ZENIT Space · Qi Vanguard Fleet

Outverse Shield

Zorak’s three-layer shield concept pairs an outer burst reserve with SERAT heat recovery and inner hull damage mapping. The simulations show where the energy goes during a strike and what it takes to respond again.

Three-layer concept
Zorak’s three shield layers An outer protection layer, a middle load and recovery layer, and an inner hull-sensing layer surround Zorak. The arrows illustrate a reference debris rebound at the outer boundary. L3 · PROTECTION L2 · RECOVERY L1 · HULL MAPPING INBOUND REBOUND ZORAK
Three functional layers. The dotted amber ring represents the hull sensors.

Reference strike · Meteoroid debris

One fragment, three energy figures

In the earlier ZENIT debris simulation, a 41 g fragment reached the shield at 620 m/s. The modeled response sent it outward at 310 m/s after a 12 ms interaction.

Incoming kinetic energy
7.88 kJ
Removed from its motion
5.91 kJ
Carried outward
1.97 kJ

75% removed25% carried away by the rebound

Over 12 ms, the rate of energy removal averaged 493 kW. That figure describes the change in the fragment’s kinetic energy.

01 · Solid impacts

From a single projectile to a cloud

These comparisons use the earlier model’s limits of 5.91 kJ of energy removal and 38.1 N·s of impulse for one fresh sector. The sector upgrade uses higher trial limits.

Earth benchmark

.50-caliber M33 round

887 m/s at the manufacturer’s reference condition. Source 1

Incoming kinetic energy
16.85 kJ
Energy removed
5.91 kJ
Energy still inbound
10.94 kJ

35.1% removed. The round continued inward at about 715 m/s in the head-on case.

Earth benchmark

Intact 155 mm M795 shell

46.7 kg at an assumed arrival speed of 800 m/s. Source 2

Incoming kinetic energy
14.950 MJ
Energy removed
5.91 kJ
Energy still inbound
14.944 MJ

0.040% removed. The shell continued inward at about 799.84 m/s in the head-on case.

Illustrative burst case

Ten simultaneous fragments

Ten copies of the reference fragment reaching the same sector together.

Incoming kinetic energy
78.80 kJ
Energy removed
5.91 kJ
Energy still inbound
70.92 kJ

7.5% removed. A focused response turned back one fragment out of ten. It carried 1.97 kJ outward.

Energy removedCarried outwardStill inbound

A burst from the TNT-filled M795 releases about 45 MJ at the source. The load at Zorak would depend on the mass, speed and arrival pattern of the fragments that cross its path. Point defence is assessed by how much of that material still crosses the hull’s path after interception. Sources 2–3

02 · Radiation and directed energy

Where radiation energy goes

The field-only simulation assigns zero attenuation to photons and neutrons. The material and charged-particle examples show separate physical effects under stated assumptions.

Illustrative material layer

X-ray and gamma-ray pulse

Each test sends 1,000 J/m² of radiation toward a reference layer of aluminum with an assumed areal mass of 1 g/cm². The results use NIST photon interaction data. Source 4

Photon energy at the layer
RadiationRemoved from direct beamEnergy straight throughEstimated heat
10 keV X-rays>99.99%<0.01 J/m²970 J/m²
100 keV X-rays15.7%843 J/m²35 J/m²
1 MeV gamma rays6.0%940 J/m²26 J/m²

Energy removed from the direct beam can be scattered or deposited in the layer. The heat column estimates deposition from the direct beam.

Optical example

HELIOS laser

A one-second pulse at the 60 kW benchmark emits 60 kJ. For every 1,000 J/m² that reaches an assumed opaque surface with 90% reflectivity, 900 J/m² is reflected and 100 J/m² heats the surface. Source 5

90% reflected10% heat

Charged-particle example

Solar and cosmic protons

In a separate example with an assumed transverse magnetic field integral of 1 T·m, a 100 MeV proton turns about 39° and a 1 GeV proton turns about 10°. Their kinetic energy stays the same in this magnetic-only model. Source 6

A 15 kt nuclear detonation represents about 63 TJ of total source energy. To estimate protection at the ship, the model would need the arriving photon and neutron spectra and their transport through the vessel’s material layers. Yield source

03 · Shield architecture

How the three layers work

  1. L3 · OuterProtection

    GENI-10 manages first contact and uses a dedicated burst reserve to redirect debris within the sector’s response limits.

  2. L2 · MiddleLoad and recovery

    Distributes the response load and transfers heat through a dedicated SERAT buffer. The Field Compression Monitor tracks temperature, leakage and reserve during recovery.

  3. L1 · InnerHull damage mapping

    Compares hull sensor readings before and after a strike to locate regions that need inspection.

What the hull map shows

NEXUS marks the location of a suspected impact or damage and the reading that raised the flag. Regions with missing readings show as unassessed. Inspection confirms whether a flagged region is damaged. Spacecraft impact-sensing reference

Earlier reference case for a degraded sector

When the trial energy and impulse limits are both reduced to 50%, a following M33 hit loses 2.96 kJ, or 17.5% of its incoming kinetic energy. It continues inward at about 805 m/s. The reduction is an imposed test condition.

