NOAH Quantum Propulsion System

28/08/2026
NOAH-QPS · Quantum Propulsion System
NOAH·QPS FT-NOAH-QPS-001
V1 · complete experimental prototype, not yet a qualified thruster

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.

Claimed Effect
ΔF — unconfirmed
Naive Q·P/c Estimate
Retracted*
Input Power
100 W (RF)
Quality Factor Q
Target >10,000
Measured: TBD
System Mass
~600 kg
Core Metric
ΔF = F_meas − F_conv

* Withdrawn thrust/Isp figures & corrections: Physics tab. Full ΔF definition, uncertainty budget & blind protocol: V1 Prototype tab.

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01 · Identification & Philosophy

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.

◔ Working philosophy

"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.

// Identification
  • 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
// Guiding principle

"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.

03 · Fundamental Physical Principles

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.

⚠ Corrections & errata (supersede the original draft)
  1. 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.
  2. 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.
  3. 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.
  4. 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.
  5. 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.
  6. 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).
  7. 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.
  8. 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.

Thrust from a reflected beamF_photon = (1 + R) · P / c

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.

What Q actually amplifiesU_stored = Q · P_diss / ω₀  (energy, not force)

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.

Casimir force between platesF_Casimir = (π² · ℏ · c) / (240 · d⁴) · A

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).

Photon generation rateṄ ≈ (ω · δL / L₀)² · (c / 4L₀)

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.

04 · General Architecture

Reading the 3D model

Toggle Labels and Exploded view on the model above to see how these seven subsystems fit together.

[A] RF Source
  • Industrial magnetron, 2.45 GHz
  • 100–1000 W, modulable, ~70% efficiency
  • Frequency stability ±1 MHz
  • 3–5 kV supply, forced-air or liquid cooled
[B] Waveguide & Matching Taper
  • 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
[C] Resonant Cavity — the core
  • 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
[D] Dilution Cryostat
  • He3/He4 dilution refrigerator, base temp 10–50 mK
  • >100 µW cooling power at 100 mK
  • ~500 kg, ~1.5 L He3/day consumption
[E] Ultra-High Vacuum System
  • Target pressure < 10⁻⁹ mbar
  • Turbomolecular + cryo + ion/getter pumping stages
  • 316L stainless steel, ConFlat metal seals
[F] Control & Instrumentation
  • 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).

05–07 · Sizing, Materials & Control Loops

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.

TE011 resonant frequency (truncated-cone approximation)f = (c/2π) · √[(X'₀₁/a)² + (π/L)²]

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.

Cavity quality factorQ = (V/S) · √(ω₀ · μ₀ · σ)

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

ComponentMaterialSpecification
Resonant cavityOFHC copper (C10100)σ > 5.96×10⁷ S/m, purity >99.99%
Internal coatingSilver (Ag)5–10 µm, σ = 6.30×10⁷ S/m
Surface protectionGold (Au)0.1 µm, anti-oxidation
MEMS membraneSiN1 µm thick, E = 250 GPa
ActuatorPZT ceramicd₃₃ ≈ 300 pm/V, ±100 V
Superconducting optionNb-Ti / YBCOT꜀ = 9.2 K / 92 K
StructureAl 6061-T6σᵧ = 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

LoopSensorActuatorPerformance
TemperatureCernox thermometerHeaters + cryostat±0.1 mK at 10 mK
Vacuum pressureIon gaugePiezo valves + pumps±10%, <5 s response
Frequency lockPhase detectorMagnetron control voltage (PLL)<1 Hz on 2.45 GHz
MEMS mirror positionCapacitive electrodesPZT ±100 V<1 nm resolution
05.6, 08–09 · Performance & Comparison

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.

