Technical Paper | Open Electrodynamic Systems

Regime-Level Energy Accounting
in Nonlinear Electrodynamic Systems:
An Event–Frequency Interpretation Framework

A two-layer energy accounting framework bridging discrete internal regime events and macroscopic power balance within classical Maxwell–Lorentz electrodynamics, applied to Armstrong-type nonlinear electrodynamic oscillators operating in a controlled discharge-resonant regime.

This paper formalizes a two-layer energy accounting framework for nonlinear electrodynamic systems operating through discrete regime events at high internal repetition frequency. At the complete device boundary, classical conservation applies: \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + \dfrac{dE_{\mathrm{stored}}}{dt}\). At the regime level, energy is redistributed across functional paths per event, linked to average power by \(P = E_{\mathrm{event}} \cdot f\). The framework provides an interpretive foundation for analysis of the VENDOR.Max platform — an Armstrong-type nonlinear electrodynamic oscillator at TRL 5–6.

A two-layer description is introduced. At the complete device boundary, conventional energy conservation applies. At the internal regime level, energy is redistributed across functional paths during each event and integrated over time through the event frequency. An analytical bridge between event-level energy and average power is established via the relation \(P_x = E_{x,\mathrm{event}} \cdot f\).

This framework is interpretive in scope and does not disclose implementation-specific design parameters, control logic, coupling geometry, protected parameter sets, or proprietary operating windows.

Authors O. Krishevich & V. Peretyachenko
Company MICRO DIGITAL ELECTRONICS CORP S.R.L. · vendor.energy
Published April 6, 2026
Updated July 7, 2026
Classification Boundary-constrained interpretation framework
TRL Status TRL 5–6 (laboratory validation)

§ 1 — Introduction

This paper defines a two-layer energy accounting framework for Armstrong-type nonlinear electrodynamic systems operating in a controlled discharge-resonant regime that redistribute energy through discrete internal regime events at high repetition frequency. At the complete device boundary, the framework imposes classical conservation: \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + \dfrac{dE_{\mathrm{stored}}}{dt}\). At the internal regime level, it organizes per-event redistribution across load, feedback, and loss channels, bridged to macroscopic average power by \(P_{x,\mathrm{avg}} = E_{x,\mathrm{event}} \cdot f\). Event-level quantities and boundary-level power balance describe distinct analytical layers of the same system and must not be conflated.

Nonlinear electrodynamic systems that operate in pulsed or regime-based modes — such as repetitive gas discharges, pulsed-power plasmas, and high-frequency streamer regimes — frequently exhibit dynamics that are not well captured by simple linear steady-state assumptions. In many experimental and evaluative contexts, attention is focused on the apparent energy associated with a single discharge or switching event, while the repetition frequency and duty cycle of these events are neglected or treated inconsistently. This practice often leads to systematic underestimation of achievable macroscopic power levels and to misinterpretation of device behavior, especially when events occur at kilohertz to megahertz rates.

Contemporary pulsed discharges and plasma-processing systems routinely operate with pulse repetition frequencies from kilohertz to tens of megahertz, and average powers ranging from watts to kilowatts. Experimental and modeling studies in high-repetition-rate discharges and pulsed laser–plasma interactions consistently demonstrate that the average power is determined by the product of the per-pulse (or per-event) energy and the repetition rate, with additional structure introduced by duty cycle, waveform shape, and loss channels.

The purpose of this work is to formalize an interpretation framework for analyzing observed operating behavior in regime-based electrodynamic systems, connecting event-level energy transfer, repetition frequency, and system-level power balance in a manner that is explicitly consistent with classical electrodynamics yet independent of any particular implementation. The framework emphasizes a two-layer description: a boundary level, where conventional conservation laws apply to the complete device, and a regime level, where internal discrete events redistribute energy among functional roles. The analysis clarifies the distinction between energy sourcing — which must be evaluated at the complete device boundary — and internal energy redistribution, which structures regime dynamics but does not itself define the net input power.

§ 2 — Two-Layer System Description

Layer 1 System Boundary Balance

Conventional energy conservation applied at the complete device boundary. The authoritative location for testing conservation and overall power accounting — independent of internal regime complexity.

Layer 2 Regime-Level Event Dynamics

Internal energy redistribution across functional paths during each discrete event. Describes regime organization — not energy sourcing. Constrained by and consistent with Layer 1.

Within the sitewide Three-Level Energy Model reference used across the VENDOR.Max glossary and interpretation framework, Layer 1 of this paper corresponds to Level 1 (macroscopic boundary accounting) and Layer 2 to Level 2 (per-event partition in the regime domain); the gap-physics material of § 4 belongs to Level 3 (gap-internal carrier dynamics). The two-layer presentation here is a local analytical device for the event–frequency bridge; it does not redefine the three-level ontology.

§ 2.1 — System Boundary Level

At the macroscopic level, the device is regarded as a black box with a complete device boundary across which net power is accounted for, an output load interface, and dissipative loss mechanisms. The energy balance for a volume \(V\) enclosing the system, with boundary surface \(S\), may be expressed through the standard integral form of electromagnetic energy conservation [1, 2]:

\[\frac{d}{dt}\int_V u_{\mathrm{em}}\,dV \;+\; \oint_S \mathbf{S}\cdot d\mathbf{A} \;+\; \int_V \mathbf{J}\cdot\mathbf{E}\,dV \;=\; 0\]
(1)

where \(u_{\mathrm{em}}\) is the electromagnetic energy density, \(\mathbf{S}\) is the Poynting vector, \(\mathbf{J}\) is the current density, and \(\mathbf{E}\) is the electric field. The surface integral represents the net electromagnetic power crossing the boundary; the volume integral of \(\mathbf{J}\cdot\mathbf{E}\) corresponds to the power delivered to charges within the system.

