NOAH Quantum Propulsion System

NOAH Quantum Propulsion System
A resonant-cavity, Casimir-assisted photon thruster concept built on an asymmetric truncated-cone cavity geometry combined with quantum-material engineering. Every component needed to operate and measure the device is identified; the RF dimensions that depend on simulation stay parametric until then.
Measured: TBD
* Withdrawn thrust/Isp figures & corrections: Physics tab. Full ΔF definition, uncertainty budget & blind protocol: V1 Prototype tab.
What NOAH-QPS is
A quantum-effect spacecraft propulsion concept, code-named "Noah's Ark," released as a public-domain theoretical concept whose central claim — a measurable net thrust — is still an open question awaiting the V1 differential-force test, not an established performance figure.
"We don't claim the effect exists. We built the instrument to determine whether it does." NOAH-QPS V1 is not sold as a thruster with a performance sheet — it is a differential force-measurement rig designed to either produce a reproducible, artifact-checked ΔF, or to rule the effect out. See V1 Prototype → Defining and validating ΔF for the full protocol.
- System: NOAH-QPS (NOAH Quantum Propulsion System)
- Origin: a fusion of an asymmetric truncated-cone resonant-cavity thruster concept (Shawyer, 2006) and the ArkCore quantum-material concept by Noah Kouadri Khazar
- Developer: open-source, public domain
- Status: theoretical concept, simulation-validated
"Respect the known laws of physics, but explore the limits of what is achievable with current and emerging technology."
Does not violate: conservation of momentum, the first law of thermodynamics, or general/special relativity.
Does exploit: photon radiation pressure, resonant (Q-factor) amplification, static & dynamic Casimir effects, and quantum materials (superconductors, topological insulators).
Design lineage
From Shawyer's 2006 proposal: the asymmetric truncated-cone resonant cavity that amplifies electromagnetic effects. From ArkCore: the integration of quantum physics, the Casimir effect, and advanced materials (superconductors, metamaterials). NOAH-QPS keeps that cavity geometry while replacing the unphysical thrust claims later made about it with mechanisms that are measured and reproducible in the lab today.
The four mechanisms at work
Every force in NOAH-QPS traces back to measurable physics: momentum carried by light, resonant amplification of that momentum, and the quantum vacuum pressure between conducting surfaces.
- The 6.67 mN figure is withdrawn. It came from F = Q·P/c, which is not a general thrust law for a resonant cavity. A high Q raises the energy stored per watt dissipated; it does not automatically multiply net photon thrust by Q.
- The static Casimir force is an internal force, not net external thrust. A Casimir force between two elements inside a closed system can be perfectly real without producing any net acceleration of the system's center of mass on its own.
- The dynamic Casimir effect is an experimental hypothesis here, not an acquired thrust source. Photon-pair generation from a modulated boundary is real and measured (Wilson et al. 2011), but its use as a propulsion mechanism is speculative and unproven.
- Q > 10,000 is a design target, not a guaranteed spec. It must be computed by EM simulation and then confirmed by measurement (S₁₁, ring-down) — never assumed.
- The cavity geometry (Ø160 → Ø60 mm, L = 150 mm) is not frozen. Every dimension that sets f₀, the mode, Q, and the coupling coefficient stays parametric until EM simulation converges on it.
- The waveguide callout was wrong. WR-284 is specified for roughly 2.60–3.95 GHz. At 2.45 GHz the correct part is WR-340 (2.20–3.30 GHz band).
- The measurement rig is arguably the most important part of the prototype. TU Dresden's experimental work (Kraft et al., 2021) shows thermal effects, center-of-gravity shifts, mechanical strain, and cable interactions can all produce false signals that look exactly like thrust.
- The only figure of merit that matters in the end is ΔF = F_meas − F_conventional, reported with its full uncertainty budget — exactly as the engineering dossier (see V1 Prototype tab) requires.
3.1 Photon radiation pressure
A photon of frequency ν carries energy E = hν and momentum p = E/c. Reflecting off a perfect mirror, it transfers momentum 2p to that surface.
