A link budget is the ledger of every gain and loss between transmitter and receiver, ending in a number we can compare with what the receiver needs. It answers the first of the six questions: does the link close?

TERPSat Received Power

Work the TERPSat Link

  • Given:

    • At 5° elevation: 𝑑=2574km
    • Frequency: 𝑓=8.4GHz
    • 𝑃𝑡=10W, [𝐺𝑡]=8dBi, [𝐿𝑡]=1dB
    • [𝐺𝑟]=45dBi, [𝐿other]=2dB
  • Calculate [EIRP], [𝐿𝑝], and [𝑃𝑟]

  1. EIRP:
    • [EIRP]=[𝑃𝑡]+[𝐺𝑡]−[𝐿𝑡]=10dBW+8dBi−1dB=17dBW
    • The spacecraft still transmits 10 W; antenna gain changes the on-axis equivalent
  2. Free-space path loss (edge cost):
    • [𝐿𝑝]=179.1dB at 2574 km (vs. 167.9 dB overhead at 705 km)
  3. Received power:
    • [𝑃𝑟]=[EIRP]−[𝐿𝑝]+[𝐺𝑟]−[𝐿other]=17−179.1+45−2=−119.1dBW
  • Does the link work? We still need noise, required performance, and margin

Check the Complete Ledger

  • Follow the reference point; write every gain and loss with its sign
TermValueRunning power [𝑃]
[𝑃𝑡]10 dBW10 dBW
−[𝐿𝑡]−1 dB9 dBW
+[𝐺𝑡]+8 dBi17 dBW
−[𝐿𝑝]−179.1 dB−162.1 dBW
+[𝐺𝑟]+45 dBi−117.1 dBW
−[𝐿other]−2 dB−119.1 dBW

NOTE

  • The path loss is enormous; the antenna gains are what make the link plausible

Predict Before Calculating

  • What happens to received power if we double transmit power?
  • What happens if we double range instead?
  • What do we gain — and lose — by raising the elevation mask?
  • Does adding a ground station necessarily strengthen this link?

Answer not on slide

Voyager 2 Received Power

Homework 2: Voyager 2

  • Problem statement (lec03 slide 4, a screenshot of the Homework 2 handout): total received signal power for Voyager 2’s X-band link to DSS-43 (the 70 m antenna in Canberra), using the updated range with radio parameters from JPL’s January 1, 1996 budget (Ludwig and Taylor, Voyager Telecommunications, JPL DESCANSO 2002, Table 5-3)
  • Given:
    • Range 21,476,670,660 km, i.e. 𝑅=2.147667066⋅1013m (21,476,670,660,000 m)
    • 𝑓=8.415GHz, 𝑃𝑡=12.3W, [𝐺𝑡]=48.20dBi, [𝐺𝑟]=74.01dBi
    • 0 dB transmit feed loss; 0.42 dB other losses (pointing, atmosphere, and polarization combined)
QuantityCalculationResult
[EIRP]10log10(12.3)+48.2059.10 dBW
[𝐿𝑝]32.45+20log10𝑅+20log10𝑓 (𝑅 in m, 𝑓 in GHz)317.59 dB
[𝑃𝑟]59.10−317.59+74.01−0.42−184.90 dBW
  • Is received power alone enough to predict data recovery?
  • Received power is only half the story; Class 4 carries the budget through noise to S/N₀

Example Inputs and Assumptions

  • Spacecraft → Earth, 8.4 GHz return link, range 384,400 km
  • Spacecraft: 1 W transmitter, 0.3 m transmit dish, transmit line loss 0.60 dB
  • Ground: 34 m receive dish, aperture efficiency 0.55
    • Antenna temperature 𝑇𝐴=30K (off the lunar disk — see the Moon)
    • Receive feed: 1 dB loss at 290 K
    • Receiver NF = 0.69 dB (𝑇𝑒,rx≈50K)
  • Other losses: 0.1 dB atmosphere + 0.8 dB pointing + 0.5 dB polarization = 1.4 dB
  • Tools (gain, path loss); diameter in meters, range in kilometers:
    • [𝐺]=17.8+20log10(𝐷/m)+20log10(𝑓/GHz)[𝐿𝑝]=92.4+20log10(𝑅/km)+20log10(𝑓/GHz)
  • Where do the 0.6 dB transmit loss and the 1 dB receive-feed loss go?
    • Transmit line loss → EIRP
    • At terminal A the signal has not yet passed through the receive feed → the feed loss lives in the noise ledger (and in G/T at A)

Signal Power at A

  • [𝑆𝐴]=[𝑃tx]−[𝐿tx]+[𝐺tx]−[𝐿𝑝]−[𝐿other]+[𝐺𝑟]

Lunar Link Signal Budget

TermValue
Transmitter power+0.0 dBW
Transmitter line loss−0.6 dB
Transmit antenna gain (0.3 m)+25.8 dBi
Free-space loss (384,400 km)−222.6 dB
Atmosphere + pointing + polarization−1.4 dB
Receive antenna gain (34 m)+66.9 dBi
Received 𝑆𝐴−131.9 dBW
  • Plane A precedes the receive feed; at B the signal is 1 dB lower
  • [EIRP]=0.0−0.6+25.8=25.2dBW

System Noise at A

  • All noise referred to antenna terminal A (two noise ledgers):
    • 𝐿𝑓=101.0/10,𝑇sys,𝐴=𝑇𝐴+(𝐿𝑓−1)𝑇phys+𝐿𝑓𝑇𝑒,rx

