Subsystem 02 of 12 · Power
Lunar Habitat ACT, the Autonomous Construction Testbed·Power·Concept definition, revision A·August 2026·See it in the tour

Forty eight kilowatts, and a night that is not a fortnight

The load never falls below 27.6 kW. At the equator the sun is gone for 14.7 days at a stretch. At the Shackleton rim the longest dark spell is a day and a half to a few days depending on the model, the array is still dark 12 to 23 percent of the year, and the in situ resource utilisation (ISRU) plant wants power the sun does not give. Every power architecture is an argument about that gap.

48 kWarray peak
210 kWhstorage
1.5 to 2.7 dlongest dark spell at the rim, by model
Contents
  1. The load, honestly stated
  2. Why the array is vertical
  3. The night
  4. Fission surface power
  5. Storage, and what it is actually for
  6. Distribution
  7. Dust, and the slow loss nobody budgets for
  8. Mass and cost
  9. Failure modes
  10. What is not yet known
  11. Increment plan
  12. Sources and further reading
Section 01

The load, honestly stated

Concept studies tend to quote peak generation and leave the load vague. The load is the hard part, because almost none of it can be shed. Life support runs continuously. Thermal control runs continuously and gets harder at night, not easier. The ISRU plant can be throttled, and is the only significant flexible load on the base.

Continuous load by subsystem ISRU plant 14 kW throttleable Greenhouse lighting 14 kW photoperiod, partly shiftable Habitation core 6.8 kW not sheddable Laboratory 3.9 kW partly sheddable Thermal control 3.4 kW rises at night Airlock and suit servicing 1.4 kW duty cycled Cupola and comms 1.5 kW not sheddable Connectors and margin 0.6 kW 45.6 kW with everything in this table running. The 27.6 kW habitat figure is the six module budget; ISRU, thermal control and comms are extra lines here.
The greenhouse is the surprise in this table. It draws as much as the ISRU plant, for 54 cubic metres of volume, because photosynthesis is the only process on the base that has to manufacture its own sunlight. It is also the most shiftable: plants do not care whether their photoperiod aligns with the lunar day.
Section 02

Why the array is vertical

At this site the sun stays low. A horizontal panel of the kind used in Earth orbit would see it at a grazing angle for the whole lunar day and produce a fraction of its rating. A vertical array, rotated slowly about one axis to follow the sun round the horizon, keeps the incidence angle near normal for as long as the sun is above the local horizon. The sun never climbs more than about 1.5 degrees above the horizon at the pole, the tilt of the Moon's spin axis to the ecliptic, and modelling based on the Lunar Orbiter Laser Altimeter (LOLA) gives the best Shackleton rim site 240 days of sun without a break.

This also solves a dust problem for free. A horizontal surface collects settling regolith. A vertical one sheds most of it, and what remains can be cleared electrostatically without anyone touching the panel face.

48 kWpeak, one axis tracked
77 to 88%of the year lit at 2 m, best rim and ridge sites
1 axisrotation, azimuth only
1.5°highest the sun ever gets at the pole
Section 03

The night

This is the section that decides the architecture, and it starts by saying what the night is. At the equator it is 14.7 days, and at even the reduced 27.6 kW habitat load that is 9,740 kWh. Lithium ion at a generous 250 Wh/kg, before packaging, thermal control and depth of discharge margin, gives about 39 tonnes of battery, a thirty nine billion dollar battery at a million dollars a kilogram. That is the case most readers know, and it is not this site. LOLA based illumination modelling at 240 m resolution finds a site on the Shackleton rim lit continuously for 240 days with a longest dark spell of about 1.5 days; the 20 m resolution model gives the best rim clusters a longest shadow of 65 to 66 hours and the best Connecting Ridge cluster 112 hours, and puts the best sites at 2 m above the ground in sun 77 to 88 percent of the year. A 36 hour spell at 27.6 kW is about 1,000 kWh, roughly 4 tonnes of cell before packaging. A 66 hour spell is about 1,800 kWh and 7.3 tonnes, already heavier than the reactor. The reactor is in the architecture for three reasons that survive that arithmetic: the longest gap at the exact array position has not been computed, and a few metres of position or height changes it; the array's output over the year is 12 to 23 percent below what a lit array gives, and the winter brings the gaps in a series; and the ISRU plant and the sintering gantry are loads that should not follow the sun. That is a weaker argument than a fourteen day night, and this document says so.