04 · Fleet qualification map

3 × 5 function map

The Qi Vanguard Fleet assigns five functions to each of the three main Outverse layers. The checks below define what a test should demonstrate for each of the 15 functions.

L3 · Outer

Protection

Function and jobPass check
L3.1 First contactIdentify the incoming track, first contact time and shield sector.Replay a known trajectory across sector boundaries and recover the correct first contact sector and time within the test tolerances.
L3.2 Sideways steeringRedirect the trajectory when there is room for a clear pass.Verify that the outgoing track meets the specified clearance from the hull and nearby vessels within the sector’s impulse allowance.
L3.3 BrakingReduce incoming speed within the available work and impulse limits.Reconcile the measured or modeled change in kinetic energy with the braking ledger and verify that the response stays within its work and impulse limits.
L3.4 Rebound controlControl and verify outward motion after braking.For the half-speed reference case, verify the outward direction and final speed. A full rebound requires enough work, impulse and thermal headroom.
L3.5 Residual debris handlingTrack the fragments that continue toward the vessel after the field response.Account for every fragment in the ten-fragment replay and report the count and kinetic energy still inbound.

L2 · Middle

SERAT load and recovery

Function and jobPass check
L2.1 Load distributionAllocate the response across the affected sectors.Apply simultaneous loads to neighboring sectors. Verify that each allocation fits its local limits and the vessel’s shared power and cooling budget.
L2.2 Transient energy handlingRoute braking work, outward push work and losses to their respective paths.Reconcile the full-capacity reference ledger of 20 kJ taken out during braking, 5 kJ returned to outward motion and 15 kJ net removed. Track heat separately.
L2.3 Heat bufferingHold deposited heat within the active sector’s available thermal headroom.In the higher-heat model, accept a 23 kJ pulse into a fresh 25 kJ buffer and withhold a full response when a subsequent pulse would exceed that capacity.
L2.4 CoolingTransfer buffered heat into the SERAT cooling path between strikes.Run the full-capacity one-second repeat-strike case at the 25 kW per-sector target and verify that buffer load stays within 25 kJ over all 120 pulses.
L2.5 Sector isolation and recoveryIsolate a degraded sector and restore it when its health and allowances recover.Inject a sector fault. Verify isolation and continued hull reporting, then verify that full response resumes only after the sector passes its health, work, impulse and thermal checks.

L1 · Inner

Hull damage mapping

Function and jobPass check
L1.1 Impact locationPlace detected hull contacts on the vessel map.Inject contacts at known hull positions and verify the reported sectors and location error against the test tolerances.
L1.2 Strain sensingCompare structural readings before and after a strike.Inject a known local strain change and verify that the correct hull region is flagged for inspection against its calibrated baseline.
L1.3 Thermal sensingLocate abnormal hull heating.Replay a localized temperature rise with normal system heating present and verify that the map identifies the affected region.
L1.4 Leak detectionLink a pressure anomaly to the relevant compartment and hull region.Inject a leak indication and normal pressure changes in separate cases. Verify that the indicated compartment is flagged and the normal case is classified correctly.
L1.5 Damage mapping and confidenceCombine the readings into a map with an evidence status for each region.Replay normal, anomalous and missing readings. Verify that the map distinguishes no change detected, inspect and unassessed. Confirmed damage requires inspection evidence.

Compare any proposed physical sublayer on the same vessel with the same strike conditions, power allocation and cooling budget. Advance it only if the test shows more debris clearance, shorter recovery or more accurate hull damage localization within the shared sector targets.

05 · Approved concept targets

Burst reserve and SERAT recovery

The approved Zorak revision gives each active sector a short-burst reserve and a separate thermal buffer. The figures below define the single-sector simulation targets.

L3 · Outer protection

Reserve for a fresh sector

Net energy removal per pulse
15 kJ
Impulse per pulse
80 N·s
Braking work before rebound
20 kJ
Modeled recovery of energy and impulse allowances
1 s

Braking work tracks how much kinetic energy the field handles on the way to zero speed. Net removal accounts for the energy carried back out by a rebound.

L2 · SERAT

Heat handling per active sector

Usable heat-buffer capacity
25 kJ
Effective cooling rate
25 kW
Heat from a full-capacity test pulse
23 kJ
Buffer headroom at peak test load
2 kJ

The higher-heat test converts all braking work to heat and adds losses equal to 20% of net energy removal. A full pulse therefore adds 20 kJ of braking heat and 3 kJ of assumed losses.

Repeated strikes in one sector, with up to 120 pulses per run
Strike and intervalCoolingComplete pulses before the first limit
Full-capacity strike every 1 s25 kW120 of 120
Full-capacity strike every 1 s20 kW1 of 120. The second would put 26 kJ into the 25 kJ buffer.
M33 round every 0.85 s25 kW120 of 120
M33 round every 0.80 s25 kW4 of 120. The net energy allowance ran short on the fifth hit.
Two reference debris fragments every 0.90 s25 kW1 of 120. The impulse allowance ran short on the second pulse.

In the single-hit trial, the fresh reserve rebounded the M33 round at about 444 m/s and turned back two of ten reference debris fragments arriving in one sector. The intact M795 benchmark continued inward at about 799.60 m/s.