ParameterStatusNote
Net photonic thrustUnconfirmedDepends on wall-asymmetry momentum transfer — not on Q; to be measured as ΔF
Static Casimir contributionInternal force~1.3 pN between internal plates (1 µm gap, 1 mm²) — real, but not net external thrust by itself
Dynamic Casimir contributionHypothesisPhoton-pair production is confirmed physics; its use as thrust is untested here
Specific impulse (Isp)Not computable yetRequires a confirmed net thrust value, which does not currently exist
Electrical consumptionSpecified100 W RF input (design parameter, independent of the thrust question)
Mass (propulsion module / cryostat / total)Estimated50–100 kg / ~500 kg / ~600 kg
ΔF = F_meas − F_conventionalTo be measuredThe 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

ParameterNOAH-QPSAsymmetric RF-cavity concept (historical)Ion (Xe)Chemical
ThrustUnconfirmed (pending ΔF)0 (debunked)0.1–5 N10³–10⁶ N
IspNot computable yetN/A2000–5000 s300–450 s
Power100 WN/A1–10 kWN/A
EfficiencyNot computable yetN/A50–80%30–50%
StatusV1 experimental prototypeRefuted (thermal/mechanical artifacts)OperationalOperational
If the effect is confirmed
  • Potentially very high Isp
  • No propellant consumed
  • No moving-part wear at the macro scale
  • Electromagnetically silent (no plasma jet)
Known drawbacks regardless
  • 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
10–11 · Open Problems & Test Protocol

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

StageTestGoal
GroundRF characterizationMeasure Q, verify resonant modes (VNA)
GroundVacuum testLeak check, verify final pressure
GroundCryogenic testCool to 10 mK, verify thermal stability
GroundForce testOptical torsion balance, 1 pN sensitivity
Vacuum chamberSimulated microgravityDrop tower, ~10 s free fall
FlightSuborbital flightSounding rocket, ~5 min microgravity
FlightOrbital missionCubeSat (3U/6U), months-long orbit-correction test
V1 · Experimental Prototype & Validation Rig

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:

Residual force under testΔF = F_meas − F_conventional

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

A — the prototype / drive chain
  • RF source → amplifier
  • Directional coupler (forward/reflected)
  • Coupler into the resonant cavity
  • QPS interaction module (swappable)
B — the scientific validation chain
  • 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

IDComponentFunction
MC-001Cavity main bodyPrimary 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-002Front flangeCavity closure, mechanical interface, optional coupler feedthrough, instrumentation access
MC-003Rear flangeClosure, stiffening, instrumentation interface, mechanical symmetry
MC-004External structure / supportHolds the cavity, transmits force to the measurement system, suppresses parasitic motion (Al, stainless, or low-expansion alloy per thermal analysis)

2 · RF subsystem

IDComponentFunction
RF-001RF sourceGenerates 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-002RF amplifierRaises 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-003Isolator / circulatorProtects the source, absorbs or redirects reflected power, stabilizes the setup
RF-004Directional couplerSeparately measures P_forward and P_reflected — the only way to know actual injected RF power
RF-00550 Ω dummy loadVerifies the measurement chain produces no artificial signal when the cavity isn't excited
RF-006RF coaxial cabling50 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-007Cavity couplerMagnetic 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:

Differential signalΔF_QPS = F_QPS − F_reference

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:

TestConfiguration
Test AQPS module installed
Test BReference (twin) module installed
Test CCavity alone, no module
Test DRF dummy load, cavity bypassed

This four-way comparison is far more powerful than a simple on/off thrust measurement.

