The Return Leg · A Surface-Power Question

Coming Back.

A standing premise first, because everything below depends on it: no magnetic fusion device has ever produced more fusion energy than the heating power put into it. The plant in our numbers is a peer-reviewed design, not a machine. With that stated, the question this page answers is simple to ask. A ship that lands on Mars has to make its fuel there to come home. How much power does that take — and at what point, if ever, does fusion become the way to supply it?

Claim type
Computed order of magnitude — ranges on every number, conditions instead of dates
Built from
Process stoichiometry, published specific energies, five independent literature estimates
Premise
Fusion figures assume a plant that has not been built; fission and solar figures do not
Status
Stated September 2026, revised the same month after one external review. Corrected 27 September 2026: this page first said the review led to seven accepted corrections; the review record shows nine. Revised again the same day: a correction to how much the Martian air cools a radiator raised the fusion plant’s landed mass from about 70,000 to about 80,000 tonnes, moving the crossover from about 490 to about 560 ships per window. No conclusion changed. Our own headline claim was narrowed by this computation; the narrowing is on this page.
01 · The Question

Every Frontier Is Two Journeys

Getting somewhere is a propulsion problem. Getting back is a supply problem. A Starship-class vehicle leaving the Martian surface for Earth needs, in the published plan, full tanks: about 1,200 tonnes of liquid methane and oxygen.2 None of it can be carried from Earth economically, so all of it is made on site — water mined from ice and split, carbon dioxide pulled from the air and combined with the hydrogen. That is a chemical plant, and a chemical plant is an electrical load. We sized the load.

02 · The Cost

A Megawatt Per Ship

Per returning ship: ≈ 10 GWh of electricity (4.6–16.9), of which three quarters goes to splitting water.6

Spread over the roughly 500 days a landed ship waits for its window home, that is about one megawatt of plant capacity per ship (0.5–1.7), running most of the time — an average draw of about 0.8 megawatts. Five published estimates, none derived from ours, bracket the same range.1234 With today’s reference reactors, the power source and the propellant plant for one returning ship weigh roughly 230–275 tonnes on the ground — more than the ship carries as payload. So the first result is plain: coming back is an energy problem before it is a rocket problem.

At fleet scale the numbers stack. A thousand ships per window, the publicly stated ambition,12 needs about a gigawatt of power plant on the surface. That is the largest surface electrical load in anything we reviewed for Mars — and it lands, uninvited, in exactly the power class of a fusion plant.

03 · What We Guessed, and What Died

Fusion Is Not the Way Home Narrowed

Before running this, we wrote down what we expected, dated and sealed, together with the result that would prove us wrong. Our claim was that fusion is the return technology of the surface frontier. The computation did not support it.

Fission has no fixed limit for this job. A reference fission unit is designed for 40 kilowatts5 — a design target; none has flown. Twenty-four of them refuel one ship per window, and twenty-four more refuel the next. The practical limits are landings, radiator area and spacing, not physics. Fusion is never the only way home. It can only be the lighter one — and whether it is depends on which fission you compare it with.

Compared withFusion lighter aboveReading
Today’s fission units (0.0067 kW per kg)≈ 560 ships per window280–990; ≈ 330 counting replacementsFusion winsinside the stated fleet ambition
Megawatt-class fission (0.02–0.06 kW per kg)never, within one plant’s capacitytwo independent design studies; none builtFission winsunless the plant is partly built on Mars
Solar with storage≈ 250–830 ships per windowFusion winsdust derates solar; it does not kill it
The Moon, any cadenceneverNot neededsolar and fission land 5–27× lighter

One more honest line. Dust storms are the usual argument for nuclear power on Mars, and they hold against solar — the 2018 storm cut array output by 97 %.7 But making propellant is a load you can defer and store, so solar is slowed by dust, not stopped. And the argument says nothing at all about fission versus fusion: both run through a storm unchanged. We will not use it for more than it proves.

NASA reached the same starting point from the other side. In December 2024 it chose fission as the primary power source for crewed Mars missions, noting that making propellant could need megawatt-class power.17 Its 2025 model of a Mars fuel plant found fission lighter than solar panels with batteries, and the power system alone up to 59 % of the plant’s landed mass.18 Both documents are recent; our numbers were computed independently of them, and they agree in direction.

