Where Does the Energy Come From
Energy is delivered to the output ensemble of VENDOR.Max by the coupled electromagnetic field of the discharge-resonant regime. The electric component of that field does work on the pickup path’s own charge carriers, producing a measurable electromotive force and an energy flow at its port.
POWER = CHARGE FLOW × ENERGY PRICE PER COULOMB
The direct physical mechanism by which electrical energy is delivered to the output path of VENDOR.Max.
How to read this pageThe question “where does the energy come from?” has two levels. At the level of the operating regime, VENDOR.Max answers it directly: the battery initiates the regime; after startup the regime branch sustains a positive input flow through the Frame 1 port; discharge-resonant conversion and the coupled field form a new charge flow in the pickup path with a defined energy price per coulomb; at the established DC port their product is expressed as power, which is divided between sustaining the next operating cycle and the customer output. Frame 0 consolidates the overall exchange of the product with its environment and does not replace this account of the physical mechanism. The mechanism of energy transfer to the output ensemble and the final energy attribution of the complete product are two different physical tasks: the first is established at the level of the operating regime, the second only by full measurement at Frame 0, and it cannot be derived from the topology of the internal circuits.
The page coversThe initial state of the charge carriers; the energy price per coulomb; the work done by the electric field component on the charge carriers; energy transfer between galvanically separated charge ensembles; the distinction between the working core and the outer boundary; the closing of the customer charge circuit when a load is connected; the difference between the boundary of the product and the boundary of the coupled working topology; the list of what is not a source.
The page establishesThe principle of moving from a charge-domain description to an energy-domain quantity at an established electrical port; an illustrative decomposition of the local conversion coefficient into the change in charge flow and the change in the energy price per coulomb; the division of the formed flow between sustaining the operating regime and the customer output; the fact that a connected load becomes a new circuit of the coupled topology and that its impedance becomes an internal boundary condition of the regime, without creating a continuing external energy input through Frame 0.
The page does not establishThe transfer route stage by stage; the protected internal topology; the quantitative balance of the working core; the real internal operating values of charge flows, voltages and coefficients; the final energy attribution of the product; certified characteristics.
The short answer
VENDOR.Max is a nonlinear electrodynamic device operating in a controlled discharge-resonant regime. Under the project’s functional classification, excitation of the coupled resonant regime is classified as Armstrong-type discharge-resonant excitation; this designation applies only to the excitation stage and does not classify the device as a whole. The term “Armstrong-type” denotes here a topological feature of the excitation stage — positive feedback between coupled circuits — and does not imply that VENDOR.Max uses the complete power-supply arrangement of the classical vacuum-tube device.
The device does not create electrons, and no continuous carrier stream passes through all stages of the device. It organises electromagnetic coupling between several galvanically separated charge-carrier ensembles. Energy is transferred across the coupling region by the electromagnetic field; the electric-field component organises the motion of the carriers on the receiving side and does work on them. The resulting electromotive force sets the energy price per coulomb for directed charge transport. Rectification and power conversion turn the alternating energy exchange into a controlled energy flow to the load.
This is an answer at the same explanatory level as for any other electrical device.
| System | What sustains the process energetically | How the energy reaches the output carriers |
|---|---|---|
| Solar panel | The energy of the absorbed photons | The internal field separates the carriers and enables their extraction |
| Electromechanical generator | The mechanical work of the drive | The induced electric field does work on the winding’s carriers |
| Transformer | The energy supplied through the primary port | The coupled electromagnetic field transfers the energy to the secondary ensemble |
| VENDOR.Max | The positive input power flow through the Frame 1 port, sustained after startup by the internal regime-feedback branch | The coupled field of the discharge-resonant regime transfers the energy to the pickup path; the electric field component does work on its own charge carriers |
The table separates the direct sustaining of the operating regime from the mechanism of energy transfer to the output carriers. For VENDOR.Max, the input flow through the Frame 1 port directly supplies the excitation node; the coupled field transfers the energy to the charge-carrier ensemble of the pickup path; after rectification the formed flow is divided between the regime branch and the customer branch. At the level of the complete product, the feedback loop remains an internal transfer and is not an independent external source.
Energy reaches the working output as a result of field transfer and of the work done by the electric field component on the charge carriers — not as a result of new charges appearing, not from frequency in itself, and not from the arithmetic multiplication of incomparable readings.
The battery initiates the operating regime, but its startup flow does not pass sequentially through the whole device to the consumer. After startup, the internal regime-feedback branch sustains the Frame 1 input. The discharge-resonant regime organises the charge circulation, and the coupled electromagnetic field does work on the pickup path’s own charge carriers and sets the energy price per coulomb for their directed transport. At the established DC port, the charge-domain description is converted into power: coulombs per second are multiplied by joules per coulomb. Part of the resulting flow sustains the next operating cycle; the remaining available part goes to the consumer.
VENDOR.Max first changes the organisation, timing and energy price per coulomb of charge motion, then combines these quantities at the established output port into measurable power. The architecture must therefore not be understood as a finite store of battery energy, supplied once and passed sequentially through a chain of efficiencies.
