The first open engineering question in VENDOR.Max.
Stage-by-stage, with literature.
A literature-grounded, numerically-sourced framework for regime-sustainment feedback in an Armstrong-type nonlinear electrodynamic oscillator — with explicit reading discipline for the boundary equation.
VENDOR.Max is classified as an Armstrong-type nonlinear electrodynamic oscillator in a controlled discharge-resonant regime. Inside that architecture, one unresolved physics-integration node remains: whether the regime formed in the regime-forming path induces, through planar transformer coupling, sufficient real power in the regime-feedback path to compensate the losses of the regime-forming path with a stability margin. Every other element of the architecture is interpretable inside published electrodynamics and standard power electronics.
The complete-device boundary equation P_in,boundary = P_load + P_losses + dE/dt is the closure constraint at the complete device boundary — and at that boundary only. The device contains eight internal architectural stages, each governed by separate physical quantities. The boundary equation does not apply at any single internal stage and cannot be used to compare any internal input port — such as the 9 V startup port — to any internal output port — such as the kW-scale customer interface. Drawing such a comparison without consulting the internal stage map is a category error.
The architecture does not claim energy creation. It does not claim overunity. It does not claim operation outside classical electrodynamics. Every numerical parameter carries an explicit source label: Cat 1 (Patent / BASECANON), Cat 2 (published literature, cited inline), Cat 3 (illustrative declared assumption with a published-range anchor), or Cat 4 (VENDOR internal model, not disclosed).
§ 1 — Engineering classification
VENDOR.Max is an Armstrong-type nonlinear electrodynamic oscillator operating in a controlled discharge-resonant regime. The engineering classification is governed by classical electrodynamics, with macroscopic device-scale accounting under Level 1 of the Three-Level Energy Model reference. The architecture is patented under Spanish patent ES2950176B2 (granted) and PCT family WO2024209235A1 (active). The technology is positioned in the infrastructure continuity layer.
The first unresolved physics-integration node is whether the regime formed in the regime-forming path induces, through planar transformer coupling, sufficient real power in the regime-feedback path — after rectification, BMS routing, and buffer regulation — to compensate the real losses of the regime-forming path with a stability margin under the BMS-permitted operating window.
The proposition of this article is fourfold. First, every physical building block required by that integration node has independent published support in mainstream plasma-physics, electromagnetics, and power-electronics literature, with inline citation [1]–[9]. Second, the integration question itself is closable by independent boundary metrology and is the central focus of the next-stage validation programme. Third, the apparent numerical asymmetry between the 0.015 Wh transient startup and the hundreds-of-watts internal regime flow is resolved by recognising them as different categories of physical quantity. Fourth, the runaway/collapse stability problem of regenerative oscillators is solved by the BMS and its Buffer — a textbook engineering pattern with literature precedent in Armstrong's super-regenerative receiver [8] and in self-excited induction generator stabilisation [9].
§ 2 — Architectural prologue
VENDOR.Max is a solid-state electrodynamic power-conversion architecture. It is not a battery, not a chemical generator, not a thermal engine, not a rotating prime-mover machine. The architecture is structured in three coupled functional layers.
Layer one — regime initiation
A discrete startup impulse of approximately 0.015 Wh at approximately 9 V for approximately 10–15 seconds charges the capacitive regime nodes designated C2.1, C2.2, C2.3 and initiates the operating regime. After regime establishment the startup port is electrically isolated from the regime nodes per patent claim 1. The startup impulse is regime initiation, not energy supply: its energy content is orders of magnitude below any record of long-duration operation.
Layer two — regime formation
The capacitive regime nodes feed sealed nonlinear conductivity cells that undergo a fast, repeatable conductivity transition. Each transition releases stored electric-field energy into a primary resonant winding of high quality factor at a fundamental frequency of 2.45 MHz. The primary winding is the core of a planar transformer-type coupling structure. The microscopic mechanism inside the sealed cell is proprietary and is not attributed in this article to any specific named mechanism.
Layer three — coupled redistribution with active buffer regulation
The planar transformer couples the regime-forming path to two further functional paths. The regime-feedback path returns rectified power, routed through the BMS-controlled Buffer, to the capacitive regime nodes to compensate the losses of the regime-forming path. The output-extraction path routes power into rectification, DC-bus conditioning, and final inverter output.
The Boundary Management System (BMS) and its Buffer are the active control architecture placed between the planar transformer secondary and the capacitive regime nodes. The BMS is the controller; the Buffer is the bidirectional storage. Both are documented in detail in § 11. For the architectural prologue here it suffices that the BMS, using the Buffer as its storage medium, absorbs surplus feedback when the regime is at operating point and releases stored energy back into the regime when the feedback undershoots demand. Without this controller-and-storage pair, a regenerative feedback architecture either runs away or collapses; this is a classical stability result first solved by Armstrong [8] in 1922.
Boundary-crossing terms
At the complete device boundary, the following terms cross the enclosure:
- The transient startup input: ~0.015 Wh, ~10–15 seconds, then the port is inactive per patent claim 1.
- The auxiliary supervisory input: a small-signal inbound flow at all operational states that powers BMS logic, telemetry, monitoring, and firmware. It is the control-domain power supply, not the regime-sustaining energy path.
- The customer output: outbound delivered power to the external load.
- The enclosure-loss term: heat and electromagnetic radiation crossing the enclosure outbound (bookkeeping under
P_losses).
Sustained operation is governed by internal regime redistribution within the formed regime under BMS supervisory authority over the Buffer. The auxiliary supervisory input is not the regime-sustaining energy path; it powers control and telemetry only.
§ 3 — The first open engineering question
Inside the architecture above, one integration node remains the first unresolved physics question.
The question. Does the regime formed in the regime-forming path induce, through planar transformer coupling, sufficient real power in the regime-feedback path — after rectification, BMS routing, buffer regulation, and return-path losses — to satisfy:
P_feedback ≥ P_loss + P_marginwhere P_feedback is the real power returned to the capacitive regime nodes C2.1–C2.3 through the regime-feedback path, P_loss is the real loss rate of the regime-forming path under operation, and P_margin is the stability reserve required to keep the regime inside its BMS-permitted operating window against drift, thermal variation, and load perturbation.
Three clarifications on what the question is not.
It is not "can the startup port directly power a kilowatt-scale load". The startup port is transient (~15 s) and electrically isolated once the regime is established.
