How it works

Operating cycle

How StarRoad proceeds from launch preparation to orbital operations, landing and servicing.

Preparation Launch chamber Preparing the shuttle, accelerator, gateway and magnetic levitation. Expand stage

The loaded shuttle is placed in the launch chamber near Batanga. Its onboard systems are tested first, followed by the accelerator systems and a pre-launch test of the gas-dynamic gateway. The onboard superconductors are energised, magnetic levitation is started and checked, and the tunnel is evacuated. On command, pulsed power begins flowing to the accelerator's initial segments.

Acceleration Evacuated maglev tunnel Accelerating to about 11 km/s while transitioning from 4g to inertial motion. Expand stage
  • 0–330 km. Initial longitudinal acceleration is about 4g. A substantial share of the energy supports levitation and overcomes gravity.
  • 330–about 1,800 km, the descending part of the S-curve. Longitudinal acceleration falls smoothly from the initial 4g to zero. The shuttle follows the underground curves under loads of up to about 4g, while surrounding electromagnetic elements stabilise its path.
  • About 1,800–2,050 km, the ascending part of the S-curve. Acceleration falls to zero as the gateway approaches. The shuttle coasts at about 11 km/s for the final 50 km.
StarRoad acceleration profile: acceleration, velocity and elapsed time along the route
StarRoad acceleration profile: acceleration, velocity and elapsed time along the route.
Gateway Vacuum-to-atmosphere transition Sequential activation of the gas-dynamic barrier and mechanical closure. Expand stage

Because the launch point is high, the shuttle is already more than 10 km above sea level about 30 km from the gateway, minimising the shock wave's effect on the surrounding area. The gateway belts are test-fired one minute before the shuttle launches, without opening the mechanical closure. After the shuttle has covered 45% of the tunnel, compressed air accumulated while the last tunnel section was evacuated is released through the gateway belts as a supersonic flow. About 10 seconds before passage, hydrogen is supplied and the gas-dynamic barrier enters its main combustion mode, producing a stable conical supersonic flow of hot, partially ionised gas. Three seconds after successful belt activation and formation of the hot barrier-gradient cone, the mechanical closure opens.

The barrier also prevents loss of tunnel vacuum and moderates the initial thermal shock. In milliseconds, the shuttle crosses the prepared zone of rarefied, heated gas. This key technology changes the timing of the first aerodynamic load by removing the ultrashort shock front that would otherwise occur when the medium changes.

The gas-dynamic barrier does not reduce total aerodynamic forces. It shifts the shock load from the microsecond to the millisecond range, critically reducing local stresses, vibration and thermal shock in the shuttle structure.

The mechanical closure shuts immediately after the shuttle passes, and the jet belts are switched off at once.

Atmosphere Penetrating the dense layers Ballistic atmospheric flight with the highest loads in the first seconds. Expand stage

Following a ballistic path, the shuttle uses its inertial mass and strong structure to penetrate the dense atmosphere. Peak thermal and dynamic loads occur in the first 10–20 seconds.

Essential clarification. On leaving the gas-dynamic barrier, the shuttle immediately interacts with the normal atmosphere at the specified altitude, about 3,400 m. All trajectory, heat-flux and load calculations assume full aerodynamic interaction with the atmosphere; they do not assume a “gas shield”, a “channel” or an accompanying rarefied volume.

AstroLiner mechanical and thermal loads over time and altitude
Mechanical and thermal loads over time and altitude for Cd = 0.08–0.12.
Orbit Reaching space and orbital operations Rejecting heat, correcting the trajectory and deploying the payload. Expand stage

After leaving the atmosphere, the radiators unfold to reject heat. The shuttle then activates its onboard electromagnetic plasma drives for fine trajectory correction and insertion into the target orbit, often directly beyond geostationary orbit or towards a Lagrange point. The payload is deployed. In the AstroLiner-S configuration, final insertion and orbital correction use the chemical propulsion system.

Return Leaving orbit Braking and trajectory correction according to the shuttle version. Expand stage

The full AstroLiner uses electromagnetic plasma engines to leave orbit. In the AstroLiner-S configuration, the chemical propulsion system performs deorbit braking, corrections and final manoeuvres.

Landing Ocean landing Parachute braking, splashdown and transition to marine operation. Expand stage

Over the Atlantic near Gabon, the braking parachute system is deployed to reduce speed. The shuttle lands at a low angle of attack on its reinforced underside, designed for contact between a heated surface and cold water. Propellers or waterjets deploy after splashdown.

Servicing Towing and preparation for the next voyage Return to port, inspection, thermal-protection repair and scheduled work. Expand stage

The shuttle's own drives, powered by its onboard reactor, or standby tugs if the shuttle systems malfunction, take it to the port complex for inspection, servicing, thermal-protection repair and preparation for the next voyage. AstroLiner-S returns to port using batteries, an auxiliary power unit or standby tugs.

Direct-departure logic

StarRoad is not designed around a mandatory stop in low Earth orbit. Its basic idea is to use the initial kinetic energy to send cargo directly towards high-energy orbits and Lagrange points, reducing the need for a chain of refuelling stops, towing operations and multiple rocket launches.