04 · Where Fusion Enters

The Smallest Unit That Fits the Fleet

What survives is narrower and, we think, more useful. One reference fusion plant — about 850 megawatts net11 — refuels roughly 890 ships per window. A fusion plant cannot be built small; its nuclear shielding does not shrink with it. Its smallest sensible size happens to match the fleet people talk about. That is a coincidence of scale, and it decides nothing on its own.

What decides it are two open questions, both checkable: how light megawatt-class fission becomes — two independent design studies put it at 0.026 to 0.06 kilowatts per kilogram, none built1516 — and whether the heaviest precision parts of a fusion plant — its magnet plate steel — can be made on the surface instead of shipped. If the second is yes, fusion becomes lighter above a few hundred ships even against the better fission. If both go the other way, fusion is not the return technology at all, and this page will say so.

The order does not depend on either answer. Fission arrives with the first ships and adds capacity with every unit landed. A fusion plant delivers nothing until it and the factory that builds it are standing. Fission carries the first several hundred ships home, whatever happens after.

05 · The Moon

The Moon Says No

From the lunar surface the climb is shorter, and no lunar carbon resource has been shown to be usable for making methane at scale, so only the oxygen is made locally. A return leg costs 1–2.5 GWh. Fusion’s power class is reached only at around a thousand return flights a year, and at that pace polar solar and megawatt fission both land five to twenty-seven times lighter than a fusion plant. On the Moon, fusion is a plant to prove, not a way home. We had argued the first; this computation removes any temptation to claim the second.

“Coming back is an energy problem before it is a rocket problem. Fission carries the first few hundred ships. Above that, the return leg becomes the one surface load in fusion’s class — if two open conditions fall the right way.” The claim, as it stands after the arithmetic. The original version was broader, and it did not survive.
Why “Far Ahead” Is a Structure

Conditions, Not Years.

Fusion on a planetary surface is far away, but the distance can be listed. Before any of this matters, a magnetic device has to exceed breakeven, which none has; the best result stands at about two-thirds.10 A breeding blanket has to be measured making its own fuel. A reactor of the hundred-kilowatt class has to run on another world — the only one tested so far ran on the ground, in Nevada, at about a kilowatt.13 Machines have to dig and build off Earth at the tonne scale, which has never been done; the deepest hole beyond Earth is 2.25 metres.14 Then the fleet has to exist, and then the factory that makes the plant. Each is a condition. None has a date. Several have funded programmes behind them. That is what we mean by far ahead, and not never.

What Compute Changes

The Deciding Gets Faster. The Building Does Not.

Fusion’s hard problems split in two. Some need hardware no model can replace: a burning plasma, a neutron source to test materials, a divertor under real load. Those move at the speed of machines. Others need only analysis that nobody had done — what a plant weighs off Earth, how it rejects heat without air, what it costs to come home. Those now move at the speed of computation. Neural surrogates already run fusion turbulence simulations about 100,000 times faster than the codes they learn from,8 and AI-driven digital twins are part of at least one plant programme on Earth.9 Earth fusion is held up by hardware. Off-world fusion is held up by analysis. The second half is where the acceleration is real, and it is the half this page is made of.

Download the technical memorandum — FUNNY-TM-2026-001 Rev G, Electric Power Requirement for Surface Production of Return Propellant (PDF, 12 pages) → · the calculation script (Python)
Every step, assumption and range, each number tagged as measured, calculated, estimated or single-source. The input that decides the most — how light megawatt-class fission gets — is bracketed by two independent design studies, and the memorandum says plainly that no such reactor has been built. Revision B incorporated an external review: nine corrections accepted, three rejected with the reason shown, three confirmed unchanged, and three further errors we found ourselves while recomputing. Revision D adds NASA’s 2024 decision and 2025 plant model, a process diagram with the energy of every step, and the fusion plant’s itemised mass; Revision F carries its corrected radiator field. Every table in the memorandum is produced by the published script. The revision record lists all of it.

A standing premise of this page: no magnetic-confinement device has yet demonstrated net fusion gain, and the fusion plant in these figures is a peer-reviewed design, not built hardware. Fission and solar figures rest on published programme values. Computed September 2026 in our internal research record; one external cross-model review received and incorporated, no human peer review yet.

Sources & Grounding

Check Our Work.

Every number above traces to a source or to our own arithmetic, and the memorandum shows the arithmetic. Click a number in the text to land here.