It is not "does the device violate energy conservation". The boundary equation P_in,boundary = P_load + P_losses + dE/dt is the closure constraint at the complete device boundary at all operational states — and at that boundary only; internal stages have separate formulas (see § 6).
It is not "what is the device efficiency". A single whole-device converter-efficiency ratio is not the correct diagnostic for this multi-boundary architecture. Per-stage efficiencies remain valid and necessary.
What the question is: whether the specific integration of nonlinear conductivity switching, LC resonance, high-Q stored energy, planar transformer coupling, and BMS-controlled Buffer regulation achieves the feedback inequality inside the actual device.
§ 4 — The numerical drama
The integration question is not abstract.
At Stage 01 of the architecture, the device receives: E_startup ≈ 0.015 Wh ≈ 54 J. This is a one-time quantum delivered at approximately 9 V over approximately 10 to 15 seconds. After that, per patent claim 1, the startup port is electrically isolated from the regime nodes.
At Stages 04 through 05 of the architecture — once the regime is established — the regime-feedback path returns real power to the capacitive regime nodes C2.1–C2.3 at every operational state. The specific magnitude under load is a Cat 4 protected design parameter. The illustrative pixel-budget in § 10 demonstrates that, with parameters within published ranges, this flow is on the order of hundreds of watts at every operational state — orders of magnitude larger, in power dimension, than the startup quantum divided by any sensible time interval.
The naive reading is immediate and wrong: "0.015 Wh in, hundreds of watts out — overunity." The reading fails on four grounds.
First, the units are not comparable. The startup input is energy (joules); the regime-feedback flow is power (watts). Dividing 0.015 Wh by 15 seconds gives an average startup power of approximately 3.6 W during ignition only — a quantity that goes identically to zero after the startup port disconnects.
Second, the regime-feedback path is not a boundary input. It is a bounded resonant circulation flow inside the formed regime, between the planar transformer secondary and the capacitive regime nodes through the BMS-controlled Buffer. At the complete device boundary it is fully internal — it does not appear as a term in P_in,boundary. Intra-boundary circulation at hundreds of watts is normal for any high-Q resonant system; the fractional loss per cycle is 2π / Q, which for Q in the hundreds is a small fraction of the circulating energy.
Third, the boundary equation closes through different terms. At steady state, P_in,boundary = P_load + P_losses [at the complete device boundary only — see § 6]. The inbound terms are the auxiliary supervisory input plus zero from the disconnected startup port. The outbound terms are the customer-delivered power and enclosure losses. The internal regime-feedback flow — the hundreds of watts — is intra-boundary by topology and does not appear in the boundary equation at all.
Fourth, classical conservation does not forbid this geometry. A flywheel spun up briefly by a small motor can store kinetic energy enough to drive a load far in excess of the motor's average power, for as long as the stored energy lasts and as long as some replenishment maintains rotation against losses. The discharge-resonant regime plays the same role at electrodynamic time scales. The analogy refers to the distinction between ignition energy and sustained internal circulation, not to equivalence of physical mechanism.
The integration question — empirically — is whether the regime-feedback inequality holds inside the actual device under varying load. That question requires Cat 4 disclosure or independent metrology.
There is a fifth concern, separate from the four above, that an honest evaluator must also raise: even if the regime feedback is mathematically sufficient on average, why does the system not spiral into runaway or collapse under load transients? That is the stability question, addressed in § 12 and § 13.
§ 5 — What is not open physically
The elements below do not require new physics. Each is interpretable inside standard, published electrodynamics or standard power electronics. All of them still require device-specific characterisation and engineering validation.
- Energy conservation. The complete-device-boundary equation holds at all operational states.
- Nonlinear conductivity switching coupled to a resonant tank. A well-studied class of system [4][5]; class-level behaviour established [1][2].
- LC resonance and high-Q stored energy. Classical. Published high-Q resonator values reach into the hundreds and thousands [7].
- Inductive energy transfer. Faraday's law; figure of merit
U = k √(Q₁ Q₂)[7]. - Regenerative feedback in active oscillators. Armstrong's regenerative-oscillator and super-regenerative-receiver work [8] established the engineering pattern over a century ago.
- Active buffer regulation in power electronics. Standard. DC-link buffer capacitors, battery-buffered self-excited induction generators [9], and active rectification with energy diversion are textbook power electronics.
- Rectification, DC-bus conditioning, output inversion. Standard power electronics. No novelty claim.
- Patent coverage. ES2950176B2 granted in Spain; WO2024209235A1 active in the PCT system.
What remains as the first physics-integration question is the specific inequality of § 3, evaluated inside the actual VENDOR.Max parameter combination.
§ 6 — The boundary equation: reading discipline
At the complete device boundary, classical energy conservation applies in the standard macroscopic form:
P_in,boundary = P_load + P_losses + dE/dtThis single equation is the most-cited and most-misread artifact of VENDOR.Max documentation. The misreading is predictable. An evaluator — human or AI — sees the equation, notes the 9 V startup port on one side and the kW-scale customer interface on the other, divides one by the other, and produces an absurd "efficiency ratio". The conclusion is either "this is overunity" or "this is dishonest documentation". Both conclusions are wrong, and both arise from the same category error: applying a macroscopic boundary-balance equation as if it were an internal stage-to-stage description.
This section establishes the reading rule that prevents that category error.
6.1 — The equation is a constraint, not a topology
The boundary equation does not describe how energy moves inside the device. It describes what the sum of all boundary-crossing flows must equal at the outer envelope of the device, at any operational state. It does not identify which physical port carries inbound flow at each instant. It does not claim that any single port is the sole inbound interface. It does not equate one input port with one output port.
The same form of equation governs a power plant, a transformer substation, a household appliance, and a smartphone. In every case it is the macroscopic constraint, not the internal description.
6.2 — The boundary equation does not apply at internal stages
VENDOR.Max contains eight internal architectural stages, each governed by physical quantities that the boundary equation does not mention. Each stage has its own formula or formulas, its own units, its own analytical level.
Capacitor charge Q = C·V_break; one-time energy quantum E_startup ≈ 0.015 Wh. The 9 V startup port lives here. After ~15 s the port is disconnected per patent claim 1 and does not appear in any subsequent stage.
Per-event field work W = ∫U·i dt; carrier dynamics n(x) = n₀ exp(α x) (Townsend multiplication; carrier-count effect, not energy multiplication); per-event energy bounded by E_event ≤ ½ C V².