Equatorial night, 14.75 days, not this site 0 10 20 30 40 50 0 5 10 15 20 25 29.5 Days through one lunation Kilowatts Solar generation Habitat load Fission output
The equatorial reference case, one 14.75 day night, kept because it is the one most readers know. It does not apply at the Shackleton rim, where the sun circles the horizon and the dark comes as spells of hours to a few days set by the local relief. The fission line is drawn flat because the reactor runs continuously once it is on line: in daylight it load follows and the surplus goes to the ISRU plant, which is why the plant runs hardest when the array is lit. At the 27.6 kW habitat load the 210 kWh store lasts 7.6 hours.
OptionMass for the equatorial 14.7 day nightLanded costMass for a 66 hour spellVerdict
Lithium ion only250 Wh/kg, 80% depth of discharge (DoD)39 t$39 bn7.3 tHeavier than the reactor even for the rim spell, and the longest spell here is not yet computed
Regenerative fuel cellH2 and O2, 500 Wh/kg, near the top of NASA Glenn's 110 to 550 Wh/kg range19 t$19 bn3.6 tLighter than cells, and NASA Glenn ran a full system on the ground in 2026, but it adds gas storage and thermal switching and it still follows the sun
Fission surface power40 kWe class6 t$6 bn6 tViable, does not depend on the local horizon, and the only option that scales
Fission plus 210 kWh bufferthe architecture here6.9 t$6.9 bn6.9 tBuffer covers reactor transients and peak load
Section 04

Fission surface power

NASA's Fission Surface Power project set the class this architecture is sized around: a 40 kWe reactor of no more than six tonnes, a design life of at least ten years and no crew intervention. Three industry teams, Lockheed Martin, Westinghouse and IX, were awarded twelve month Phase 1 design contracts of about 5 million dollars each in June 2022 and completed them in 2023. In August 2025 NASA's directive on fission surface power moved the target to a minimum of 100 kWe with a closed Brayton cycle, carried on a heavy class lander and ready to launch by the first quarter of 2030. The 40 kWe unit here is therefore a class, not a product. If the 100 kWe unit flies first, one of them carries this base with margin to spare. It is still the single largest piece of infrastructure the base depends on that does not yet exist.

NASA's own 40 kWe point design, worked up by the Glenn Compass team for a south pole outpost, is the reference for what the unit is and where it stands. It is a heat pipe cooled reactor on high assay low enriched uranium, with eight 6.2 kWe Stirling convertors in opposed pairs, deployable radiators and a shadow shield rather than a full shield, carried to site in three sleds by a repurposed crew rover chassis. The study places the reactor about one kilometre from the crew, the distance at which the shadow shield holds the dose below 5 rem a year for permanently present crew, and it notes that moving the reactor further away or over the horizon does not reduce the shield mass. The base follows that. The unit stands about one kilometre out on the far side of a natural rise, with a regolith berm on the habitat side as a second line, and the crew's working area stays inside the shielded sector. Power leaves the reactor at plus or minus 2,800 V DC over an aluminium cable that the study puts at about 45 kg for the kilometre, and is bucked to 120 V DC at the habitat end.

Honest statement of risk

Increment three depends on hardware that has not been built. The closest flown relative is KRUSTY (Kilopower Reactor Using Stirling Technology), the 1 kWe class Kilopower core that NASA and the Department of Energy ran at the Nevada National Security Site in March 2018, and a 40 kWe unit is a different machine. If fission surface power slips, the base does not stop, but the ISRU plant does. The plant is the largest flexible load and would be shut down through the night, which turns the outpost from a construction base back into a shelter with a resupply bill. That is the schedule risk worth arguing about, and it is not a habitat risk.

Section 05

Storage, and what it is actually for

210 kWh of lithium ion is not there to carry the night. It is there for four things that all happen on timescales of minutes to hours: reactor start transients, the peak when the airlock cycles while the greenhouse is at full photoperiod, ride through when a string trips, and the shadow transits when a local ridge takes the low sun off the array faster than the reactor can ramp.

FunctionEnergyDurationWhy storage and not generation
Reactor ramp coveragecold start40 kWh1.5 hA reactor cannot follow a step load
Peak clippingairlock plus greenhouse22 kWh40 minCheaper than sizing generation for a rare peak
String trip ride throughsingle fault28 kWh1 hBuys time to isolate and reconfigure
Shadow transitwhen local relief occults the sun95 kWh3.5 hArray falls off faster than the reactor ramps
Total sized185 kWh210 kWh installed, 12 percent margin
Section 06

Distribution

Everything runs at 120 V DC. There is no reason to carry an inverter and its losses when every source on the base is inherently DC and every load can be. The exception is the ISRU plant, whose electrolysis cells want low voltage and very high current, and which therefore has its own converter sited at the plant rather than at the habitat. The other exception is the reactor line: a kilometre at 120 V would need a cable of hundreds of kilograms, so the reactor's converter boosts to plus or minus 2,800 V DC for the run and a second converter at the field combiner brings it back to the bus voltage, as in NASA's study.