For a lumped description, the aggregate Level-1 accounting term for all electrical energy crossing the complete device boundary is written as:

Canonical Boundary Balance
\[P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + \frac{dE_{\mathrm{stored}}}{dt}\]
(2)

where \(P_{\mathrm{in,boundary}}\) is the total power accounted for at the device boundary, \(P_{\mathrm{customer}}\) is the power delivered to the external load, \(P_{\mathrm{losses}}\) accounts for irreversible losses within the system, and \(E_{\mathrm{stored}}\) is the stored electromagnetic and electrostatic energy in the device. Equation (2) is the appropriate reference for evaluating overall energy conservation and system-level power accounting, independent of internal regime organization. \(P_{\mathrm{in,boundary}}\) is an aggregate accounting quantity at the complete device boundary: it does not by itself imply a specific topology of continuous external supply, does not identify a single physical input port, and does not by itself identify or characterize the physical boundary-crossing processes responsible for that accounting — it is the accounting constraint, not a topology statement.

Under quasi-stationary operation, where macroscopic observables vary slowly compared to the characteristic energy storage time scales, \(dE_{\mathrm{stored}}/dt \approx 0\). The boundary-level power balance simplifies to:

\[P_{\mathrm{in,boundary}} \;\approx\; P_{\mathrm{customer}} + P_{\mathrm{losses}}\]
(3)

This expression is the correct location for testing conservation of energy and overall accounting, regardless of the complexity of the internal regime.

§ 2.2 — Regime-Level Description

Internally, many nonlinear electrodynamic systems may be described — for interpretive purposes — as operating through repetitive regime events: discrete internal events associated with energy redistribution across functional paths, characterized by rapid localized changes in field configuration and charge distribution, such as micro-discharges, streamer heads, or fast current commutations in pulsed inductive circuits.

For interpretive purposes, the energy associated with a single regime event may be decomposed into functional components:

Canonical Event-Level Balance
\[E_{\mathrm{extract,event}} = E_{\mathrm{customer,event}} + E_{\mathrm{fb,event}} + E_{\mathrm{loss,conv,event}}\]
(4)

where \(E_{\mathrm{customer,event}}\) denotes energy associated with transfer to useful output paths, \(E_{\mathrm{fb,event}}\) quantifies energy routed to self-stabilizing feedback processes (for example, sustaining a preionized state or biasing an internal resonator), and \(E_{\mathrm{loss,conv,event}}\) denotes irreversible dissipative losses such as collisional heating, resistive dissipation, and radiation that does not couple to the load.

Relation (4) is an internal bookkeeping statement that organizes how event-associated energy is partitioned during each discrete event; it does not, by itself, specify the total energy that must cross the external boundary to sustain the regime. The sourcing of \(E_{\mathrm{extract,event}}\) is governed by boundary-level power flows and energy storage dynamics as encapsulated in (2)–(3). System-level energy conservation must always be evaluated at the complete device boundary; event-level relations capture the internal organization of energy redistribution.

§ 3 — Event–Frequency Relation for Average Power

§ 3.1 — Discrete Event Representation

Consider a periodic or quasi-periodic sequence of discrete internal events with repetition frequency \(f\), such that events occur at times \(t_k = k/f\) for integer \(k\), and the energy associated with path \(x\) in the \(k\)-th event is \(E_{x,k}\). Over an observation interval \(T\) containing \(N = fT\) events, the total energy delivered through path \(x\) is:

\[E_x(T) = \sum_{k=1}^{N} E_{x,k}\]
(5)

The corresponding time-averaged power is:

\[P_x = \frac{E_x(T)}{T} = \frac{1}{T}\sum_{k=1}^{N} E_{x,k}\]
(6)

If event-to-event variations are small, one can define a characteristic event energy \(E_{x,\mathrm{event}}\) as:

\[E_{x,\mathrm{event}} = \lim_{N\to\infty}\frac{1}{N}\sum_{k=1}^{N} E_{x,k}\]
(7)

leading directly to the key bridge relation:

Event–Frequency Bridge
\[P_x = E_{x,\mathrm{event}} \cdot f\]
(8)

Equation (8) is the key bridge between microscopic (event-level) and macroscopic (average) descriptions, and it is the standard way to connect pulse energy, repetition rate, and average power in pulsed systems such as lasers and repetitive discharges [7, 8, 9].

For architectures in which events run over \(N_{\mathrm{ch}}\) parallel channels — in the VENDOR.Max architecture, \(N_{\mathrm{ch}} \geq 3\) parallel discharge channels with overlapping frequency spectra per patent claim 5 — the bridge relation generalizes to \(P_{x,\mathrm{avg}} = E_{x,\mathrm{event}} \cdot f \cdot N_{\mathrm{ch}}\), with the derivation above applying per channel. The channel count \(N_{\mathrm{ch}}\) is written with a subscript to distinguish it from the event count \(N = fT\) of equation (5).