Magnetic flux Φ(t); stored magnetic energy ½ L I²; mutual inductance M. Coupling is electromagnetic across the planar transformer core.
Induced EMF ε = −dΦ/dt on the regime-feedback winding and the output-extraction winding independently. Per-event energy partitions across both windings in parallel — neither is downstream of the other.
Per-event feedback energy E_fb,event; per-stage efficiency η_secondary_path (rectifier chain + BMS routing + return path). The first open inequality P_feedback ≥ P_loss + P_margin lives at this stage.
Per-event tertiary energy E_tertiary,event; per-stage efficiency η_tertiary_path and η_rectifier. Structurally separate from Stage 05.
Real power P_load = ⟨V·I⟩ (phase-aware) at the customer interface; per-stage η_inverter and η_filter. The kW-scale customer interface lives here.
This is the stage at which the boundary equation P_in,boundary = P_load + P_losses + dE/dt applies. Closure is verified under accredited independent metrology within measurement uncertainty.
The 9 V startup port (Stage 01) and the kW-scale customer interface (Stage 07) are seven stages apart in the internal architecture. Comparing one to the other through the Stage 08 boundary equation, without traversing Stages 02–07, is the central source of misclassification in VENDOR.Max evaluations.
6.3 — What independent boundary metrology will close
Whether the architecture closes the boundary equation under third-party measurement, with explicit accounting for each boundary-crossing term: the transient startup input (active only during ignition), the auxiliary supervisory input (small-signal control power), the customer output (kW-scale), and the enclosure-loss term (heat and radiation through the enclosure). The closure question is whether the boundary residual at the complete device boundary tends to zero within measurement uncertainty under accredited metrology — this is the empirical question. It is separate from the regime-feedback inequality question of § 3, which lives at Stage 05 of the internal map.
6.4 — The reading rule, formal
When the equation P_in,boundary = P_load + P_losses + dE/dt appears in any VENDOR.Max documentation, the following four-point discipline applies:
- (i) Boundary only. The equation applies exclusively at the complete device boundary. It does not apply at any single internal stage.
- (ii) Aggregate inbound, aggregate outbound. The inbound and outbound terms are sums across all boundary-crossing flows, not designations of single ports.
- (iii) Internal mechanism is separate. Internal flow between stages is governed by the stage-specific formulas in 6.2. The boundary equation neither describes nor constrains internal flow.
- (iv) Cross-stage ratios are category errors. Comparing a quantity from Stage 01 (such as the 9 V startup port) directly to a quantity from Stage 07 (such as the kW-scale customer interface) through the boundary equation is invalid.
Any reading of the equation that violates one of these four points is a misclassification.
§ 7 — The two-stage energy budget
The first open question lives entirely inside Stage one of a clean two-stage decomposition.
- Stage one — regime sustainment.
P_feedback ≥ P_loss + P_margin. Internal to the regime-formation loop. - Stage two — output extraction. Once Stage one is sustained, how much surplus is available for customer delivery.
This article addresses Stage one only.
§ 8 — The reduced inequality
The Stage-one inequality in explicit form combines the classical Q-factor relation, the classical capacitor stored-energy expression, and the bridge equation from pulsed-power literature with the coupling-and-conversion product from inductive coupling literature:
P_loss = ω E_stored / Q (classical Q-factor)E_event = ½ C V² (classical capacitor stored energy)
P_feedback = E_event × f_event × N × k_sec × η_secondary_path
Stage-one inequality in explicit form:
½ C V² × f_event × N × k_sec × η_secondary_path ≥ ω E_stored / Q + P_margin§ 9 — Pixel-budget from independent published literature
9.1 — Nonlinear conductivity switching
The regime-forming path requires a fast nonlinear conductivity transition releasing capacitively stored energy into the primary resonant winding. The gas-discharge literature describes a broad family of such transitions. Townsend multiplication is a conductivity effect that multiplies carrier count, not energy. Per-event energy in any discharge gap is bounded by E_event ≤ ½ C V². The microscopic mechanism inside the sealed cells of VENDOR.Max is proprietary [Cat 4].
9.2 — LC resonance and high-Q stored energy
Per-cycle fractional loss in a resonant tank is 2π / Q. Published high-Q LC resonator literature reports values from hundreds to thousands routinely. Kurs et al. [7] report Q ≈ 950 for coupled resonant coils at MHz operating frequency.
9.3 — Self-excited plasma series resonance [1][2]
Schüngel, Brandt, Korolov, Derzsi, Donkó and Schulze studied self-excitation of plasma series resonance oscillations [1] and electron heating via self-excited PSR [2]. The class of phenomenon — nonlinear discharge regime self-exciting high-frequency oscillatory current structure — is independently established.
9.4 — Nonlinear power absorption and geometry [3]
Noesges and Mussenbrock identified stepwise increases in cumulative electron power density during sheath expansion associated with PSR excitation [3]. Geometry is a primary design parameter modulating power-absorption efficiency.
9.5 — Self-pulsing in dielectric barrier discharges [4]
Thagunna, Kolobov and Zank demonstrated multiple current pulses per AC period across Townsend and capacitively coupled discharge modes [4], with transitions depending on gap conditions and external circuit parameters.
9.6 — Multi-cell pulse synchronisation [5]
Shaygani and Adamiak demonstrated self-synchronised pulse trains through mutual electric-field and space-charge interactions in multi-point corona discharge systems [5].
9.7 — Measured pulse energies in discharge channels [6]
Elkholy et al. measured pulse energies of approximately 1.9 µJ and 2.7 µJ per channel [Cat 2] in a nanosecond DBD microplasma reactor [6].
9.8 — Resonant inductive coupling [7]
Kurs et al. demonstrated efficient mid-range power transfer at approximately 60 W with overall efficiency near 40% across approximately 2 m, with coupling coefficient k ≈ 0.001 and Q ≈ 950 [7]. Figure of merit U = k √(Q₁ Q₂).
The Kurs et al. result is cited here as the established literature anchor for two specific things: (a) the coupling formalism U = k √(Q₁ Q₂), which governs energy transfer between tuned resonators; and (b) the demonstration that high-Q resonators with values approaching 10³ are reproducible in published laboratory conditions. The cited numerical values (60 W, 40%, 2 m) describe the MIT wireless-power-transfer demonstration geometry — two free-standing resonant coils separated by a substantial distance — and are not direct support for the geometry or power density of VENDOR.Max. The relevance of [7] is to the coupling formalism and to the published-range Q values, not to the specific demonstrated wireless-transfer geometry.