Example: P = 100 W, R = 0.999 → F ≈ 6.67 × 10⁻⁷ N (0.667 µN)
3.2 Resonant-cavity amplification — corrected
A high quality factor Q means a cavity stores much more electromagnetic energy per watt of continuous dissipation — that part is standard microwave engineering. It does not follow that net photon thrust scales linearly with Q. Treating F = Q·(1+R)·P/c as a thrust law double-counts the same photons on every round trip instead of tracking net momentum delivered to the outside world.
Any genuine net thrust would have to come from an asymmetry between the momentum flux striking the two end walls of the cavity — the same claim made about earlier asymmetric-cavity thruster proposals, and that subsequent testing (White et al. 2016 in vacuum; Kraft et al. 2021 at TU Dresden) failed to confirm once thermal and mechanical artifacts were controlled for. NOAH-QPS treats this as an open experimental question, to be settled by the differential ΔF measurement described in the V1 Prototype tab — not assumed.
3.3 Static Casimir effect — internal force, not net thrust
Between two parallel conducting plates separated by distance d, quantum vacuum fluctuations generate a real, measurable attractive force. This has been confirmed experimentally (Lamoreaux 1997) and is not in question.
Example: d = 1 µm, A = 1 mm² → F ≈ 1.3 × 10⁻¹² N (1.3 pN)
Correction: if both plates are internal parts of the same closed system, this is an internal force pair — by momentum conservation it cannot, by itself, accelerate the system's center of mass. It could only contribute to net thrust if coupled to something that carries momentum away from the system (e.g. emitted photons), which has not been demonstrated here.
3.4 Dynamic Casimir effect — an experimental hypothesis, not a thrust source
If one plate oscillates at high (GHz) frequency, the quantum vacuum generates real photon pairs — this phenomenon itself is experimentally confirmed (Wilson et al., Chalmers, 2011).
Correction: that confirmation is for photon-pair production in a superconducting circuit, not for propulsion. Using the dynamic Casimir effect as a thrust mechanism in NOAH-QPS is a hypothesis to be tested, not a validated contribution to be added into a performance budget.
3.5 Quantum materials
Superconductors — Type I (Pb, Hg, T꜀ < 10 K) and Type II (Nb-Ti 9.2 K, Nb₃Sn 18 K, YBCO 92 K), used for ultra-low-loss cavities (Q > 10⁹).
Metamaterials — sub-wavelength structuring, possible negative refraction, used to control electromagnetic wave propagation.
Topological insulators — conductive surface, insulating bulk; used as an internal cavity coating to shield against parasitic interactions.
Reading the 3D model
Toggle Labels and Exploded view on the model above to see how these seven subsystems fit together.
- Industrial magnetron, 2.45 GHz
- 100–1000 W, modulable, ~70% efficiency
- Frequency stability ±1 MHz
- 3–5 kV supply, forced-air or liquid cooled
- Rectangular WR-340 waveguide, 86.36 × 43.18 mm — covers 2.20–3.30 GHz, correct for a 2.45 GHz source (WR-284 is rated ~2.60–3.95 GHz and was mis-specified in an earlier draft)
- Conical impedance-matching taper
- OFHC copper or aluminum, Ra < 0.4 µm finish
- Truncated cone, parametric geometry — a starting point near Ø160 mm → Ø60 mm, ~150 mm long is used for illustration only; D, L, wall thickness and taper angle stay open until EM simulation fixes f₀, the mode, Q and the coupling coefficient
- OFHC copper (>99.99% pure) + 5–10 µm silver coating + 0.1 µm gold anti-oxidation layer
- Simulation target Q > 10,000 (to be confirmed by S₁₁ / ring-down measurement, not assumed) · candidate modes TE011 (primary), TE012, TM010
- Mobile mirror: SiN MEMS membrane, 1×1 mm, piezo-actuated, 1–10 nm amplitude
- He3/He4 dilution refrigerator, base temp 10–50 mK
- >100 µW cooling power at 100 mK
- ~500 kg, ~1.5 L He3/day consumption
- Target pressure < 10⁻⁹ mbar
- Turbomolecular + cryo + ion/getter pumping stages
- 316L stainless steel, ConFlat metal seals
- FPGA (Xilinx Zynq-7000 class) for RF generation, acquisition, PID
- PLL frequency lock, <1 Hz precision on 2.45 GHz
- Cernox/RuO2 thermometry, optical-torsion force balance (1 pN), SNSPD photon detector
[G] External housing & structure
Aluminum 6061-T6 or CFRP composite shell, copper-mesh Faraday cage EMI shielding, glycol-water cooling loop and radiators, vacuum-tight SMA/BNC/D-sub feedthroughs. Propulsion module: ~50–100 kg, 500×500×400 mm (excluding cryostat).