§ 3.2 — Relation to Instantaneous Power Waveforms

An alternative representation begins from the instantaneous power waveform \(p_x(t) = v_x(t)\,i_x(t)\) associated with a given path. The energy per event is:

\[E_{x,\mathrm{event}} = \int_{t_k}^{t_k+\Delta t} p_x(t)\,dt\]
(9)

where \(\Delta t\) is the event duration, often much smaller than the period \(1/f\). For a perfectly periodic waveform, the time-averaged power over one period is:

\[P_x = \frac{1}{T_0}\int_0^{T_0} p_x(t)\,dt = \frac{E_{x,\mathrm{event}}}{T_0} = E_{x,\mathrm{event}} \cdot f\]
(10)

The distinction between peak power during an event and time-averaged power is particularly important in systems where peak powers can reach very high levels while average power remains in the kilowatt range.

§ 4 — Physical Basis of Event Formation in Gas Discharges

§ 4.1 — Townsend Ionization Framework

Many pulsed gas-discharge regimes relevant to this interpretive framework can be partially described — particularly at the discharge-initiation level — using Townsend-type ionization models [3, 4]. The first ionization coefficient \(\alpha\) quantifies the number of ionizing collisions per unit length experienced by an electron:

\[\alpha(E,p) = A\,p\,\exp\!\left(-\frac{B\,p}{E}\right)\]
(11)

where \(p\) is the gas pressure, \(E\) is the electric field strength, and \(A\), \(B\) are gas-dependent constants. For a uniform field in a gap of width \(d\), the electron population grows approximately exponentially with distance:

\[n(x) = n_0\,e^{\alpha x}\]
(12)

where \(n_0\) is the initial electron density at the entry of the gap. The derived carrier multiplication factor \(M_T = e^{\alpha d}\) (dimensionless, over an effective gap length \(d\)) completes the production-level canonical set of this framework: \(n(x)\), \(\alpha\), and \(M_T\). Carrier multiplication is a count, not an energy gain; per-event energy remains bounded by the capacitive reserve of the driving circuit.

These forms provide a classical reference framework for interpreting discharge initiation and event-scale field–charge evolution in pulsed gas-discharge regimes [3, 4]. Within the VENDOR.Max documentation they belong to the Townsend pre-breakdown framework of the 2023 patent disclosure (ES2950176B2 family) — the patent-baseline analytical formulation. The engineering implementation has advanced beyond that baseline; the working medium and microscopic mechanism of the current sealed switching cells are proprietary, and the forms above are not asserted as a measured description of any specific device.

§ 4.2 — Energy Associated with a Single Event

The electrical energy associated with an individual discharge event in a gas gap or a pulsed-power plasma structure is given by the time integral of the instantaneous power during the event:

\[E_{\mathrm{event}} = \int_{t_{\mathrm{start}}}^{t_{\mathrm{end}}} v(t)\,i(t)\,dt\]
(13)

where \(v(t)\) is the voltage across the discharge region and \(i(t)\) is the discharge current. For short, high-field events, \((t_{\mathrm{end}} - t_{\mathrm{start}})\) can be nanoseconds to microseconds, with strongly non-sinusoidal waveforms. Experimental and modeling studies report per-pulse energies ranging from microjoules to several joules, depending on geometry, gas mixture, and applied voltage.

§ 5 — Electromagnetic Energy Transfer to an Extraction Circuit

§ 5.1 — Inductive Coupling and Faraday’s Law

In many practical realizations, energy stored in an internal electrodynamic regime is coupled to an extraction circuit via electromagnetic induction, capacitive coupling, or a combination thereof. For inductive coupling, the instantaneous electromotive force (EMF) induced in a coil of \(N\) turns linked by magnetic flux \(\Phi(t)\) is Faraday’s law in lumped form [1, 2]:

\[\mathcal{E}(t) = -N\,\frac{d\Phi}{dt}\]
(14)

When the induced EMF is applied across a load with current \(i(t)\), the instantaneous power delivered to the load is:

\[p_{\mathrm{customer}}(t) = v_{\mathrm{customer}}(t)\,i(t)\]
(15)

The time-averaged power delivered to the load over an interval \(T\) is:

\[P_{\mathrm{customer}} = \frac{1}{T}\int_0^T v_{\mathrm{customer}}(t)\,i(t)\,dt = \bigl\langle v_{\mathrm{customer}}(t)\,i(t)\bigr\rangle\]
(16)

§ 5.2 — Consistency with Boundary-Level Energy Accounting

The inductive energy transfer described by (14)–(16) is a local manifestation of the global energy balance expressed by (1)–(3): changes in magnetic flux correspond to reconfiguration of electromagnetic field energy, and the product of EMF and current represents the rate at which field energy is converted to work on charges in the extraction circuit.

In the global picture, the Poynting vector flux across the device boundary equals the net power entering or leaving the system, while internal field reconfigurations — including inductive coupling to coils — redistribute energy among internal and external degrees of freedom. The complete device boundary power balance (2)–(3) remains the authoritative statement regarding overall energy conservation; the sum over all events and all paths is constrained by the total net input.

§ 5.3 — Measurement and Boundary-Level Verification

Correct evaluation of nonlinear regime-based electrodynamic systems requires measurement at the complete device boundary, not at internal nodes or sub-circuits. Internal nodes carry quantities that belong to Layer 2 (regime-level redistribution) and cannot, on their own, characterize the Layer 1 input–output balance. The authoritative reference for testing energy conservation is the enclosing surface defined in equations (1)–(3): \(P_{\mathrm{in,boundary}}\) referenced at the complete device boundary as an aggregate accounting quantity, and \(P_{\mathrm{customer}}\) at the external load interface.