9.9 — Regenerative feedback and buffered stabilisation [8][9]
Armstrong [8] established two foundational engineering patterns relevant to VENDOR.Max. The 1915-era regenerative oscillator demonstrated that positive feedback from a tuned output back to a nonlinear active element produces sustained oscillation with amplification orders of magnitude beyond passive circuits. The 1922 super-regenerative receiver introduced active runaway-prevention — a periodic quench that bounds the regenerative amplifier and keeps it within a stable operating envelope. The super-regenerative receiver demonstrated that a regenerative architecture with active stability control is a robust, deployable engineering pattern, not a theoretical curiosity.
The self-excited induction generator (SEIG) literature [9] demonstrates the same pattern in the power-engineering domain: a regenerative machine started by a small excitation and stabilised under load by capacitor self-excitation in combination with a battery or capacitor buffer that absorbs surplus and releases stored energy under transients. SEIG systems are a routine engineering technology in microgrids and remote-power applications.
For VENDOR.Max the relevance is conceptual: the BMS-and-Buffer pair is not a novelty class — it is a conceptually analogous control pattern to Armstrong's super-regenerative quench mechanism [8] and to capacitor/battery-buffered self-excitation in SEIG designs [9]. Armstrong's 1922 super-regenerative receiver used a periodic quench signal to drive the regenerative detector into and out of oscillation, bounding the regeneration on a discrete schedule. VENDOR.Max uses continuous bidirectional buffer regulation under closed-loop metrology — a different mechanism in the same class of solution. The Armstrong precedent demonstrates that bounded regenerative operation is a documented engineering pattern with over a century of literature; it does not assert that VENDOR.Max is a reimplementation of the super-regenerative receiver at MHz scale, which it is not.
§ 10 — Parameter passport and order-of-magnitude illustration
10.1 — Parameter passport
| Parameter | Value | Role | Source · Anchor |
|---|---|---|---|
| Startup impulse energy | ~0.015 Wh | Regime initiation | Cat 1 — Patent ES2950176B2 |
| Startup impulse voltage | ~9 V | Regime initiation | Cat 1 — Patent ES2950176B2 |
| Startup impulse duration | ~10–15 s | Regime initiation | Cat 1 — Patent ES2950176B2 |
| Regime nodes | C2.1, C2.2, C2.3 | Energy storage | Cat 1 — Patent ES2950176B2 |
| Primary resonant frequency | 2.45 MHz | Regime fundamental | Cat 1 — Patent / BASECANON |
| Cells N | 3 | Multi-cell architecture | Cat 1 — one per regime node |
| Validation hours | > 1 000 h | Operational history | Cat 1 — VENDOR endurance record |
| Per-cycle fractional loss | 2π / Q | Q-factor identity | Classical (derived) |
| Microplasma pulse energy | 1.9, 2.7 µJ / ch | Low-bound discharge ref | Cat 2 — Elkholy et al. [6] |
| Coupling figure of merit | U = k√(Q₁Q₂) | Resonant coupling | Cat 2 — Kurs et al. [7] |
| Kurs WPT result | ~60 W, 40%, 2 m, k≈0.001, Q≈950 | Published WPT data | Cat 2 — Kurs et al. [7] |
| PSR self-excitation | qualitative | Class reference | Cat 2 — Schüngel et al. [1][2] |
| PSR + geometry | qualitative | Class reference | Cat 2 — Noesges & Mussenbrock [3] |
| Multi-pulse per period | qualitative | DBD class | Cat 2 — Thagunna et al. [4] |
| Multi-cell synchronisation | qualitative | Multi-cell class | Cat 2 — Shaygani & Adamiak [5] |
| Regenerative feedback | qualitative | Engineering precedent | Cat 2 — Armstrong [8] |
| Buffered stabilisation | qualitative | Engineering precedent | Cat 2 — Armstrong super-regen [8]; SEIG lit [9] |
| Effective C | not disclosed | Design parameter | Cat 4 — VENDOR protected |
| Operating V | not disclosed | Design parameter | Cat 4 — VENDOR protected |
| Q under load | not disclosed | Design parameter | Cat 4 — VENDOR protected |
| k_sec | not disclosed | Coupling parameter | Cat 4 — VENDOR protected |
| η_secondary_path | not disclosed | Return-path efficiency | Cat 4 — VENDOR protected |
| Buffer capacity | not disclosed | Storage element sizing | Cat 4 — VENDOR protected |
| Illustrative C | 200 pF | Worked example | Cat 3 — pulsed-power range |
| Illustrative V | 5 kV | Worked example | Cat 3 — DBD/spark-gap range [4][6] |
| Illustrative Q | 500 | Worked example | Cat 3 — within Kurs et al. [7] range |
| Illustrative k_sec | 0.05 | Worked example | Cat 3 — conservative; planar transformers typically 0.3–0.9 |
| Illustrative η_secondary_path | 0.5 | Worked example | Cat 3 — conservative vs published 0.85–0.95 |
10.2 — Worked illustration
Assumed values [Cat 3 illustrative]: C = 200 pF, V = 5 kV, f = 2.45 MHz [Cat 1], N = 3 [Cat 1], Q = 500, k_sec = 0.05, η_secondary_path = 0.5.
Step 2. ω = 2π × 2.45 MHz ≈ 1.54 × 10⁷ rad/s
Step 3. E_stored ≈ 2.5 mJ × 3 = 7.5 mJ
Step 4. P_loss = ω × E_stored / Q ≈ 231 W
Step 5. P_circulating = E_event × f × N ≈ 18.4 kW
Step 6. P_feedback ≈ 18.4 kW × 0.05 × 0.5 ≈ 460 W
Step 7. 460 W ≥ 231 W + P_margin (inequality satisfied)
The P_circulating ≈ 18.4 kW estimate in Step 5 represents resonant intra-stage energy circulation inside a high-Q regime and is not a boundary-crossing supply term. It is the bookkeeping of energy that circulates internally between the capacitive regime nodes and the primary winding inductance — the same quantity that, in any LC resonator of moderate Q, exceeds boundary-crossing flows by the factor Q / 2π. See § 6 reading rule and Stage 03 of the eight-stage map.