4 · Thrust measurement system

IDComponentNotes
MM-001Force sensorMeasures 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-002SuspensionTorsion pendulum or flexible mount, low friction, with known natural frequency f_mechanical and damping ratio ζ, both characterized
MM-003Reference structureMechanically 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_conventional(t) = F_thermal(t) + F_leakage + F_cable + F_vibration(t) + F_buoyancy + F_magnetic
  • 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 sourceTypeMitigation
Sensor noise / resolutionA (statistical)Signal averaging, lock-in detection synced to RF chop frequency
Sensor calibration & linearityB (systematic)Traceable calibration via electrostatic comb actuator or calibrated micro-mass
Thermal driftBTH-001 array + subtraction of the modeled F_thermal(t)
Mechanical vibrationA/BENV-001 accelerometer-derived correction, vibration-isolated bench
RF leakage / EM couplingBSH-001 shielding + leakage characterized with cavity de-tuned
Cable couplingBFixed, symmetric, damped routing; verified via dummy-load-only run
Environmental (pressure, B-field)BENV-002/003 logging and subtraction
Calibration-standard traceabilityBCalibration source itself independently certified

Calibration & run procedure

  1. Baseline / zero — Test D (dummy load, RF off): establish the noise floor and sensor offset over an extended quiet period.
  2. Calibrated force injection — apply a known force (electrostatic comb or calibrated small mass) to confirm sensor gain and linearity in physical units.
  3. 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.
  4. Reference run — Test B (reference twin installed): sweep RF power (0–100 W) to build the F_conventional(P) curve for this exact geometry.
  5. QPS run — Test A (QPS module installed): repeat the identical sweep and protocol.
  6. 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

IDComponentPurpose
ENV-001AccelerometersMeasure a_x, a_y, a_z → estimate F_vib = m·a to quantify vibration contribution
ENV-002Pressure sensorTrack air → reduced pressure → vacuum, to compare results in atmosphere vs. under vacuum (V1.1)
ENV-003MagnetometerAmbient magnetic field B_ambient(t)
ENV-004EMI / electrical sensorCharacterizes 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 electronics
  • 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)
Power supply
  • 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
Shielding
  • 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)
Safety
  • 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

IDComponentSubsystemV1 status
MC-001Cavity bodyMechanicalEssential
MC-002Front flangeMechanicalEssential
MC-003Rear flangeMechanicalEssential
MC-004Structure / supportMechanicalEssential
RF-001RF sourceRFEssential
RF-002RF amplifierRFEssential
RF-003Circulator / isolatorRFRecommended
RF-004Directional couplerRFEssential
RF-00550 Ω loadRFEssential
RF-006RF cablesRFEssential
RF-007Cavity couplerRFEssential
QC-001Resonant cavityQPS coreEssential
QC-002QPS moduleQPS coreExperimental
QC-003Reference moduleQPS coreEssential for validation
MM-001Force sensorMeasurementEssential
MM-002SuspensionMeasurementEssential
MM-003Reference structureMeasurementEssential
TH-001Temperature sensorsThermalEssential
TH-002Local temperature sensorThermalRecommended
TH-003Thermal controlThermalRecommended
ENV-001AccelerometersEnvironmentEssential
ENV-002Pressure sensorEnvironmentV1.1
ENV-003MagnetometerEnvironmentRecommended
ENV-004EMI sensorEnvironmentRecommended
DAQ-001Multichannel DAQAcquisitionEssential
DAQ-002SynchronizationAcquisitionEssential
DAQ-003ADCAcquisitionEssential
PM-001Main power supplyPowerEssential
PM-002Instrumentation supplyPowerEssential
SH-001RF shieldingShieldingEssential
SH-002Magnetic shieldingShieldingRecommended
SH-003Experimental enclosureEnvironmentV1.1
VAC-001Vacuum chamberVacuumV1.1
VAC-002Vacuum pumpVacuumV1.1
VAC-003Pressure gaugeVacuumV1.1
SAF-001RF interlockSafetyEssential
SAF-002Emergency stopSafetyEssential
SAF-003Electrical protectionSafetyEssential

13 · What to freeze now, what to leave open

Freeze now

Architecture + interfaces + instrumentation + measurement system

Determine by simulation

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.

12–14 · References, Glossary & Conclusion

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.

"Science knows no borders, for knowledge belongs to all of humanity."

FT-NOAH-QPS-001 · v1.0 · 2025 · Public Domain / Open Source

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