At the complete device boundary, the boundary-crossing inventory comprises all physical channels: conducted electrical terms, thermal flows, radiative losses, and field-mediated interaction with the surrounding medium. Boundary closure is verified against the complete inventory — not against the electrical port list alone.

At regime-level operation with high internal repetition frequency, instantaneous voltage and current waveforms at any internal node can exhibit non-sinusoidal, sharply discretized features. These waveform features describe regime structure; they do not, by themselves, define power. Time-averaged power is recovered through the integral \(P = \langle v(t)\,i(t)\rangle\) over an interval much longer than the event period \(1/f\), or equivalently through the bridge relation \(P = E_{\mathrm{event}} \cdot f\) defined in equation (8). Reading peak values directly as power, or comparing instantaneous waveform amplitudes between internal nodes and the complete device boundary, is a category error: peak power and time-averaged power are distinct quantities, and only the latter participates in the boundary balance.

Consequently, no measurement at an internal node — the regulated feedback path, the capacitive node, or any intermediate winding terminal — can replace boundary-level measurement of \(P_{\mathrm{in,boundary}}\) and \(P_{\mathrm{customer}}\). Internal measurements characterize regime organization; boundary measurements characterize energy accounting. Both are meaningful within their respective layers, but only the latter answers the conservation question. Verification of overall energy balance is performed exclusively at the complete device boundary under time-averaged conditions consistent with equations (2)–(3) and (8).

§ 6 — Illustrative Frequency-Domain Example

Non-Design-Specific Example

Parameters used in § 6 are illustrative and deliberately non-design-specific. No claim is made that values shown constitute disclosed operating parameters of any particular implementation. The example applies the identity \(P = E_{\mathrm{event}} \cdot f\) and boundary-level conservation law (3) only. The values are not a prediction or specification of VENDOR.Max performance; the calculation is an order-of-magnitude consistency check of the bridge relation, treating the event stream as a single aggregate sequence. Actual device parameters remain protected.

§ 6.1 — Parameter Selection

To illustrate the relationship between event energy and macroscopic power, consider a representative example with event repetition frequency:

\[f = 2.45\times 10^{6}\,\mathrm{s}^{-1}\]
(17)

and a target average load power of:

\[P_{\mathrm{customer}} = 4\,\mathrm{kW}\]
(18)

Here, the frequency refers to internal regime-level electrodynamic processes and must not be confused with the inverter output frequency or external load-interface frequency. Using the general relation (8), the characteristic energy per event delivered to the load is:

\[E_{\mathrm{customer,event}} = \frac{P_{\mathrm{customer}}}{f} = \frac{4\times 10^{3}}{2.45\times 10^{6}} \approx 1.63\times 10^{-3}\,\mathrm{J}\]
(19)

Thus, a load power of 4 kW corresponds to event-scale load energies on the order of a few millijoules when events repeat at multi-megahertz internal regime frequencies.

§ 6.2 — Inclusion of Feedback and Loss Channels

The total event-level extraction energy is partitioned into customer delivery, regulated internal feedback, and conversion losses — see equation (4). The extended decomposition:

\[E_{\mathrm{extract,event}} = E_{\mathrm{customer,event}} + E_{\mathrm{fb,event}} + E_{\mathrm{loss,conv,event}}\]
(20)

Over many events, the corresponding average powers are:

\[P_{\mathrm{extract}} = E_{\mathrm{extract,event}}\cdot f, \quad P_{\mathrm{fb}} = E_{\mathrm{fb,event}}\cdot f, \quad P_{\mathrm{losses}} = E_{\mathrm{loss,conv,event}}\cdot f\]
(21)

Under quasi-stationary conditions after regime stabilization, the boundary-level balance (3) implies:

Boundary Invariance
\[P_{\mathrm{in,boundary}} \approx P_{\mathrm{customer}} + P_{\mathrm{losses}} = \bigl(E_{\mathrm{customer,event}} + E_{\mathrm{loss,conv,event}}\bigr)\cdot f\]
(22)

Equation (22) emphasizes that while the power associated with the regulated internal feedback path is part of the internal regime organization, it does not constitute an independent net energy source; its existence is constrained by the net input power and the energy stored in the system. Equivalently, boundary-level accounting closes for any quasi-stationary regime: internal feedback redistribution neither adds a boundary input term nor relaxes the closure constraint. The verification metric is the conservation closure residual — the requirement that the terms of equation (2) sum to zero within measurement uncertainty under accredited metrology.

§ 6.3 — Interpretation

The numerical example demonstrates that macroscopic kilowatt-scale power levels are entirely compatible with millijoule-scale per-event energies when the repetition frequency of internal regime processes is in the megahertz range. Conversely, examining only the per-event energy without accounting for \(f\) underestimates the continuous average power by the event-frequency factor itself; for the parameters of § 6.1, that factor is approximately \(2.45 \times 10^6\). This is precisely the type of misinterpretation the present framework is designed to correct.

§ 7 — Interpretation Principles

The two-layer framework yields four principles essential for correct interpretation of experimental data and system behavior in nonlinear, regime-based electrodynamic systems.

Principle 1 Event energy must be evaluated together with repetition frequency.

Per-event energy \(E_{\mathrm{event}}\) must always be interpreted in conjunction with the event frequency \(f\) to obtain average power via \(P = E_{\mathrm{event}} \cdot f\). Neglecting \(f\) conflates microscopic and macroscopic scales.

Principle 2 Internal energy redistribution does not represent total system input.

The decomposition (4) describes internal energy partitioning, but the net sourcing of this energy is constrained by the boundary-level balance (2)–(3). The regulated internal feedback path does not constitute an independent net energy source.