10.3 — The numerical drama, made arithmetic
P_startup,avg ≈ 54 J / 15 s ≈ 3.6 W (only during 15 s ignition). After ignition, the startup port is disconnected. The illustrative regime-feedback flow is approximately 460 W at every operational state, of which approximately 231 W compensates regime losses and the remainder is managed by the BMS via routing to the Buffer.
The ratio of steady regime-feedback flow to time-averaged startup power is approximately 460 / 3.6 ≈ 128 in this illustration. This is the expected ratio for an LC resonator of moderate Q. A flywheel spun up briefly by a small motor produces exactly the same dimensional ratio: small ignition motor, large stored kinetic energy, large internal circulation, small external replenishment against losses.
Honest framing. No parameter value is outside commonly reported ranges, and each Cat 3 value carries an explicit literature anchor in 10.1. The specific combination is illustrative, not literature-derived as a single package. The actual VENDOR.Max parameter combination is Cat 4. Validation requires Cat 4 disclosure under NDA or independent boundary metrology.
§ 11 — The Boundary Management System and the Buffer
The integration core of the architecture is a pair of distinct elements placed between the planar transformer secondary and the capacitive regime nodes C2.1–C2.3:
- The Boundary Management System (BMS) — the active control element. It is the supervisory regulator that manages internal routing and operating-window stability while independent boundary closure is evaluated empirically at the complete device boundary, by routing internal flows under priority rules and by acting on real-time metrology data. It is a controller: it commands, schedules, and prioritises; it does not itself store or supply energy, and it does not — and cannot — enforce conservation laws. Conservation is a physical constraint of the complete device boundary; the BMS operates inside that constraint and supports its empirical verification.
- The Buffer — the physical bidirectional energy storage element managed by the BMS. It is implemented as a combination of battery cells, DC-link capacitors, and active-rectification electronics. It is the storage medium: it absorbs energy when commanded by the BMS, releases stored energy when commanded by the BMS, and holds state of charge in equilibrium.
The two are functionally distinct. BMS = controller, Buffer = controlled storage. The Buffer alone could not maintain the regime because there would be no decision logic. The BMS alone has no energy to redistribute because it has no storage of its own. The engineering integration is the pair.
11.1 — The BMS as primary architectural role
The BMS in VENDOR.Max is, primarily and architecturally, a Boundary Management System. Its function is to manage internal routing and operating-window stability — through closed-loop metrology acquisition and real-time decision logic — during empirical evaluation of boundary closure at the complete device boundary under accredited measurement. The BMS routes internal energy flows between three destinations: (a) to the capacitive regime nodes C2.1–C2.3, to sustain the regime-forming path; (b) to the Buffer, when the regime is at operating point and surplus exists; (c) to the output-extraction path, into rectification and inverter stages for customer delivery.
The BMS is a control element. It does not appear as a power-supply term in any architectural stage. It does not create energy. It is a supervisory negative-feedback regulator — a well-understood class of element in power-electronics literature.
11.2 — The Buffer as controlled storage element
The Buffer operates in three modes under BMS command:
- Inbound mode (regime sufficient or surplus). When the regime-feedback path returns more power than the capacitive regime nodes require for sustainment, the BMS routes the surplus into the Buffer. The capacitive node voltage is held at its operating point. The regime is slightly damped to prevent over-accumulation.
- Outbound mode (regime in deficit). When the regime-feedback path returns less power than required — for example, when the output-extraction path is drawing heavily under peak load — the BMS draws stored energy from the Buffer and returns it to the capacitive regime nodes. The regime is sustained against the transient.
- Equilibrium mode. When feedback supply and regime demand are matched, the Buffer holds its state of charge and the system runs at thermal equilibrium.
11.3 — The acronym, and why it is a cognitive trap
The acronym BMS is, in conventional power-electronics usage, Battery Management System — control logic that supervises a battery: state-of-charge balancing, over-voltage and under-voltage prevention, temperature management, cycle counting, charge-discharge orchestration. This is routine industrial practice, and the same function is performed inside the VENDOR.Max architecture because the Buffer contains battery cells.
But in the VENDOR.Max architectural sense, BMS is primarily Boundary Management System, not Battery Management System. The distinction matters because the cognitive trap is built into the acronym: a reader who expands "BMS" to "Battery Management System" sees a system that "manages the battery" (i.e., manages the Buffer), and the Buffer contains batteries, and the loop closes in on itself — the reader concludes that BMS is just industrial battery housekeeping. That conclusion misses the architectural significance entirely.
The correct reading hierarchy: (1) Primary function: Boundary Management. The BMS manages internal routing and operating-window stability through closed-loop metrology and decision logic, during empirical evaluation of boundary closure at the complete device boundary. This is the architectural role. The BMS does not enforce conservation laws; conservation holds independently. (2) Subordinate function: Battery Management. Because the Buffer contains battery cells, standard battery-management functions are performed by the BMS as routine supervision of one component of the Buffer. This is industrial convention. (3) The Buffer itself: the controlled object. Battery cells + DC-link capacitors + active-rectification electronics, treated as a single bidirectional storage element under BMS command.
11.4 — Why both elements are necessary
A regenerative architecture with positive feedback has exactly two failure modes without active stabilisation: runaway (under low load) and collapse (under peak load). § 13 develops the dynamics. Without the BMS the regime would be uncontrolled. Without the Buffer the BMS would have no place to route surplus and no reservoir from which to draw under deficit. The engineering integration is the pair: controller plus controlled storage. The control pattern — active bounding of a regenerative process — is conceptually analogous to Armstrong's super-regenerative quench mechanism (1922) [8] and to capacitor/battery-buffered self-excitation in SEIG designs [9]. It is a precedent for bounded regenerative operation through active control. It is not a reimplementation of those specific architectures, which operate at audio or 60 Hz scales rather than at MHz discharge-resonant scales.
§ 12 — The control-layer architecture
A common misreading of the BMS-and-Buffer pair is that the BMS somehow "enforces" the boundary equation — as if a control element could override or guarantee a physical law. That reading is incorrect. Conservation of energy is a physical constraint of the complete device boundary; it holds independently of any control element. The BMS does not enforce it and cannot enforce it.
The architecturally correct framing is a standard six-layer control-system hierarchy, in which each layer plays a well-understood role:
12.1 — The six layers
The first-law-of-thermodynamics constraint. Holds unconditionally at the complete device boundary. Independent of any device-specific design. This is physics.
The accounting expression of Layer 1 as applied to the VENDOR.Max device: P_in,boundary = P_load + P_losses + dE/dt. Boundary-only; see § 6 reading rule.