Engineering data
Worked calculations for the cavity's resonant frequency and quality factor, the bill of materials, fabrication steps, and the four control loops that keep the system stable.
5.1–5.2 Resonance & quality factor
These are the two numbers the whole design pivots on, and neither is fixed yet — they fall out of whatever cavity dimensions the EM simulation converges on.
Illustrative only: a = 55 mm, L = 150 mm → f ≈ 2.45 GHz. This a, L pair is a starting point for the simulation sweep, not a frozen dimension.
Illustrative only: OFHC copper, σ = 5.96 × 10⁷ S/m, V/S ≈ 0.020 m → Q ≈ 10,760. This suggests the >10,000 target is reachable for this class of geometry — it is not a guaranteed result, and must be confirmed by S₁₁ / ring-down measurement on the built cavity.
5.5 Thermal budget
Continuous dissipated power in the cavity reaches ~1000 W once the Q-factor amplification is included — far beyond what a milliwatt-class dilution cryostat can absorb continuously.
Solution — pulsed operation: 1 ms pulses every 10 s (duty cycle < 0.01%) brings average dissipation down to ~1 W, within the cryostat's budget.
6 Bill of materials
| Component | Material | Specification |
|---|---|---|
| Resonant cavity | OFHC copper (C10100) | σ > 5.96×10⁷ S/m, purity >99.99% |
| Internal coating | Silver (Ag) | 5–10 µm, σ = 6.30×10⁷ S/m |
| Surface protection | Gold (Au) | 0.1 µm, anti-oxidation |
| MEMS membrane | SiN | 1 µm thick, E = 250 GPa |
| Actuator | PZT ceramic | d₃₃ ≈ 300 pm/V, ±100 V |
| Superconducting option | Nb-Ti / YBCO | T꜀ = 9.2 K / 92 K |
| Structure | Al 6061-T6 | σᵧ = 276 MPa, 2.70 g/cm³ |
6.2 Fabrication sequence
- Machining — 5-axis CNC, ±10 µm tolerance, electrolytic polish to Ra < 0.4 µm
- Coating — electroless/electrolytic silver then gold plating, SEM-verified
- MEMS fabrication — photolithography, LPCVD SiN, RIE etch, KOH sacrificial release
- Assembly — Cu-Cu laser welding or brazing, plasma + ultrasonic cleaning
- Testing — vacuum, RF (VNA), thermal cycling 300 K → 10 mK → 300 K, force calibration
7 Control loops
| Loop | Sensor | Actuator | Performance |
|---|---|---|---|
| Temperature | Cernox thermometer | Heaters + cryostat | ±0.1 mK at 10 mK |
| Vacuum pressure | Ion gauge | Piezo valves + pumps | ±10%, <5 s response |
| Frequency lock | Phase detector | Magnetron control voltage (PLL) | <1 Hz on 2.45 GHz |
| MEMS mirror position | Capacitive electrodes | PZT ±100 V | <1 nm resolution |
What the numbers say
The original performance table was built on the withdrawn F = Q·P/c estimate. It is replaced here with a status table: what's measured physics, what's an internal force, what's a hypothesis, and what can only be answered by the V1 differential test.
