SLPA is built on a simple principle: if you can store heat and move gas, you can move anything. The propulsion architecture is only half the story. The other half is how we obtain working gas and bulk mass off-world without rockets, refineries, or megastructures.
This page describes the gas-driven EMU (Extraction Mass Uplift) launcher – an in-situ mass launch system that turns subsurface ice and frozen volatiles into a reusable “barrel” for launching material into orbit using solar-heated gas.
Instead of building a physical gun barrel out of metal, the SLPA architecture uses the terrain itself as the structure. A robotic miner drills into ice or volatile-rich ground, freezes a solid column, and then drills a narrow acceleration EMU through that column.
Underneath this frozen barrel, a compact pressure chamber houses the engineered hardware: a pressure vessel, fast-acting valve, and instrumentation. Pressurised gas from a surface gas plant is fed down to this chamber and released into the EMU to accelerate projectiles into space.
The result is a gas cannon formed from the landscape itself – a reusable, self-healing launcher with almost no imported structure.
| Angle Range | Meaning | When Used |
|---|---|---|
| 0°–20° | Very shallow | Low-gravity worlds; efficient horizontal orbit injection |
| 20°–30° | Gentle slope | General-purpose EMU launches with balanced vertical and horizontal velocity |
| 30°–45° | Standard range | Most EMU launchers on the Moon and similar bodies; good all-round performance |
| 45°–60° | Steep | High orbits; higher-gravity surfaces; polar or steep ballistic trajectories |
| 60°–90° | Very steep / vertical | Special cases: escape trajectories or depots directly overhead; niche use |
| World | Surface Gravity | Required Exit Velocity | Typical Barrel Length | Peak Pressure Needed | Notes |
|---|---|---|---|---|---|
| Moon | 1.62 m/s² (0.165 g) | ~2.4 km/s | 35–60 m | 80–120 bar | Ideal EMU environment. Frozen regolith adds wall strength. |
| Ceres | 0.27 m/s² | ~0.6 km/s | 10–20 m | 25–40 bar | Extremely low difficulty. Near-perfect for mass drivers. |
| Europa | 1.31 m/s² | ~2.0 km/s | 30–50 m | 70–100 bar | Ice quality excellent; stable barrel formation at depth. |
| Ganymede | 1.43 m/s² | ~2.0–2.1 km/s | 35–55 m | 80–120 bar | Similar to Europa; regolith overburden gives strong support. |
| Enceladus | 0.11 m/s² | ~0.2–0.3 km/s | 5–10 m | 5–15 bar | Tiny escape velocity. EMUs here are extremely efficient. |
| Titan | 1.35 m/s² | ~2.6 km/s | 50–90 m | 120–180 bar | Dense atmosphere → EMU works only for surface-to-upper-atmosphere mass lift. |
| Mars | 3.71 m/s² (0.38 g) | ~3.6–4.0 km/s | 120–200 m | 200–300 bar | Not suitable for pure ice barrels; hybrid reinforced barrels required. |
Even with conservative assumptions—payloads of 5–10 kg per shell and firing intervals of 15, 30, or 60 minutes—throughput accelerates rapidly with tube count. The table below shows total payload mass delivered to orbit in a 24-hour period. A 50-tube installation firing every 15 minutes lifts 24–48 tonnes per day into lunar orbit. At 100 tubes, throughput reaches 48–96 tonnes per day, demonstrating how EMUs transition from experimental systems to full industrial mass-lift infrastructure. With even modest clustering, the EMU system expands rapidly in throughput. A 50-tube array firing every 15 minutes lifts 24–48 tonnes per day into lunar orbit, demonstrating why EMUs become a decisive enabler for large-scale off-world construction.
| Firing Interval | Tubes | 5 kg Payload (t/day) |
10 kg Payload (t/day) |
|---|---|---|---|
| 15 min | 1 | 0.48 | 0.96 |
| 10 | 4.8 | 9.6 | |
| 50 | 24 | 48 | |
| 100 | 48 | 96 | |
| 30 min | 1 | 0.24 | 0.48 |
| 10 | 2.4 | 4.8 | |
| 50 | 12 | 24 | |
| 100 | 24 | 48 | |
| 60 min | 1 | 0.12 | 0.24 |
| 10 | 1.2 | 2.4 | |
| 50 | 6 | 12 | |
| 100 | 12 | 24 |
Once the barrel is formed, a typical launch sequence is:
EMU launcher projectiles are implemented as iron shells filled with compacted lunar regolith. Lunar mare soils contain metallic iron grains and iron-bearing minerals that can be magnetically separated and melted using solar or resistive furnaces. This provides a scalable, fully in-situ metal supply for projectile casings.
Once captured in orbit, iron shells are treated as standard logistics units rather than expendable hardware:
The same iron-shell architecture can be applied at other low-gravity bodies (e.g. Ceres, icy moons) using locally produced metal casings. Where convenient, outbound miners can collect shells staged in orbit on the way to their destination, or deposit shells in staging orbits for later reuse.
The EMU launcher uses a deep, ice-supported bore as a natural pressure vessel. At depth, ice and ice-rich regolith remain stable for geological timescales due to low temperatures and shielding from direct vacuum. Sublimation becomes significant only in the final section near the surface, where the barrel opens to space and is exposed to solar heating.
Only the last ~0.5–1.0 m near the surface requires special treatment to control sublimation and erosion. This region is implemented as a hard, non-volatile throat:
To further suppress sublimation and protect the throat, the launcher mouth is covered when not firing:
By combining a deep, ice-supported barrel with a short, replaceable hard liner and a simple surface cover, the EMU launcher maintains long-term structural stability while minimising sublimation and erosion effects at the surface interface.
The EMU launcher feeds SLPA’s orbital depots:
It requires only local materials and sunlight.
This system closes SLPA’s logistics loop:
The EMU launcher is not limited to vertical shafts or flat terrain. Its geometry can be adapted to the environment and mission profile.