The measurement layer. Sensors that acquire real-time data on regime state, capacitive-node voltages, planar transformer fluxes, currents, Buffer state-of-charge, thermal envelope, and customer-side load.
The control layer that consumes Layer 3 metrology data, performs regime-state estimation, and issues routing commands. A closed-loop digital controller analogous in role to a PLL, an SMPS controller, or a grid-tied inverter control architecture.
The controlled storage layer. Bidirectional energy storage made of battery cells, DC-link capacitors, and active-rectification electronics, responding to Layer 4 commands.
The controlled dynamic process. The discharge-resonant regime itself, maintained inside its permitted operating window by the action of Layers 4 and 5.
12.2 — What the hierarchy says about the BMS
The BMS does not enforce conservation laws. Conservation is the physical constraint of Layer 1, mediated through the accounting constraint of Layer 2. The role of the BMS, at Layer 4, is strictly operational: (i) continuous acquisition of metrology data from Layer 3; (ii) real-time regime-state estimation; (iii) dynamic routing of internal flows through the Layer 5 Buffer; (iv) maintenance of the Layer 6 regime within its operating window under changing load conditions.
The BMS supports stable boundary-balanced operation at the complete device boundary. It does not — and cannot — guarantee that boundary closure under independent metrology will be met; that is the empirical question of Layer 1 / Layer 2, closable only by third-party measurement.
12.3 — Why this is a standard control architecture
The six-layer hierarchy is the same architecture used in deployable industrial control systems across power electronics and signal processing.
- Phase-locked loops (PLL). A controlled VCO tracks a reference signal; the PLL controller is Layer 4; the loop filter is Layer 5; the VCO is the Layer 6 controlled process; reference comparison is the Layer 3 metrology.
- Switching-mode power supplies (SMPS). The controller adjusts switching duty cycle (Layer 4); the output filter capacitor and inductor act as the storage element (Layer 5); the switched topology is the Layer 6 controlled process; voltage and current sensing form Layer 3 metrology.
- Grid-tied inverters. The inverter controller manages active and reactive power injection (Layer 4); the DC-link capacitor is Layer 5 storage; the IGBT bridge is the Layer 6 controlled process; phase-aware grid metrology drives the loop.
- Self-excited induction generators (SEIG) [9]. The excitation controller manages capacitor-bank reactive power (Layer 4); the capacitor bank is Layer 5 storage; the induction machine is the Layer 6 controlled process; voltage and current sensing close the loop.
VENDOR.Max maps cleanly onto this pattern. The novelty of VENDOR.Max is not the control architecture; the control architecture is textbook. The novelty is the Layer 6 controlled process — a discharge-resonant regime at MHz time scales — and the specific integration of that process with the standard control stack.
12.4 — What changes about the evaluation question
This hierarchy changes the right question to ask. The naive question — "how does the BMS enforce conservation?" — is ill-posed: the BMS cannot enforce conservation, and need not, because Layer 1 holds independently. The correct evaluation question is: does the Layer 6 regime, under Layer 4/5 control, satisfy the Layer 1/2 boundary closure under independent Layer 3 metrology? That is a falsifiable, measurable, single-point empirical test. It is not a physics dispute.
§ 13 — The dynamic balance
The architecture is in continuous dynamic balance. This section describes the dynamics in scenarios — Layer 6 process behaviour under Layer 4/5 control.
13.1 — The runaway scenario, without the BMS and Buffer
Imagine the BMS and Buffer are removed and the regime-feedback path is connected directly to the capacitive regime nodes through only a rectifier. At nominal load, the regime-forming path discharges into the primary winding. The secondary induces real power that is rectified and dumped into C2.1–C2.3. The capacitive node voltage rises slightly. Higher node voltage produces a stronger discharge event (E_event = ½ C V²). The stronger discharge induces more secondary current. More secondary current produces still higher node voltage. The cycle amplifies until either a component fails or the regime locks at the supply rail.
This is the classical regenerative-oscillator runaway. Armstrong encountered it in 1912 with his regenerative receiver and solved it in 1922 with the super-regenerative architecture — by introducing active quench. VENDOR.Max faces the same problem and uses a continuous analog of Armstrong's solution: instead of periodically quenching the regeneration, the Buffer absorbs surplus at every operational state and the BMS damps the regime in real time.
13.2 — The collapse scenario, without the Buffer
Now the output-extraction path encounters a heavy load transient. The primary regime is loaded harder by the output-extraction path; the circulating energy in the primary tank drops. Less primary energy produces less secondary induced power. Less secondary power produces less rectified return to C2.1–C2.3. The capacitive node voltage droops. Lower node voltage produces weaker discharge events (E_event = ½ C V² falls quadratically with V). Weaker discharges produce less primary energy. The cycle decays until the regime collapses.
This is the classical regenerative-oscillator collapse under transient load. It is symmetric to the runaway problem. The same class of solution applies: a bidirectional energy buffer that can release stored energy quickly enough to sustain the regime during the transient.
13.3 — The balanced scenario, with the BMS and Buffer
Now restore the BMS and the Buffer between the secondary and C2.1–C2.3.
Under nominal load, the secondary delivers approximately 460 W of rectified feedback (illustrative budget of § 10). The regime requires approximately 231 W to compensate losses. The BMS routes approximately 231 W to C2.1–C2.3 to hold the regime at operating point and routes the remaining approximately 229 W into the Buffer. Buffer state of charge rises slowly. Capacitive node voltage held constant.
Under peak load, the output-extraction path draws harder. The primary regime is loaded more heavily, the secondary delivers less rectified feedback, and the regime would otherwise droop. The BMS detects the droop, draws stored energy from the Buffer, and augments the return flow to C2.1–C2.3 so the regime is held at operating point. Buffer state of charge falls.
Under low load, the output-extraction path draws less. The BMS detects the overshoot, diverts the excess into the Buffer, and slightly damps the regime by reducing the feedback delivered to C2.1–C2.3. Buffer state of charge rises.
This dynamic balance is the constant game of the architecture. It is the same class of balance maintained by the DC-link capacitor in any modern inverter, the capacitor bank in a self-excited induction generator [9], or the quench oscillator in Armstrong's super-regenerative receiver [8] — applied at the time scale of MHz discharge-resonant operation.