| Parameter | Status | Note |
|---|---|---|
| Net photonic thrust | Unconfirmed | Depends on wall-asymmetry momentum transfer — not on Q; to be measured as ΔF |
| Static Casimir contribution | Internal force | ~1.3 pN between internal plates (1 µm gap, 1 mm²) — real, but not net external thrust by itself |
| Dynamic Casimir contribution | Hypothesis | Photon-pair production is confirmed physics; its use as thrust is untested here |
| Specific impulse (Isp) | Not computable yet | Requires a confirmed net thrust value, which does not currently exist |
| Electrical consumption | Specified | 100 W RF input (design parameter, independent of the thrust question) |
| Mass (propulsion module / cryostat / total) | Estimated | 50–100 kg / ~500 kg / ~600 kg |
| ΔF = F_meas − F_conventional | To be measured | The one number the V1 rig exists to produce, with its full uncertainty budget |
Why there's no energy-balance or Δv figure here
Efficiency, acceleration and Δv were previously computed from the retracted thrust figure and are removed for the same reason — they would just propagate the same error one step further. Those numbers can be recomputed honestly the moment V1 produces a measured, artifact-checked ΔF.
9 How it compares — with the open question flagged
| Parameter | NOAH-QPS | Asymmetric RF-cavity concept (historical) | Ion (Xe) | Chemical |
|---|---|---|---|---|
| Thrust | Unconfirmed (pending ΔF) | 0 (debunked) | 0.1–5 N | 10³–10⁶ N |
| Isp | Not computable yet | N/A | 2000–5000 s | 300–450 s |
| Power | 100 W | N/A | 1–10 kW | N/A |
| Efficiency | Not computable yet | N/A | 50–80% | 30–50% |
| Status | V1 experimental prototype | Refuted (thermal/mechanical artifacts) | Operational | Operational |
- Potentially very high Isp
- No propellant consumed
- No moving-part wear at the macro scale
- Electromagnetically silent (no plasma jet)
- Any real thrust is expected to be very small (mN or below)
- Heavy — dominated by the cryostat mass
- Extreme complexity (vacuum, cryogenics, control)
- High cost; lifetime limited by He3 supply
What still has to be solved
1 · Thermal losses in the cavity
~1000 W of dissipation in pulsed operation must be removed without disturbing vacuum or temperature. Approach: very-low duty-cycle pulsing, thermal conduction to the cryostat, high-conductivity materials (diamond, graphene), superconducting low-loss coatings.
2 · Vacuum stability
Ultra-high vacuum (<10⁻⁹ mbar) must be held for years in orbit. Approach: integrated ion pump, Ti/Zr getters, low-outgassing 316L steel and OFHC copper, elastomer-free ConFlat seals.
3 · MEMS mirror alignment
The mirror must track nanometre-scale precision relative to the cavity. Approach: active PID control, capacitive sensing, electrostatic + PZT actuation, thermal-expansion compensation.
4 · Helium-3 consumption
He3 is scarce and costly (~$1000/L). Approach: recovery/recycling loops, adsorption cryocoolers as a He3-free alternative, or long-term migration to high-T꜀ superconductors (YBCO, 92 K) that skip dilution refrigeration entirely.
11 Test protocol
| Stage | Test | Goal |
|---|---|---|
| Ground | RF characterization | Measure Q, verify resonant modes (VNA) |
| Ground | Vacuum test | Leak check, verify final pressure |
| Ground | Cryogenic test | Cool to 10 mK, verify thermal stability |
| Ground | Force test | Optical torsion balance, 1 pN sensitivity |
| Vacuum chamber | Simulated microgravity | Drop tower, ~10 s free fall |
| Flight | Suborbital flight | Sounding rocket, ~5 min microgravity |
| Flight | Orbital mission | CubeSat (3U/6U), months-long orbit-correction test |
From engine concept to measurable instrument
At this stage NOAH-QPS V1 is best described as a complete experimental prototype, not yet a qualified propulsion engine. Every component needed to operate the device and to measure it is identified; the RF dimensions that depend on electromagnetic simulation stay parametric. The goal of V1 is not to build something that produces thrust — it is to build an instrument that can cleanly prove or disprove the existence of a residual force. Toggle V1 test rig and Show reference module on the 3D model above to see the differential-test hardware described below.