Lunar Link Noise at A

AntennaFeed emission, (𝐿𝑓−1)290Receiver via feed, 𝐿𝑓(50)Total 𝑇sys,𝐴
30.0 K75.1 K62.9 K168.0 K
  • [𝑇sys,𝐴]=10log10(168.0)=22.3dB-K
  • [𝐺/𝑇]𝐴=[𝐺𝑟]−[𝑇sys,𝐴]≈44.7dBK−1 (G/T)

Signal-to-Noise Density

Lunar Link S/N₀

  • 𝑁0,𝐴=𝑘𝑇sys,𝐴, so [𝑁0,𝐴]=[𝑘]+[𝑇sys,𝐴]
  • With [𝑘]=−228.6: [𝑁0,𝐴]≈−206.35dBWHz−1
  • [𝑆/𝑁0]=[𝑆𝐴]−[𝑁0,𝐴]=−131.87−(−206.35)=74.48≈74.5dB-Hz

The Complete Budget in One View

  1. Transmit: [EIRP]=25.2dBW
  2. Propagate: free space −222.6 dB; other losses −1.4 dB
  3. Collect: +66.9 dBi → [𝑆𝐴]=−131.9dBW
  4. Noise at A: 𝑇sys=168.0K, [𝑇sys]=22.3dB-K, [𝑁0]=−206.3dBWHz−1
  5. Compare: [𝑆/𝑁0]=74.5dB-Hz
  6. Design trades: more EIRP or G/T helps; more propagation loss hurts

NOTE

What Changes When We Point at the Moon?

  • Same signal power, but the beam now sees the lunar disk: 𝑇𝐴: 30 K → 230 K
  • 𝑇sys,new=𝑇sys,old+(230−30)=368.0K
    • 𝑇sys,𝐴: 168.0 K → 368.0 K; [𝑇sys,𝐴]: 22.3 → 25.7 dB-K
  • Δ[𝑆/𝑁0]=−10log10(368.0168.0)=−3.4dB
  • [𝑆/𝑁0]new=74.5−3.4=71.1dB-Hz

What Changes in the Budget?

Change (everything else held fixed)Effect
Double received signal powerΔ[𝑆/𝑁0]=10log10(2)=+3.0dB
Double range (gains and temperatures fixed)Δ[𝐿𝑝]=20log10(2)=+6.0dB, so S/N₀ drops 6.0 dB
Double 𝑇sys (signal budget fixed)Δ[𝐺/𝑇]=−10log10(2)=−3.0dB
Add 0.5 dB atmospheric lossΔ[𝑆/𝑁0]=−Δ[𝐿atm]+Δ[𝐺/𝑇]
  • Weather: update both the atmospheric signal loss and the antenna noise — atmospheric emission can change G/T, so 𝑁0 changes too (weather in the budget)

Link Budget Equation (S/N₀ form)

  • [𝑆/𝑁0]=[EIRP]−[𝐿𝑝]−[𝐿atm]−[𝐿point]−[𝐿pol]+[𝐺/𝑇]+228.6
  • EIRP: transmitter power, transmit-line loss, and transmit antenna gain
  • Losses: free space, atmosphere, pointing, and polarization
  • G/T: receive gain and total system noise at one plane (receive-feed effects are already in G/T)
  • The constant 228.6 is −[𝑘], for EIRP in dBW and G/T in dB/K

Lunar Link, One Line

  • [𝑆/𝑁0]=25.2−222.6−0.1−0.8−0.5+44.7+228.6=74.5dB-Hz
  • Noise and receiver references (Class 4): JPL DESCANSO Vol. 10, Ch. 2, System Noise Concepts with DSN Applications; NIST, Johnson-noise thermometry and SI defining constants; JPL Report 42-143, Follow-up Receiver Noise-Temperature Contribution; Keysight, Noise Figure Application / Noise Concepts; JPL DESCANSO Ch. 5, HEMT Low-Noise Amplifiers; Analog Devices AN-2622
  • Further reading: DSN 810-005 Modules 104 and 105 (station and environmental noise); ITU-R P.838-3 (rain attenuation) and P.618-14 (Earth-space propagation); Condon & Ransom, Essential Radio Astronomy, Chs. 1–3; ITU-R P.525-5 (free-space attenuation)
  • Class 5 extends the budget past S/N₀ to the energy per bit the demodulator actually sees

Link Budget Equation (Eb/N₀ form)

  • [𝐸𝑏/𝑁0]=[EIRP]−[𝐿𝑝]−[𝐿other]+[𝐺/𝑇]−[𝑘]+[𝑞]−[𝑅𝑏]
  • [𝑞]=10log10(𝑞), where 𝑞 is the fraction of received signal power allocated to data (power allocation)
  • [𝑅𝑏]=10log10(𝑅𝑏/1 bit/s), using the information bit rate
  • [𝑘]=−228.6dBW/Hz/K; 𝐺 and 𝑇sys use the same reference plane
  • Available 𝐸𝑏/𝑁0 must cover the requirement, implementation loss, and reserve (Link Margin)

The Remaining Trades

ChangeBudget effectMission cost
More data-channel EIRPMore available 𝐸𝑏/𝑁0Spacecraft power or antenna demands
Better G/T or lower lossesMore available 𝐸𝑏/𝑁0Ground hardware, siting, or operations
Lower information bit rateMore energy per information bitLonger delivery time
Different modulation / codingMay lower required 𝐸𝑏/𝑁0Bandwidth, complexity, or latency

WARNING

  • A lower requirement must come from a justified performance comparison at the same delivered error target
  • We have optimized power, antennas, receiver noise, losses, and data rate — and available 𝐸𝑏/𝑁0 still falls short of the requirement
  • Could we transmit the bits in a way that requires less 𝐸𝑏/𝑁0?
  • → Next class: Demodulation, BER, and Coding