Principle 3 System-level energy balance must be evaluated at the complete boundary.

The correct location for testing conservation of energy is the enclosing surface of the physical device. Internal surfaces or subvolumes can exchange energy with each other without violating global conservation.

Principle 4 Event-level relations describe regime organization, not energy sourcing.

Relations such as (4), (11)–(13), and (20) characterize how the regime organizes field and particle dynamics during individual events. They do not, on their own, determine the net power that must be accounted for at the device boundary to sustain the regime.

Failure to distinguish these layers leads to erroneous comparisons between event energy and continuous power, to apparent contradictions with conservation of energy, and to incorrect extrapolations of experimental results.

§ 7.5 — Interpretation Boundaries and Common Failure Modes

Beyond the four principles of § 7, five specific analytical failure modes recur in evaluations of regime-based electrodynamic systems. Each failure mode shares a common structural origin: implicit conflation of analytical layers. The two-layer framework defined in § 2 makes this conflation explicit and corrigible. These interpretation boundaries are not additional physical assumptions but constraints on correct analytical mapping between already defined layers.

Failure Mode F1 · Layer Conflation Between Event and Power

A direct comparison between \(E_{\mathrm{event}}\) and continuous power without accounting for the repetition frequency \(f\) constitutes a category error — a mismatch of analytical layers. Per-event energy is a Layer 2 quantity; continuous power is a Layer 1 quantity. The only valid translation between the two is the bridge relation \(P_x = E_{x,\mathrm{event}} \cdot f\) defined in equation (8). Comparing them directly, without the frequency aggregation, is not a physics conclusion but a layer-mapping error.

Failure Mode F2 · Feedback Path Misclassified as Energy Source

Internal regime-level redistribution is already accounted for within \(P_{\mathrm{in,boundary}}\). The feedback path is a regulated redistribution route within the formed regime; it does not contribute net energy across the complete device boundary. \(E_{\mathrm{fb,event}}\) and its time-averaged counterpart \(P_{\mathrm{fb}}\) describe how a fraction of extracted energy is routed back to sustain the operating regime — analogous to regulated internal recirculation or bias-maintenance processes within an already formed oscillatory regime. Treating \(P_{\mathrm{fb}}\) as an independent energy source is a Layer 2 quantity misinterpreted as a Layer 1 input.

Failure Mode F3 · Startup Impulse Misinterpreted as Steady-State Source

The startup impulse belongs exclusively to the regime initiation phase and is temporally decoupled from steady-state operation. It does not contribute to sustained power delivery and must not be included in steady-state energy accounting. The two stages are governed by distinct energy regimes: regime initiation is a one-time bounded event (in the VENDOR.Max platform, approximately 9 V across approximately 15 seconds, delivering on the order of 0.015 Wh of total energy); steady-state operation is governed by the complete device-boundary balance \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + dE_{\mathrm{stored}}/dt\). Conflating the two produces apparent paradoxes that dissolve once the temporal separation is recognized.

Failure Mode F4 · Interaction Medium Misclassified as Energy Source

The surrounding gas, atmospheric air, or plasma medium provides boundary conditions for regime formation — ionization thresholds, breakdown criteria, and collision dynamics — and does not function as a source of energy at any timescale. The medium structures the regime; it does not source it. All net energy is accounted for through the complete device boundary balance in equation (2). Reading regime activity in the medium as autonomous energy production is a misclassification of interaction medium as input source.

Failure Mode F5 · Boundary Equation Misread as Topology

The boundary equation (2) is an accounting constraint at the complete device boundary; it does not identify which physical port carries inbound flow at any instant, does not assert a continuous external supply line, and does not equate any single input port with any single output port. Reading \(P_{\mathrm{in,boundary}}\) as a topology claim — a supply cable that must exist somewhere in the diagram — converts a Layer 1 bookkeeping term into a circuit statement. The startup port is a one-time initialization interface, disconnected after regime formation; the identification and quantification of the flows crossing the complete device boundary is the subject of independent boundary metrology, not of inference from the equation’s form.

All five failure modes share a common structural origin: implicit layer conflation. Each is corrected by the same procedural discipline — identify which analytical layer the question belongs to, then apply the correct formula for that layer. The framework provides this procedural discipline; the failure modes diagnose what happens when it is omitted.

§ 7.6 — Energy Transformation Map: Stage × Quantity

The interpretation principles of § 7 and the failure modes of § 7.5 can be compressed into a single map. The rows below follow the eight-stage patent sequence of the VENDOR.Max architecture, documented in full at How VENDOR.Max Works; this article does not restate the stage mechanics — it maps which physical quantity is calculable at which stage. Quantities live at different analytical levels — complete device boundary (macroscopic accounting), per-event partition (regime domain), and gap-internal carrier dynamics — and carry different units. The carrier-dynamics column refers to the Townsend pre-breakdown forms of the patent-baseline analytical framework (ES2950176B2 family, priority 2023); the engineering implementation has advanced beyond that baseline, and the microscopic mechanism of the sealed switching cells is not disclosed. Boundary closure in the final column is verified through the conservation closure residual Rboundary — the requirement that the terms of equation (2) sum to zero residual within measurement uncertainty under accredited metrology.