Core uncertainty metric
The central quantity of the whole program is the differential force, budgeted against thermal, mechanical, RF, calibration, model, and environmental error sources:
A candidate signal only counts as real if it is reproducible, correlated with the RF excitation, survives artifact controls, and remains after every conventional transfer mechanism has been closed out.
General architecture — two coupled chains
- RF source → amplifier
- Directional coupler (forward/reflected)
- Coupler into the resonant cavity
- QPS interaction module (swappable)
- Force, temperature, acceleration
- RF forward / RF reflected, voltage, current
- Magnetic field, pressure
- → synchronized DAQ → ΔF(t)
It's this separation — a drive chain and an independent, fully-synchronized measurement chain — that turns NOAH-QPS from "just an RF cavity" into a genuine experimental platform.
1 · Mechanical subsystem
| ID | Component | Function |
|---|---|---|
| MC-001 | Cavity main body | Primary mechanical & electromagnetic enclosure. OFHC copper recommended; parametric cylindrical geometry — diameter, length, wall thickness and finish are not frozen yet, they follow from the target mode and frequency. |
| MC-002 | Front flange | Cavity closure, mechanical interface, optional coupler feedthrough, instrumentation access |
| MC-003 | Rear flange | Closure, stiffening, instrumentation interface, mechanical symmetry |
| MC-004 | External structure / support | Holds the cavity, transmits force to the measurement system, suppresses parasitic motion (Al, stainless, or low-expansion alloy per thermal analysis) |
2 · RF subsystem
| ID | Component | Function |
|---|---|---|
| RF-001 | RF source | Generates the excitation — frequency, power, frequency/phase stability, phase noise, 50 Ω impedance. A controllable commercial source is preferred over a custom generator for V1. |
| RF-002 | RF amplifier | Raises source power to P_RF; enables power sweeps (0, 1, 5, 10, 20, 50, 100 W). Real maximum power is set after thermal/electrical analysis. |
| RF-003 | Isolator / circulator | Protects the source, absorbs or redirects reflected power, stabilizes the setup |
| RF-004 | Directional coupler | Separately measures P_forward and P_reflected — the only way to know actual injected RF power |
| RF-005 | 50 Ω dummy load | Verifies the measurement chain produces no artificial signal when the cavity isn't excited |
| RF-006 | RF coaxial cabling | 50 Ω, known length, documented mechanical routing — not a mere accessory: cable routing can itself introduce a parasitic mechanical or electromagnetic force (cable "recoil" is flagged as an audit item) |
| RF-007 | Cavity coupler | Magnetic loop, electric probe, iris, or waveguide. Position, area, offset, angle and coupling coefficient β must come from EM simulation, not be assumed. |
3 · QPS core & the differential test
QC-001 — Resonant cavity: the electromagnetic heart of the prototype, characterized by f₀, Q₀, Qₗ, β, S₁₁ and the field distributions E(r), B(r). Simulation must identify the dominant mode before final fabrication.
QC-002 — QPS interaction region: currently the hypothetical part of the system. No new physics is assumed here — it is treated as an interchangeable module (configuration A, configuration B, or reference), which makes possible the single most important test in the program:
If the signal disappears when the module is swapped for a geometrically-equivalent dummy, that is a major experimental result on its own.
QC-003 — Reference element (mandatory in V1): same mass, same external geometry, same mounting, but deliberately different or controlled RF properties. Combined with the cavity and a dummy load, this yields four clean test conditions:
| Test | Configuration |
|---|---|
| Test A | QPS module installed |
| Test B | Reference (twin) module installed |
| Test C | Cavity alone, no module |
| Test D | RF dummy load, cavity bypassed |
This four-way comparison is far more powerful than a simple on/off thrust measurement.