13.4 — What the Buffer is not
The Buffer is not the energy source of the device. Its state of charge is bounded; if the regime-feedback path were genuinely insufficient on average, the Buffer would discharge to zero and the regime would collapse. The Buffer can ride through transients of bounded duration; it cannot supply average power that the feedback path fails to provide.
The Buffer is not a hidden boundary input. It sits inside the device enclosure; it does not introduce any new boundary-crossing flow. The Buffer does not violate conservation. It stores energy delivered to it and releases energy from its store, with standard charge/discharge efficiencies subject to the constraints of battery and capacitor electrochemistry.
§ 14 — The integrated architecture in literature
The architecture has literature support at every stage, assembled into a coherent integrated picture. The map below lists each of the eight architectural stages with its function and its specific cited reference.
| # | Stage | Function | Cited anchor |
|---|---|---|---|
| 01 | Startup Impulse | One-time capacitor charging from external source through rectifier | Patent claim 1 [Cat 1]; classical electrostatics |
| 02 | Discharge & Regime Formation | Nonlinear conductivity transition releases capacitive energy into primary LC tank | Thagunna et al. [4]; Schüngel et al. [1][2]; Shaygani & Adamiak [5]; Elkholy et al. [6] |
| 03 | Primary Field & Non-Galvanic Coupling | High-Q LC tank circulates energy at fundamental frequency | Kurs et al. [7] (Q≈950 demonstrated); classical electromagnetics |
| 04 | Parallel Faraday Induction | Time-varying flux induces EMF in secondary and tertiary windings independently | Classical electromagnetics; Kurs et al. [7] (figure of merit) |
| 05a | Feedback Path (Regenerative) | Rectified secondary returns power toward the capacitive regime nodes — positive feedback architecture | Armstrong [8]; standard oscillator literature |
| 05b | BMS + Buffer (Active Stabilisation) | The BMS and Buffer together prevent runaway and collapse; support operating-window stability through metrology-driven internal routing | Armstrong super-regenerative [8]; SEIG literature [9]; textbook power electronics |
| 06 | Load Path (Tertiary Extraction) | Independent extraction of power from the primary field | Classical electromagnetics; standard transformer literature |
| 07 | Inverter & Output Conditioning | DC bus from tertiary rectifier feeds inverter producing standard AC waveform | Textbook power electronics |
| 08 | Boundary Closure | All boundary-crossing flows balance at the complete device boundary: P_in,boundary = P_load + P_losses + dE/dt (boundary-only; see § 6) | Classical thermodynamics |
No stage of the architecture lacks an independent literature anchor. The novelty of VENDOR.Max is not the existence of any single physical mechanism — every mechanism is documented. The novelty is the specific engineering integration of all eight stages into one device operating in the discharge-resonant regime at 2.45 MHz, with the BMS and Buffer as the stability control architecture that closes the regenerative loop.
This integration is what the patent family protects (ES2950176B2, WO2024209235A1). The patent grants certify that the integration is novel, disclosed, and inventive. The first physics-integration question — whether the assembled integration satisfies the regime-feedback inequality under load — is closable by independent boundary metrology. Every other stage has a class-level literature anchor and remains subject to device-specific engineering validation under independent metrology.
§ 15 — What remains proprietary
Effective capacitance and operating voltage of the regime nodes C2.1–C2.3. Internal geometry and microscopic conductivity mechanism of the sealed nonlinear conductivity cells. Effective quality factor of the regime-forming path under load. Coupling coefficient k_sec. Rectification topology, BMS operating-window logic, and Buffer capacity / sizing. Collapse threshold of the regime under load perturbation. Thermal and phase-stability characteristics under extended operation. Specific power level of the auxiliary supervisory input.
These parameters are Cat 4. They are documented internally and disclosed only under controlled technical review.
§ 16 — Honest experimental closure
The decisive closure of the Stage-one question requires independent boundary-calorimetric metrology under controlled third-party conditions. The closure protocol is: establish the regime via the discrete startup impulse; disconnect the startup port per patent claim 1; measure the capacitive-node state at C2.1–C2.3 over extended duration; measure induced feedback at the planar transformer secondary before and after rectification; measure the bidirectional flow through the BMS-controlled Buffer in both directions; measure return power into the capacitive nodes under BMS supervision; measure the regime-forming path losses calorimetrically and electrically; verify the inequality P_feedback ≥ P_loss + P_margin; apply controlled load perturbation through the output-extraction path under BMS priority enforcement and observe the Buffer dynamics.
§ 17 — Misconceptions: what this article does not claim
The article does not claim energy creation, overunity, perpetual motion, free energy, self-sustaining operation, or any deviation from conservation of energy. It does not claim that the startup port supplies the operating power of the device. It does not claim that the auxiliary supervisory boundary input is the regime-sustaining energy path.
It does not claim that the BMS or the Buffer creates energy. The BMS is a control element; the Buffer is a bidirectional energy storage element. Neither is a source.
It does not claim that 0.015 Wh of startup energy creates hundreds of watts of continuous flow. The startup energy initiates a regime; the regime operation is maintained through bounded intra-boundary energy circulation under BMS control within the complete-device boundary accounting framework, with the Buffer as bidirectional storage; the boundary equation closes through separately accounted boundary terms.
It does not claim that any single cited paper proves the VENDOR.Max implementation. The cited papers establish independent published support for the class-level physical mechanisms and engineering patterns required by the architecture.
It does not claim a specific microscopic conductivity mechanism inside the sealed cells. That mechanism is proprietary (Cat 4).
What this article does claim: the entire engineering implementation is interpretable within standard electrodynamics and standard power electronics with one integration node remaining unresolved as a physics question; that node reduces to a specific inequality; each physical building block has independent published support [1]–[9]; the order-of-magnitude pixel-budget is satisfiable within commonly reported parameter ranges; the apparent asymmetry between transient startup quantum and steady-state internal regime flow is resolved by recognising them as different categories of physical quantity; the BMS and the Buffer together form the textbook engineering solution to regenerative-oscillator stability, with literature precedent at least a century old; the entire architecture maps stage-by-stage to published literature in § 14; the integration question will be closed empirically through independent boundary metrology.
References
- E. Schüngel, S. Brandt, I. Korolov, A. Derzsi, Z. Donkó, J. Schulze. On the self-excitation mechanisms of plasma series resonance oscillations in single- and multi-frequency capacitive discharges.