Energy Transformation Map · Stage × Quantity

What is calculable where — and why one efficiency ratio cannot describe the whole device

Each stage of the architecture is governed by a different physical quantity. Charge transport, per-event energy, continuous power, field work, induced EMF, per-stage converter η, gap carrier dynamics, and boundary closure are not the same kind of object — they live at different analytical levels and in different units. The matrix below shows, for each of the eight patent stages, which quantities are directly defined, which are conditional (require a bridge equation or describe a state variable), and which would be a category error if applied at that stage.

directly defined at this stage conditional · bridge / state / causal condition × category error if applied here
Stage
Q Charge · Coulomb
E Energy · Joule
P Power · Watt
W Field work · ∫U·i dt
ε EMF · −dΦ/dt
η Per-stage
n(x) Carrier dyn.
Rb Boundary closure
STAGE 01 Startup Impulse
Q = C·Vbreak
~0.015 Wh one-time
× event, not flow
× charging only
×
× no converter formalism
×
boundary event quantum
STAGE 02 Discharge & Regime Formation
ΔQ per event
Eevent ≤ ½CV2
bridge: P = E·f·N
W = ∫U·i dt
× primary only, not induced yet
× partition, not conversion
n(x) = n0·exp(αx)
× internal event
STAGE 03 Primary Field & Non-Galvanic Coupling
× no carrier transport in core
stored: ½LI2
×
× no carriers here
causal: dΦ/dt drives induction
× field is coupling, not converter
×
× internal field
STAGE 04 Parallel Faraday Induction
× induction, not transport
Esec,event + Etert,event
bridge equation required
× no gap carriers
ε on (7) and (10) in parallel
× no combined η for two paths
×
× internal partition
STAGE 05 Feedback Path · Secondary (7)
recharge storage capacitors
Efb,event
bridge: Pfb = Efb·f·N
×
at winding (7)
ηsec_path, ηrect 17/18/19
×
× regime-domain only
STAGE 06 Load Path · Tertiary (10)
through rectifier (12)
Etert,event
at DC bus, not customer side
×
at winding (10)
ηtert_path, ηrect 12
×
× pre-boundary stage
STAGE 07 Inverter & Output Conditioning
× continuous AC, not event Q
× no event partition here
Pcustomer = ⟨V·I⟩ real
×
× past induction stage
ηinverter, ηfilter
×
× pre-boundary stage
STAGE 08 Boundary Closure
× aggregated into P terms
dEstored/dt — stored-state variation
Pin,b, Pcustomer, Plosses
× internal gap-level quantity
× aggregated upstream
× per-stage values only, no global η
× gap-internal, not boundary
Rboundary → 0

What the matrix shows. No stage-level quantity remains directly defined across all eight rows. The only quantity that holds end-to-end is the boundary equation itself (Pin,boundary = Pcustomer + Plosses + dEstored/dt, with the conservation closure residual Rboundary → 0 under accredited metrology) — defined only at Stage 08. A single end-to-end efficiency ratio cannot be assembled from the per-stage η column because the chain spans charge transfer, per-event energy partition, field storage, induction, and continuous power across different units and analytical levels. Each stage is calculable on its own terms; the device closes at the boundary.

§ 8 — Discussion

§ 8.1 — Clarifying the Event–Power Misinterpretation

A recurring analytical inconsistency in the evaluation of pulsed and regime-based electrodynamic systems is the direct comparison of the energy observed in a single event with the continuous power rating of the load or power supply, ignoring the role of repetition frequency. For instance, observing a per-event energy on the order of millijoules may be incorrectly judged as incompatible with kilowatt-scale average power; under the identity \(P = E_{\mathrm{event}} \cdot f\), the two scales are consistent whenever \(f\) lies in the megahertz range, as illustrated by the § 6.1–§ 6.2 example.

The present framework clarifies this inconsistency by explicitly embedding event-level quantities in the time-averaged power relation (8) and anchoring the entire description in the boundary-level conservation law (2)–(3). When this structure is respected, no contradiction arises between discrete, nonlinear internal dynamics and classical energy conservation; instead, the system is seen as a nonlinear electrodynamic system with internally organized repetitive energy-transfer processes through which boundary-accounted energy is redistributed into useful output and losses.

Misinterpretation of regime-based systems typically arises from implicit layer conflation — treating event-level quantities as boundary-level power descriptors. The present framework eliminates this ambiguity by enforcing strict analytical separation between Layer 1 (boundary) and Layer 2 (regime), with the bridge relation \(P = E_{\mathrm{event}} \cdot f\) governing the only valid translation between the two. The five failure modes catalogued in § 7.5 each instantiate this structural error in a specific analytical context.

§ 8.2 — Consistency with Classical Electrodynamics

All elements of the framework are consistent with standard macroscopic electrodynamics and plasma physics. Boundary-level power balances and Faraday induction govern energy flow and coupling at the terminals and in the extraction circuits. Townsend-type ionization theory, together with related criteria and modern global models, provides a classical reference framework for describing the formation, growth, and quenching of avalanche and streamer events in gases.

High-power pulsed experiments across lasers and discharges provide extensive empirical evidence that the relation between per-event energy, repetition rate, and average power is quantitative and robust across many orders of magnitude in energy and frequency.

§ 8.3 — Scope and Limitations

The framework presented here is deliberately agnostic with respect to implementation-specific details such as electrode geometry, control electronics, and proprietary coupling structures. It therefore applies to a broad class of systems but does not by itself predict optimal designs or performance limits for a given architecture. The framework also makes no claim that any surrounding gas, atmospheric air, or plasma medium functions as an energy source; such media participate exclusively as interaction media that provide boundary conditions for regime formation, with all net energy accounted for at the device boundary through (2).