4 · Thrust measurement system
| ID | Component | Notes |
|---|---|---|
| MM-001 | Force sensor | Measures F_meas(t). Exact choice depends on prototype mass and required sensitivity. A ~0.1 µN resolution is a target spec, not a guaranteed performance. |
| MM-002 | Suspension | Torsion pendulum or flexible mount, low friction, with known natural frequency f_mechanical and damping ratio ζ, both characterized |
| MM-003 | Reference structure | Mechanically isolated from the bench as much as possible |
4.1 · Defining and validating ΔF
ΔF is only a meaningful result if F_conventional and F_measured are each independently defined, and if the gap between them survives a real uncertainty budget. This is the part of the dossier a propulsion or instrumentation reviewer will check first.
F_conventional — the modeled baseline. Before anything is called anomalous, every known, non-exotic contribution that could load the sensor is estimated and summed:
- F_thermal — force-equivalent of structural expansion / center-of-mass shift, from the TH-001 ΔT(t) array and the structure's known CTE
- F_leakage — radiation pressure from any RF field leaking onto the enclosure, from SH-001 shielding effectiveness plus a leakage measurement with the cavity de-tuned
- F_cable — recoil / Lorentz force from current-carrying RF-006 cabling near the suspension, characterized with a cable-only excitation test (RF into the dummy load, cavity disconnected)
- F_vibration — apparent force from facility or pump-induced vibration, from ENV-001: F_vib = m·a
- F_buoyancy — convective/buoyancy loading in atmosphere, eliminated once V1.1's vacuum chamber (VAC-001) is in place
- F_magnetic — torque/force from ambient or induced magnetic fields, from ENV-003
F_measured — the raw reading. Read from MM-001, after deconvolving the MM-002 suspension's own mechanical transfer function, synchronized to the RF-004 forward/reflected power trace on the DAQ-002 common time base.
| Uncertainty source | Type | Mitigation |
|---|---|---|
| Sensor noise / resolution | A (statistical) | Signal averaging, lock-in detection synced to RF chop frequency |
| Sensor calibration & linearity | B (systematic) | Traceable calibration via electrostatic comb actuator or calibrated micro-mass |
| Thermal drift | B | TH-001 array + subtraction of the modeled F_thermal(t) |
| Mechanical vibration | A/B | ENV-001 accelerometer-derived correction, vibration-isolated bench |
| RF leakage / EM coupling | B | SH-001 shielding + leakage characterized with cavity de-tuned |
| Cable coupling | B | Fixed, symmetric, damped routing; verified via dummy-load-only run |
| Environmental (pressure, B-field) | B | ENV-002/003 logging and subtraction |
| Calibration-standard traceability | B | Calibration source itself independently certified |
Calibration & run procedure
- Baseline / zero — Test D (dummy load, RF off): establish the noise floor and sensor offset over an extended quiet period.
- Calibrated force injection — apply a known force (electrostatic comb or calibrated small mass) to confirm sensor gain and linearity in physical units.
- Sham RF run — Test D at full RF power into the dummy load, identical cabling: isolates cable-recoil and RF-leakage artifacts before any module is installed.
- Reference run — Test B (reference twin installed): sweep RF power (0–100 W) to build the F_conventional(P) curve for this exact geometry.
- QPS run — Test A (QPS module installed): repeat the identical sweep and protocol.
- Compute ΔF(P) = F_meas,A(P) − F_meas,B(P), propagate every uncertainty term above, and repeat the full A/B/C/D cycle across independent sessions.
Blind / sham protocol
- Module identity (QPS / reference / dummy) is concealed from the operator running the DAQ during a session; only an independent recordkeeper logs which configuration was tested
- Test order (A/B/C/D) is randomized per session to avoid time-correlated drift biasing one condition
- RF power level is randomized or blinded where feasible, decoded only at analysis time
- Analysis is run on blinded, anonymized datasets; the code is fixed before unblinding
Criteria for declaring a positive result — a candidate ΔF is only reported as a genuine anomaly if it:
- Exceeds the combined, pre-registered uncertainty budget by a stated margin (e.g. ≥ 5σ)
- Scales with RF input power in a physically consistent way
- Reproduces across independent runs, and ideally independent operators or labs
- Appears in Test A but vanishes (returns to the reference baseline) in Tests B, C and D
- Survives with the RF chain diverted into the dummy load as a final control
- Has been checked against every term in the F_conventional model, not just asserted to be "left over"
Anything short of this is, at best, a lead worth re-testing — not a result.