Solar array 48 kW peak Fission unit 40 kWe 120 V DC bus dual, isolatable Battery 210 kWh Habitat 27.6 kW ISRU plant 14 kW Construction 9 kW buffer
The bus is dual and isolatable at every branch. A fault anywhere on the construction or ISRU side can be dropped without touching the habitat, which is the whole reason for splitting them.
Section 07

Dust, and the slow loss nobody budgets for

Regolith is electrostatically charged and moves near the terminator. It settles on everything. The Apollo dust detector experiments at the 12, 14 and 15 sites measured settling dust at about 100 micrograms per square centimetre a year, enough to cut the output of their solar cells measurably over the years they ran, and on Apollo 16 and 17 the rover batteries ran over their temperature limits because dust on their radiators could not be brushed off.

A vertical array sheds most of what lands on it. What remains is cleared by an electrodynamic dust shield, a set of transparent electrodes on the panel face driven with a travelling wave that walks charged particles off the edge. NASA demonstrated it on the Blue Ghost lander in March 2025, where it lifted regolith off glass and radiator surfaces, and it has no moving parts. The alternative, sending a crew member out with a brush, both wears the coating and consumes the scarcest resource on the base, which is crew time.

100 µg/cm²a year of settling dust, Apollo 12, 14 and 15
March 2025electrodynamic shield proven on the surface
0moving parts in the shield
0 hcrew time per clean
Section 08

Mass and cost

ElementMassPowerIncrementNote
Solar array and mastone axis tracked1,240 kg48 kW peak1Vertical, about 120 m² of cell at 30 percent efficiency and 1,361 W/m²
Battery, 210 kWhlithium ion890 kgnone1Includes thermal control and packaging
Fission surface power40 kWe class6,000 kg40 kW3Includes shielding and radiator
Power management and distributiondual bus410 kg1.1 kW losses1120 V DC throughout
Cabling1 km reactor line and site runs320 kgnone1 to 3Aluminium, not copper, on mass grounds. The kilometre at 2,800 V is about 45 kg of this in NASA's study; the 120 V site runs are the rest
Electrodynamic dust shieldsarray face34 kgnot yet budgeted2Removes all crew time from cleaning
Total8,894 kg88 kW installed$8.9 bn landed at $1M/kg

Power is the single heaviest subsystem on the base, at nearly nine tonnes, and the reactor is two thirds of it. That is the price of not being dependent on the sun, and it is the reason the ISRU plant has to earn its keep: a base that lands nine tonnes of power hardware and then still ships oxygen from Earth has not made an argument for itself.

Section 09

Failure modes

FailureEffectBufferResponse
Array string tripone of six strings8 kW lost210 kWhReconfigure. Daylight surplus absorbs it entirely.
Reactor scramin a dark spell40 kW lost210 kWh at 27.6 kW is 7.6 hShed ISRU and greenhouse, hold life support and thermal. Restart, or hold survival load until the sun clears the ridge.
Battery string failureone of four52 kWh lostRemaining 158 kWhIsolate. Shadow transits become tighter but remain covered.
Bus faultshort on one sideHalf the baseDual busIsolate the faulted side. Every load has a feed from both.
Dust accumulationgradualOutput fallsWeeks of marginElectrodynamic clearing while the array is lit.
Section 10

What is not yet known

The longest dark spell at the exact array position has not been computed. The 1.5 day figure is for the best rim site in a 240 m per pixel LOLA model; the 20 m per pixel model gives the best rim clusters 65 to 66 hours and the best Connecting Ridge cluster 112 hours, so the design gap sits somewhere between a day and a half and five days until the site is modelled at the mast position. How much dust a vertical face collects against a horizontal one has not been measured; the Apollo detectors were horizontal cells. The shield's power draw at array scale is not yet budgeted. No fission unit exists. NASA's 2025 directive targets a minimum of 100 kWe ready to launch by the first quarter of 2030, and if it slips the ISRU plant runs only while the array is lit and the outpost falls back to a shelter with a resupply bill. That is the schedule risk worth arguing about. The communications document carries the mast at 0.9 kW continuous while the load table here folds 0.6 kW of comms into the cupola line; the two have to be reconciled.

Section 11

Increment plan

Increment 1, solar and storage

48 kW of array and 210 kWh of battery, landed with the habitat. This supports the habitat while the array is lit and for 7.6 hours of dark at full load. Early increments accept a reduced night mode through the longer spells.