Moreover, while the event–frequency relation (8) is exact for periodic or stationary statistics, strongly nonstationary regimes — for example, during startup, shutdown, or transitions between discharge modes — require explicit time-domain treatment using (1), (2), and (13) without assuming a single characteristic \(E_{\mathrm{event}}\). In such regimes, the two-layer interpretation remains valid conceptually but the quantitative mapping from event energies to average power becomes time-dependent.

§ 8.4 — Limits of Linear Evaluation Models

A linear \(P_{\mathrm{in}}\)-to-\(P_{\mathrm{out}}\) evaluation implicitly assumes continuous, time-invariant transfer between input and output at the same boundary, with no internal regime structure mediating the relationship. This assumption holds for converters and amplifiers operating in their linear regime, where the input–output relation can be characterized by a single transfer function and steady-state efficiency. It does not hold for systems where energy transfer is discretized into high-frequency nonlinear events with internal redistribution paths.

Applying linear steady-state assumptions to regime-based systems collapses the two analytical layers defined in § 2 into a single linear model, removing both the event–frequency aggregation defined in equation (8) and the internal redistribution structure defined in equation (4). The result is systematic underestimation when event frequency is high relative to the observation timescale, or misclassification when internal feedback paths are read as independent inputs. The linear model is not wrong by itself — it is correctly applied to the system class for which it was developed; misapplication to nonlinear regime-based systems produces interpretive errors of the kind catalogued in § 7.5.

§ 9 — Conclusion

A two-layer interpretation model for nonlinear, regime-based electrodynamic systems has been developed, connecting discrete energy-redistribution events with macroscopic power output through a frequency-domain perspective anchored in classical electrodynamics. At the complete device boundary, standard conservation laws enforce energy accounting and define the net power balance, while internally, event-level relations describe how event-associated energy is partitioned among load, feedback, and irreversible loss channels.

By formalizing the relation \(P_x = E_{x,\mathrm{event}} \cdot f\) — with its parallel-channel generalization \(P_{x,\mathrm{avg}} = E_{x,\mathrm{event}} \cdot f \cdot N_{\mathrm{ch}}\) — and embedding it in a consistent boundary-level energy balance, the framework eliminates a common source of misinterpretation in the evaluation of pulsed and regime-based systems — namely, the direct comparison of event energy to continuous power without accounting for event frequency. The illustrative example shows explicitly how millijoule-scale events at multi-megahertz internal regime frequencies correspond to kilowatt-scale average power delivery, fully within the bounds of classical energy conservation.

This interpretation framework is intended as a tool for analyzing and communicating experimental results in nonlinear electrodynamic systems, providing a mathematically consistent and physically transparent connection between internal regime dynamics and system-level performance. It provides the scientific foundation for the VENDOR.Max platform — an Armstrong-type nonlinear electrodynamic oscillator at validation stage TRL 5–6 — while remaining independent of implementation-specific disclosure, protected design details, and proprietary operating parameters.

Beyond defining the relation between event-level energy and macroscopic power, the framework establishes strict interpretation boundaries preventing systematic category errors, including: (i) event-to-power miscomparison without frequency aggregation, (ii) feedback misclassification as net energy source, (iii) startup-impulse misinterpretation as steady-state input, (iv) interaction-medium misclassification as energy source, and (v) misreading of the boundary equation as a supply-topology statement rather than an accounting constraint at the complete device boundary. Each boundary is enforced by the two-layer accounting structure and its canonical bridge relation \(P_x = E_{x,\mathrm{event}} \cdot f\).

The present framework defines the correct interpretation model for regime-based electrodynamic systems. It does not, by itself, constitute experimental proof of any specific implementation. Empirical validation of operating performance is addressed separately through controlled testing, time-averaged measurements at the complete device boundary in the sense of § 5.3, and independent third-party verification protocols associated with the certification pathway toward TRL 7–8. The framework and the empirical validation programme are complementary but analytically distinct: this article specifies the language of correct evaluation; the validation programme specifies the data.

Open-System Boundary Doctrine

(a) Inside the boundary — closure is physically enforced. Within the complete device boundary, energy accounting closes at all operational states: \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + dE_{\mathrm{stored}}/dt\). A sustained boundary-level imbalance is not an available operating condition of the architecture — it would manifest as regime runaway or regime decay. (b) Across the boundary — identification is a metrology question. The identification and quantification of the flows crossing the complete device boundary is the subject of independent boundary metrology under accredited protocol — the TRL 6 validation milestone, with four committed outcomes, including the possible identification and quantification of previously unresolved flows crossing the complete device boundary. (c) Implementation — an engineering disclosure question. The engineering means by which the architecture organizes its operating regime and its boundary flows are protected know-how, subject to controlled disclosure within the TRL 8 certification pathway.

Disclosure Statement

This paper presents an interpretation framework for observed behavior of nonlinear electrodynamic systems and does not disclose implementation-specific architecture, control logic, coupling geometry, protected parameter sets, or proprietary operating windows. It is intended solely to clarify the relationship between event-level regime dynamics and macroscopic power balance within the constraints of classical electrodynamics.

Frequently Asked Questions

Does this framework claim that output exceeds input?

No. The framework is explicitly anchored in boundary-level energy conservation: \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + dE_{\mathrm{stored}}/dt\). Both analytical layers — boundary and regime — are required for a complete description. Neither layer, alone or combined, produces a result where output exceeds device-boundary input. At the complete device boundary, accounting closes for any steady-state regime, and internal regime-level redistribution does not relax this closure constraint.