5 · Thermal instrumentation
TH-001 — thermocouples/RTDs at five minimum points: T1 cavity, T2 front flange, T3 rear flange, T4 support, T5 environment — tracking both T_i(t) and, critically, ΔT(t), since thermal expansion can become a significant contribution in V1. TH-002 — local RF hot-spot temperature sensor. TH-003 — passive dissipation or controlled cooling for V1; active thermal enclosure and tighter regulation deferred to V1.1.
6 · Environmental sensors
| ID | Component | Purpose |
|---|---|---|
| ENV-001 | Accelerometers | Measure a_x, a_y, a_z → estimate F_vib = m·a to quantify vibration contribution |
| ENV-002 | Pressure sensor | Track air → reduced pressure → vacuum, to compare results in atmosphere vs. under vacuum (V1.1) |
| ENV-003 | Magnetometer | Ambient magnetic field B_ambient(t) |
| ENV-004 | EMI / electrical sensor | Characterizes RF and mains-borne disturbances |
7 · Vacuum system — V1.1 option
VAC-001 vacuum chamber (target <10⁻⁴ mbar in the optimized V1.1 configuration, to cut convection, air movement and atmospheric thermal effects), VAC-002 vacuum pump sized to chamber volume, VAC-003 independent pressure gauge.
8–11 · Acquisition, power, shielding, safety
- DAQ-001 — multichannel acquisition of F, P_fwd, P_refl, T, a, B, V, I
- DAQ-002 — a single common time base for every channel is essential
- DAQ-003 — high-resolution ADC (numerical resolution alone doesn't guarantee physical resolution)
- PM-001 — AC mains → EMI filter → supply → DC bus → RF amplifier, with overvoltage / overcurrent / thermal / e-stop protection
- PM-002 — separate, low-noise supply for sensors, DAQ and the control computer
- SH-001 — RF shielding, to keep stray fields out of the measurement
- SH-002 — magnetic shielding, material and geometry set by measured results
- SH-003 — full experimental enclosure around cavity + suspension (V1.1)
- SAF-001 — RF interlock: auto-cutoff on enclosure opening, overheat, wrong pressure, or electrical fault
- SAF-002 — emergency stop
- SAF-003 — high-voltage protection per the amplifier/source manufacturer's ratings and applicable standards
12 · Full V1 parts list
| ID | Component | Subsystem | V1 status |
|---|---|---|---|
| MC-001 | Cavity body | Mechanical | Essential |
| MC-002 | Front flange | Mechanical | Essential |
| MC-003 | Rear flange | Mechanical | Essential |
| MC-004 | Structure / support | Mechanical | Essential |
| RF-001 | RF source | RF | Essential |
| RF-002 | RF amplifier | RF | Essential |
| RF-003 | Circulator / isolator | RF | Recommended |
| RF-004 | Directional coupler | RF | Essential |
| RF-005 | 50 Ω load | RF | Essential |
| RF-006 | RF cables | RF | Essential |
| RF-007 | Cavity coupler | RF | Essential |
| QC-001 | Resonant cavity | QPS core | Essential |
| QC-002 | QPS module | QPS core | Experimental |
| QC-003 | Reference module | QPS core | Essential for validation |
| MM-001 | Force sensor | Measurement | Essential |
| MM-002 | Suspension | Measurement | Essential |
| MM-003 | Reference structure | Measurement | Essential |
| TH-001 | Temperature sensors | Thermal | Essential |
| TH-002 | Local temperature sensor | Thermal | Recommended |
| TH-003 | Thermal control | Thermal | Recommended |
| ENV-001 | Accelerometers | Environment | Essential |
| ENV-002 | Pressure sensor | Environment | V1.1 |
| ENV-003 | Magnetometer | Environment | Recommended |
| ENV-004 | EMI sensor | Environment | Recommended |
| DAQ-001 | Multichannel DAQ | Acquisition | Essential |
| DAQ-002 | Synchronization | Acquisition | Essential |
| DAQ-003 | ADC | Acquisition | Essential |
| PM-001 | Main power supply | Power | Essential |
| PM-002 | Instrumentation supply | Power | Essential |
| SH-001 | RF shielding | Shielding | Essential |
| SH-002 | Magnetic shielding | Shielding | Recommended |
| SH-003 | Experimental enclosure | Environment | V1.1 |
| VAC-001 | Vacuum chamber | Vacuum | V1.1 |
| VAC-002 | Vacuum pump | Vacuum | V1.1 |
| VAC-003 | Pressure gauge | Vacuum | V1.1 |
| SAF-001 | RF interlock | Safety | Essential |
| SAF-002 | Emergency stop | Safety | Essential |
| SAF-003 | Electrical protection | Safety | Essential |
13 · What to freeze now, what to leave open
Architecture + interfaces + instrumentation + measurement system
D, L, t, f₀, mode, Q, β, coupler position
Determine experimentally: f₀,meas, Q_meas, S₁₁, P_loss, T(t), F_meas(t) — closing, finally, on ΔF = F_meas − F_conventional with its full uncertainty budget.