- E. Schüngel, S. Brandt, Z. Donkó, I. Korolov, A. Derzsi, J. Schulze. Electron heating via the self-excited plasma series resonance in geometrically symmetric multi-frequency capacitive plasmas.
- J. R. Noesges, T. Mussenbrock. Nonlinear power absorption in geometrically asymmetric capacitively coupled plasmas and the role of plasma series resonance in beam-driven electron heating.
- S. K. Thagunna, V. I. Kolobov, G. P. Zank. Self-pulsing of dielectric barrier discharges at low driving frequencies.
- A. Shaygani, K. Adamiak. Self-synchronised Trichel pulse trains in multi-point corona discharge systems.
- A. Elkholy, E. van Veldhuizen, S. Nijdam, U. Ebert, J. van Oijen, N. Dam, L. P. H. de Goey. Characteristics of a nanosecond dielectric barrier discharge microplasma reactor for flow applications. Pulse energies: approximately 1.9 µJ and 2.7 µJ per channel.
- A. Kurs, A. Karalis, R. Moffatt, J. D. Joannopoulos, P. Fisher, M. Soljačić. Wireless power transfer via strongly coupled magnetic resonances. Science, 2007.
- E. H. Armstrong. Foundational work on regenerative and super-regenerative receiver architectures, establishing positive-feedback oscillation and the active runaway-prevention pattern. Some recent developments in the audion receiver (1915); Some recent developments of regenerative circuits, Proc. IRE (1922).
- Self-excited induction generator (SEIG) literature on capacitor-buffered self-excitation: the engineering pattern of a regenerative machine started by a small excitation and stabilised under varying load by a capacitor and battery buffer combination.
Frequently Asked Questions
What is the engineering classification of VENDOR.Max?
Armstrong-type nonlinear electrodynamic oscillator in a controlled discharge-resonant regime, governed by classical electrodynamics, patented under ES2950176B2 and PCT WO2024209235A1.
Does VENDOR.Max claim to violate conservation of energy?
No. The complete-device-boundary equation P_in,boundary = P_load + P_losses + dE/dt holds at all operational states. This equation applies at the complete device boundary only (Stage 08 of the eight-stage internal architecture); it cannot be used to compare any internal port (such as the 9 V startup port) to any internal output port (such as the kW-scale customer interface). See § 6 for the full reading rule.
How can a 0.015 Wh startup impulse be consistent with hundreds of watts of regime-feedback flow?
They are different physical quantities. The 0.015 Wh is a one-time transient energy that ignites the regime over about 15 seconds; the startup port is then disconnected. The hundreds of watts are steady-state internal energy circulation inside the formed regime — they do not cross the device boundary as a supply term. The boundary equation closes through separate terms.
If the startup port disconnects, what powers the device?
Sustained operation is governed by bounded intra-boundary energy circulation within the formed regime under Boundary Management System (BMS) supervisory authority over the Buffer, together with the separately accounted auxiliary supervisory control input. The auxiliary supervisory boundary input powers BMS, telemetry, and control functions only.
What does BMS stand for in VENDOR.Max, and how does it relate to the Buffer?
In VENDOR.Max, BMS denotes primarily Boundary Management System — the architectural control element that manages internal routing and operating-window stability through closed-loop metrology acquisition and real-time decision logic, during empirical evaluation of boundary closure at the complete device boundary. The BMS does not enforce conservation laws — conservation is a physical constraint that holds independently of any control element. The Buffer is a separate physical element — a bidirectional energy storage made of battery cells, DC-link capacitors, and active-rectification electronics — placed under BMS supervision. The BMS is the controller; the Buffer is the controlled storage. The acronym BMS is shared with the industrial term Battery Management System; that convention is preserved because the Buffer contains battery cells and standard battery-management functions are performed as a subordinate sub-function. The primary architectural role is boundary management, not battery management.
How does the Buffer prevent runaway in the regenerative architecture?
When the regime-feedback path delivers more power than the capacitive regime nodes require, the BMS routes the surplus into the Buffer and damps the regime slightly to prevent voltage rise. Without the Buffer, positive feedback would amplify until component failure or rail saturation — the classical runaway mode of regenerative oscillators identified by Armstrong in 1912 and solved in 1922 [8].
How does the Buffer prevent collapse under peak load?
When the output-extraction path draws heavily and the primary regime is loaded more than the feedback path can immediately replenish, the BMS draws stored energy from the Buffer and returns it to the capacitive regime nodes. The Buffer rides through the transient, preventing the regime from decaying.
Doesn't Townsend multiplication mean energy is multiplied?
No. Townsend multiplication is a conductivity effect that multiplies carrier count, which is dimensionless. Per-event energy is bounded by capacitive storage, E_event ≤ ½ C V².
Is the long runtime under operation evidence of perpetual motion?
No. Sustained operation under boundary-balanced conditions with a separately accounted supervisory control input and bidirectional buffer regulation is not perpetual motion. The architecture has boundary-crossing inputs at all operational states; sustained operation is supported by closed-loop control, not by an unbounded internal source.
Does the entire VENDOR.Max architecture have literature support stage by stage?
Yes. Every architectural stage maps to independent published literature: discharge physics (Schüngel [1][2], Noesges & Mussenbrock [3], Thagunna et al. [4], Shaygani & Adamiak [5], Elkholy et al. [6]); LC resonance and inductive coupling (Kurs et al. [7]); regenerative feedback and buffered stabilisation (Armstrong [8]; SEIG literature [9]); standard power electronics (textbook). § 14 of the article provides the full stage-by-stage map.
Has VENDOR.Max been independently validated?
VENDOR.Max has more than 1,000 hours of cumulative regime validation under internal testing. Independent third-party boundary-calorimetric metrology is the central milestone of the next-stage validation programme. See § 16 for the closure protocol.
Why can't I just put the 9 V startup voltage and the kW-scale customer output into the boundary equation and compute the device efficiency?
Because the boundary equation P_in,boundary = P_load + P_losses + dE/dt applies at the complete device boundary only — Stage 08 of an eight-stage internal architecture. The 9 V startup port lives at Stage 01 and is disconnected after ~15 s per patent claim 1. The kW-scale customer interface lives at Stage 07. The two are seven stages apart in the internal map, each governed by its own physical quantities (charge transport, per-event energy, induced EMF, per-stage efficiency, gap carrier dynamics). The boundary equation is a macroscopic sum-constraint, not a single-port-to-single-port ratio. Drawing such a ratio is a category error documented in § 6.