X-like), peak Tx 3.3 kW. Rough link margin logic: resolution cell σ⁰·δr·δaz with σ⁰ ≈ −10 dB, δr = 3 m, δaz = 3 m → σ = 0.1×9 ≈ −0.5 dBsm. Accepting the computed SNR ≈ 15–20 dB from the radar equation for this class, the design point is consistent with published SAR mission parameters — always verify against the radar equation as taught in the radar-equation sections.

Section 14

14. Formula and Design-Rule Sheet

#RelationUse
1Δv = g₀·Isp·ln(m₀/mf)Propellant mass from manoeuvre budget
2mp/m₀ = 1 − exp(−Δv/g₀Isp)Propellant fraction
3PBOL = 1361·η·A·cosθ·KtempSolar array sizing
4Cbat = P·tecl/(V·DoD·η)Battery capacity
5Q = εσSBA(T⁴ − Tspace⁴)Radiator sizing
6τ = m × BMagnetic torque (LEO desaturation)
7Hwheel ≥ τdist·TMomentum storage requirement
8Lfs = 92.45 + 20logfGHz + 20logRkmFree-space path loss
9C/N₀ = EIRP − L + G/T − kLink budget (k = −228.6 dBW/K/Hz)
10(C/N₀)tot−1 = Σ(C/N₀)i−1Combining uplink/downlink/IM/interference
11Rslant,max = √( (Re+h)² − (RecosE)² ) − ResinEGround-contact geometry
12δaz = L/2; δr = c/(2B sinγ)SAR resolutions
13R(t) = e−λt; two-parallel: Ps = 1 − (1−R)²Reliability math
14EIRP = Pt + Gt; G/T = G − 10log TsPayload figures of merit

Section 15

15. Glossary of Key Terms

TermDefinition
Bus / platformThe satellite structure and supporting subsystems that carry and service the payload
PayloadMission equipment (transponders, sensors) that the satellite exists to operate
ADCSAttitude Determination and Control Subsystem
BOL / EOLBeginning / End of Life (array power, reliability conditions)
TTC / TT&CTelemetry, Tracking and Command — the satellite's link to the ground
Bent-pipe transponderRepeater that translates and amplifies signals without demodulation
EIRPEffective isotropic radiated power, Pt·Gt (dBW + dBi)
G/TFigure of merit: antenna gain over system noise temperature (dB/K)
FDIRFault Detection, Isolation and Recovery (autonomy)
MLIMulti-layer insulation (thermal blanketing)
OSROptical solar reflector (low α/ε radiator surface)
PMDPropellant management device (surface-tension liquid acquisition)
CCSDSConsultative Committee for Space Data Systems (standards body)
SEU / TIDSingle-event upset / total ionizing dose (radiation effects)
Safe modeMinimal autonomous configuration awaiting ground recovery
Station-keepingSmall manoeuvres maintaining assigned orbital box

References

  1. J. J. Pocha, An Introduction to Mission Design for Geostationary Satellites, Springer, 1987.
  2. M. J. Sidi, Spacecraft Dynamics and Control: A Practical Engineering Approach, Cambridge, 1997.
  3. W. J. Larson & J. R. Wertz (eds.), Space Mission Analysis and Design, 3rd ed., Microcosm, 1999.
  4. G. Maral & M. Bousquet, Satellite Communications Systems, 5th ed., Wiley, 2009.
  5. I. G. Ngoma (ed.), Satellite Systems for Personal Applications, Wiley, 2010.
  6. A. K. Maini & V. Agrawal, Satellite Technology, 2nd ed., Wiley, 2010.
  7. J. C. Anselmo et al., Synthetic Aperture Radar for Earth Observation, ESA reference materials.