What does the internal feedback path represent?

The regulated internal feedback path — denoted \(E_{\mathrm{fb,event}}\) per event and \(P_{\mathrm{fb}}\) on average — routes a fraction of extracted energy back to sustain the operating regime, analogous to regulated internal recirculation or bias-maintenance processes within an already formed oscillatory regime. It is a regulated redistribution route within a formed regime, not an independent energy source and not a positive-feedback amplifier. Its power contribution is included within \(P_{\mathrm{in,boundary}}\) and is constrained by the total net input at the device boundary.

How does per-event energy relate to kilowatt-scale output?

Through the identity \(P = E_{\mathrm{event}} \cdot f\), applied over the repetition frequency of the internal regime. At megahertz event rates, per-event energies in the millijoule range can correspond to kilowatt-scale average power: for example, 1.63 mJ per event at 2.45 MHz corresponds to 4 kW of average load power (see § 6.1–§ 6.2). Evaluating \(E_{\mathrm{event}}\) without accounting for \(f\) therefore yields an incomplete model and can underestimate the continuous average power by the event-frequency factor — a systematic error that this framework identifies and corrects.

What is the startup impulse in practice, and how does it relate to sustained operation?

The startup impulse initiates the nonlinear regime but does not itself power the load. In the VENDOR.Max platform, startup uses approximately 9 V for approximately 15 seconds, delivering on the order of 0.015 Wh of total energy, after which the startup source is disconnected. Once the regime is formed, all energy crossing the complete device boundary is accounted for through \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + dE_{\mathrm{stored}}/dt\); the regime-level feedback path redistributes energy internally within that bound. The startup impulse belongs to the startup stage; steady-state operation is governed by complete device-boundary accounting. The two stages must not be conflated.

Does the surrounding gas or air function as an energy source?

No. The surrounding gas, atmospheric air, or plasma medium participates exclusively as an interaction medium that provides boundary conditions for the formation of regime events (ionization thresholds, breakdown criteria, and collision dynamics). It is not fuel, not a consumable, and not an energy source. All net energy is accounted for through the device boundary balance in equation (2). The medium structures the regime; it does not source it.

Does this framework apply to the VENDOR.Max system?

Yes. This framework presents the interpretive model that applies to the VENDOR.Max operating architecture. VENDOR.Max is an Armstrong-type nonlinear electrodynamic oscillator internally validated at TRL 5–6 with more than 1,000 cumulative operational hours, including a 532-hour continuous regime operation segment; the full operating record is documented on the Endurance Test page. Patent context (six-jurisdiction family, common priority date 05.04.2023): WO2024209235A1 (PCT international publication, family anchor); ES2950176B2 (granted, Spain/OEPM, first granted patent); EP4693872A1 (Europe, EPO, under examination); US20260088633A1 (United States, USPTO, under examination); CN119096463A (China, CNIPA, under examination); IN 202547010911 (India, IPO, under examination); EUTM 019220462 (EU trademark, EUIPO, registered). Specific operating parameters, coupling geometry, and control logic are not disclosed at the current pre-commercial validation stage.

Why is a linear Pin-to-Pout evaluation insufficient for this class of system?

A linear Pin-to-Pout model assumes a single steady-state boundary input mapped directly to a steady-state load, with no internal regime structure. In nonlinear electrodynamic systems, energy is transferred through discrete high-frequency regime events, and observables such as waveforms, instantaneous voltage, and current are strongly non-sinusoidal. A linear evaluation either averages away the regime structure or compares event-level quantities directly to continuous power, producing systematic misinterpretation. The two-layer framework presented here resolves this inconsistency explicitly.

Why is a single whole-device efficiency ratio not the right diagnostic for this architecture?

Per-stage efficiencies remain valid and necessary — each converter block in the rectification and inversion chain has a well-defined \(\eta\) bounded below unity. A single whole-device ratio, however, would divide quantities that belong to different boundary interfaces and different analytical layers: the startup port is a one-time initialization interface, the internal event partition is a Layer 2 quantity, and customer delivery is a Layer 1 term. The correct Layer 1 verification instrument is conservation closure at the complete device boundary — the requirement that the terms of equation (2) sum to zero residual within measurement uncertainty under accredited metrology. The full due-diligence treatment of the efficiency-multiplication objection is given in Where Is the “Plus”? — the due-diligence answer.

What prevents this framework from being classified as perpetual motion?

The startup impulse initiates the regime; all subsequent operation is governed by the complete device-boundary energy balance \(P_{\mathrm{in,boundary}} = P_{\mathrm{customer}} + P_{\mathrm{losses}} + dE_{\mathrm{stored}}/dt\). Any increase in extracted output requires a corresponding increase in power accounted for at the device boundary, subject to dissipative losses. The regulated internal feedback path redistributes energy within the boundary bound, not across it. The system is an open electrodynamic architecture operating within classical electrodynamics, not a closed-loop autonomous device, and therefore cannot be classified as a perpetual-motion system by definition.

Does this framework, by itself, prove that VENDOR.Max works?

No. This framework is an interpretation model — it specifies the correct language for reasoning about energy balance in regime-based nonlinear electrodynamic systems. Empirical validation of the VENDOR.Max platform is supported separately through the validation dataset (TRL 5–6; the operating record is documented on the Endurance Test page). Independent third-party verification through a qualified accredited pathway is the next validation stage. The framework and the empirical validation are complementary but distinct.

References

Primary · Peer-reviewed / Canonical Monographs
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