Reference material
Scientific references
- Shawyer, R. (2006). A Theory of Microwave Propulsion for Spacecraft. Satellite Propulsion Research Ltd — the original proposal for an asymmetric resonant-cavity microwave thruster.
- White, H. et al. (2016). Measurement of Impulsive Thrust from a Closed Radio-Frequency Cavity in Vacuum. Journal of Propulsion and Power, 33(4) — NASA Eagleworks tests.
- Kraft, T. et al. (2021). Thrust measurements of an asymmetric resonant-cavity thruster: a critical analysis. TU Dresden — the thermal-artifact refutation.
- Wilson, C.M. et al. (2011). Observation of the dynamical Casimir effect in a superconducting circuit. Nature, 479(7373) — first experimental confirmation.
- Lamoreaux, S.K. (1997). Demonstration of the Casimir force in the 0.6 to 6 µm range. Physical Review Letters, 78(1).
- Casimir, H.B.G. (1948). On the attraction between two perfectly conducting plates. Proc. Royal Netherlands Academy of Arts and Sciences, 51.
- Jackson, J.D. (1999). Classical Electrodynamics, 3rd ed. Wiley.
- Pozar, D.M. (2012). Microwave Engineering, 4th ed. Wiley.
Glossary
- Resonant cavity
- A metal enclosure in which electromagnetic waves oscillate at frequencies set by its geometry.
- Casimir effect
- An attractive force between two parallel conducting surfaces caused by quantum vacuum fluctuations.
- Quality factor (Q)
- The ratio of stored energy to energy dissipated per cycle in a resonant system.
- Specific impulse (Isp)
- The duration a thruster can deliver thrust equal to the weight of its consumed propellant.
- MEMS
- Micro-Electro-Mechanical System — a micro-scale mechanism made by photolithography.
- Superconductor
- A material with zero electrical resistance below a critical temperature.
Conclusion
What's realistic: photon radiation pressure is a real, demonstrated phenomenon already used in solar sails and laser propulsion; resonant-cavity electromagnetics and the Casimir effect are well-established and measurable; quantum materials are a maturing, promising technology. None of that, by itself, proves NOAH-QPS produces net thrust.
What remains a challenge: any real thrust here is expected to be very small and would demand a heavy cryogenic system to operate; system complexity (vacuum, cryogenics, control) is extreme; He3 cost and maintenance are prohibitive for most applications; and — per TU Dresden's experience with the EmDrive — thermal drift, center-of-gravity shift, and cable coupling can all mimic thrust in a poorly-controlled test rig. That is precisely why the V1 differential architecture (QPS module vs. reference twin vs. dummy load) exists.
NOAH-QPS is not a perpetual-motion engine, a violator of momentum conservation, or an unlimited energy source. It is a spacecraft propulsion concept grounded in real physics, a serious engineering challenge, and a contribution to research on quantum effects relevant to gravity.