Increment 2, second string and the reactor's site

Electrodynamic shields on the array face, a second distribution string so no single bus fault can reach the habitat, and the reactor's ground work: the berm, the graded kilometre for the cable and the field combiner, laid while the unit is still being built on Earth.

Increment 3, fission surface power

The 40 kWe unit, delivered by rover to a point about 1 km out and cabled back at plus or minus 2,800 V DC. This is the step that makes continuous ISRU operation possible and turns the base from a shelter into a plant, and it is the one that waits on NASA's reactor schedule.

Increment 4, capacity for construction

Additional array to cover the sintering gantry at full duty. Construction is the load that grows fastest as the site expands.

Sources

Sources and further reading

Every figure in this document traces to one of these. Agency documents and peer reviewed work first, reporting only where it is the primary record.

NASA, Artemis concept awards for nuclear power on the Moon, June 2022 nasa.govLockheed Martin, Westinghouse and IX; 40 kWe class, at least ten years, about 5 million dollars each for twelve months
NASA, request for industry feedback on Fission Surface Power nasa.govThe 40 kWe, six tonne, ten year class this architecture is sized around
NASA, directive on Fission Surface Power, 4 August 2025 nasa.govMinimum 100 kWe, closed Brayton cycle, heavy class lander, ready to launch by the first quarter of 2030; notes the 2023 completion of the 40 kWe Phase 1 studies
NASA, demonstration proves nuclear fission system can provide space exploration power, May 2018 nasa.govKRUSTY, the 1 kWe class Kilopower ground test at the Nevada National Security Site, March 2018
Mazarico et al., Illumination conditions of the lunar polar regions using LOLA topography, Icarus, 2011 https://ntrs.nasa.gov/citations/20120010094Shackleton rim site: 240 days of continuous sun, longest dark spell about 1.5 days, at 240 m per pixel
Gläser et al., Illumination conditions at the lunar poles: implications for future exploration, Planetary and Space Science, 2018 https://ntrs.nasa.gov/api/citations/20170007365/downloads/20170007365.pdfTable 1: 77.1 to 88.0 percent average illumination at 2 m; longest shadow 65 to 66 hours at the Shackleton rim clusters and 112 hours at Connecting Ridge C1, at 20 m per pixel
Williams et al., Seasonal polar temperatures on the Moon, JGR Planets, 2019 https://doi.org/10.1029/2019JE006028The 1.54 degree tilt of the spin axis to the ecliptic that caps the polar sun elevation
NASA, industry to mature vertical solar array technologies for the lunar surface nasa.govVertical Solar Array Technology (VSAT): the vertical, one axis tracked array class assumed here, with thermal vacuum tests in 2024
NASA, fuel cell tests pave way for energy storage on the Moon, 2026 nasa.govRegenerative fuel cell ground test at Glenn, February to May 2026; NASA states it can weigh less than batteries storing the same energy
Hollick and O'Brien, Lunar weather measurements at three Apollo sites 1969 to 1976, Space Weather, 2013 https://doi.org/10.1002/2013SW000978Dust settling at about 100 micrograms per square centimetre a year, measured by the Apollo dust detector experiments
Gaier, The effects of lunar dust on EVA systems during the Apollo missions, NASA TM 2005 213610 https://ntrs.nasa.gov/citations/20050160460Rover battery overheating on Apollo 16 and 17 from dust on the radiators
NASA, dust shield successfully repels lunar regolith on the Moon, Blue Ghost, March 2025 nasa.govThe electrodynamic clearing method assumed for the array face
NASA, State of the art of small spacecraft technology, power nasa.govMultijunction space cells at a nominal 30 percent, behind the cell area check
Kopp and Lean, A new, lower value of total solar irradiance, GRL, 2011 https://doi.org/10.1029/2010GL045777Solar constant 1,360.8 W/m², behind the cell area check
Oleson et al., A deployable 40 kWe lunar fission surface power concept, NASA Glenn Compass team, 2022 https://ntrs.nasa.gov/citations/20220004670Reactor about 1 km from the crew, under 5 rem a year with a shadow shield, eight 6.2 kWe Stirling convertors, plus or minus 2,800 V DC transmission, a 1 km aluminium cable of about 45 kg, 120 V DC at the user end
NASA Glenn, Regenerative fuel cell power systems for lunar and Martian surface exploration, 2017 https://ntrs.nasa.gov/citations/20170009088Specific energy goals of 110 to 550 Wh/kg, more than double space rated lithium ion at 200 Wh/kg; behind the fuel cell row in the night table
Electrical system of the International Space Station, Wikipedia https://en.wikipedia.org/wiki/Electrical_system_of_the_International_Space_StationPrecedent for a low voltage DC secondary bus, at about 124 V on the station