The 18 sources, gradedexpand
  1. MeasuredMiyajima, ICES-2023-169: break-even analysis of Mars propellant production for Starship; about 1.04 MW per ship-equivalent, 9.7 kWh per kg. ICES 2023, TTU repository →
  2. MeasuredMaiwald et al., Scientific Reports 14:11804 (2024): full tanks required for the return; 14–16 kWh per kg at first-generation hardware; the MW-class fission value it quotes, traced to its origin in source 16. Scientific Reports, nature.com →
  3. MeasuredKleinhenz & Paz, AIAA-2017-0423: full-scale propellant plant for a Mars ascent vehicle; 13.6 kWh per kg excluding regolith heating. NTRS 20170001421 →
  4. MeasuredRucker et al., AIAA SPACE 2016, Solar Versus Fission Surface Power for Mars: solar lighter for a deferrable load, fission lighter through a 120-day storm. NTRS 20160010550 →
  5. EstablishedFission Surface Power programme requirement: 40 kWe, no more than 6,000 kg, 10-year life. A requirement, not a flown unit. NETS 2023 FSP overview, NTRS →
  6. MeasuredU.S. DOE Hydrogen Program: PEM electrolyser system at 55.2 kWh per kg of hydrogen, the dominant term in the energy per ship. DOE Record 24005 →
  7. MeasuredGillespie et al., JGR Planets 2020: the 2018 global dust storm and its effect on surface solar power. JGR Planets, AGU →
  8. MeasuredGyroSwin (arXiv 2510.07314, 2025): neural surrogate for five-dimensional gyrokinetic turbulence, up to five orders of magnitude faster than full simulation. Preprint. arXiv 2510.07314 →
  9. ReportedCommonwealth Fusion Systems with Siemens and Nvidia: AI-driven digital twins in a fusion plant programme. Company announcement. cfs.energy →
  10. EstablishedNo magnetic-confinement device has exceeded plasma breakeven; the record ratio, about 0.67, was set at JET in 1997. EUROfusion, history of fusion →
  11. CalculatedReference plant: Stellaris, a peer-reviewed quasi-isodynamic stellarator design (Lion et al., Fusion Engineering and Design 214:114868, 2025; read in full). The 850 MW net and 70 kt landed figures are our own computations on that design, not the paper’s. Publication announcement →
  12. ReportedThe stated ambition of about 1,000 ships per Mars window, as reported. A public statement, not a plan of record. space.com →
  13. MeasuredKRUSTY nuclear system test (Poston et al., Nuclear Technology 2020): the 2018 ground test of a kilowatt-class space fission reactor. Ground test; not flown. NASA NTRS 20205009351 → (also OSTI 1648091)
  14. EstablishedLuna 24 (1976) drilled to 2.25 m, still the deepest penetration made off Earth, checked against our register of more than 100 primary sources. Luna 24 mission record, LPI →
  15. MeasuredMason, NASA/TM-2001-210593 (NASA Glenn): surface reactor systems with crew-rated shielding at 500 kWe, 38.2 kg/kWe near-term to 19.0 kg/kWe with all advances — 0.026 to 0.053 kW per kg. A design study; no such system built. NTRS 20010016863 →
  16. ReportedPoston, Space Nuclear Power Corporation, presentation (2021): a 2 MWe surface system at about 32,000 kg with modest shielding — 0.0625 kW per kg. The origin of the value quoted by source 2. Company presentation, not peer reviewed. SpaceNukes presentation (PDF) →
  17. EstablishedNASA, Mars Surface Power Technology Decision (2024 Moon to Mars Architecture Concept Review, December 2024): fission selected as the primary surface power for crewed Mars missions; propellant manufacturing could require megawatt-class power. An agency decision record. nasa.gov (PDF) →
  18. MeasuredAndersen, Carlson, Ostendorp & Collins, “Assessing the Feasibility of a Martian ISRU Propellant Plant”, AIAA ASCEND 2025 (NASA JSC model study, extended abstract): for 30 and 300 t of methane and oxygen per Mars year, fission traded better than solar with batteries; power system 34–59 % of plant landed mass; electrolysis 53–62 % of plant power. NTRS 20240014064 →

Full derivation, assumptions and sensitivity: FUNNY-TM-2026-001 (download above). Internal research record, September 2026; not externally reviewed.