The energy is not inside the electrons
Charge carriers are not brought into the device at startup. They are already there.
Conductors, windings, contacts and the connected load already contain free carriers. Every cubic millimetre of copper contains an enormous amount of mobile charge. Even under macroscopically static conditions, its carriers continue to move randomly: their mean velocity is zero, and no energy is transferred to the load.
Startup does not create carriers. It establishes an organised electromagnetic field. Under the action of its electric component, the mean carrier velocity acquires a small directed component — the drift component: a current appears and energy transfer begins.
Charge is not fuel. Charge is the carrier of the interaction. Energy is transferred by the field, whose electric component does work on the charge carriers.
A battery illustrates the same principle in familiar engineering terms: during discharge electrons move through the external circuit, but the energy is released by the change of chemical state. Charge takes part in the transport; the source is the change in the internal energy of the electrochemical system. The consumer does not destroy electrons — it receives the energy that the field transfers through the organised motion of the charge carriers.
The price of a coulomb
Two systems of description run in parallel and do not substitute for one another.
- Coulomb
- Quantity of charge.
- Ampere
- C/s — rate of charge transport.
- Joule
- Quantity of energy.
- Volt
- J/C — energy price per unit charge.
- Watt
- J/s — rate of energy transfer.
A relation between them exists only at a correctly defined electrical port:
\[p(t) = u(t)\,i(t) = u(t)\,\frac{dQ}{dt}\] \[E = \int u(t)\,i(t)\,dt = \int u(t)\,dQ(t)\]The same amount of charge — one coulomb — can be associated with very different amounts of energy at different transport prices; the difference can be several hundredfold. The question “how much charge has passed?” is therefore not equivalent to the question “how much energy has been transferred?”.
The roles are clearly separated:
- The charge map establishes which carriers move, in which ensemble, through which cross-section and in which direction.
- The field map establishes what does work on them.
- Voltage shows the energy price per coulomb.
- Current shows how many coulombs are transported per second.
- Their synchronous combination at a defined port gives the energy flow.
Charge accounting is not energy accounting and does not replace it. It builds the measurement basis on which energy accounting becomes possible in the first place.
How active power is measured in open systems
Where the charge-domain description becomes power
Charge is not physically converted into energy and is not consumed like fuel. Something else happens: at every stage the quantity of charge, the rate of transport, the direction, the temporal organisation and the energy price are tracked. Once a correct electrical port is established, the two systems of description meet again:
\[P = \frac{dE}{dt} = U\,\frac{dQ}{dt} \qquad \mathrm{J/C} \times \mathrm{C/s} = \mathrm{J/s}\]Physically, this transition is established at the electromagnetic pickup stage: the coupled field does work on the receiving ensemble’s own carriers and produces an electromotive force. In measurement terms, the result can be read consistently as power after rectification, at the established DC port, where directed charge flow and energy price per coulomb are defined simultaneously.
| Question | Answer |
|---|---|
| Where does the physical transfer of energy take place? | At the electromagnetic pickup node, where the field does work on the receiving ensemble’s own carriers |
| Where does the result become readable power? | At the established DC port after rectification: C/s × J/C = W |
| Plane | Charge flow | Energy price | Power |
|---|---|---|---|
| Plane 1 — input of the working node | 10 C/s | 10 J/C | 100 W |
| Plane 2 — after conversion, field transfer and rectification | 2.5 C/s | 100 J/C | 250 W |
The left factor is the ratio of charge flows, the right factor the ratio of energy prices per coulomb. The number of coulombs per second has fallen to a quarter, while the energy price of each coulomb has become ten times higher. Charge has been neither created nor multiplied: what has changed is the organisation of the charge flow and the field work corresponding to the directed transport of a unit of charge. Their combined result at the output port is already expressed in watts.
The two planes of the example are defined working planes of a multi-port architecture, chosen to describe a local conversion. The coefficient \(G\) shows how the charge flow and the energy price per coulomb changed together between these planes. It is not an efficiency: efficiency is defined from the complete balance of a single control volume over all of its ports, whereas \(G\) characterises the conversion between two previously defined working planes.
For that reason the local coefficient must not be confused with an end-to-end efficiency from the startup battery to the consumer. The startup source belongs to the initiation phase; the coefficient connects two defined working planes of the steady-state regime. At the established DC bus, part of the available flow returns to the Frame 1 input and sustains the next cycle, while the remaining part, after internal needs and losses are covered, goes to the customer branch.
We are not trying to carry a single initial coulomb or startup joule through the entire device. We track the conversion of charge states and field transfer between their respective charge-carrier ensembles, then restate the result at the established port as measurable power: C/s × J/C = W.
How the field transfers energy between separated ensembles
The key fact of the architecture: no charge carrier travels the entire path of the device.
Energy is transferred across the electromagnetic coupling region without carriers moving between the galvanically separated ensembles. The changing field excites the motion of the receiving side’s own carrier ensemble; the electrons of the excitation side do not cross to the pickup side.
Three consequences follow, each of which is regularly disregarded when such systems are interpreted.
Equality of the currents on the two sides is not a law. The ports belong to different ensembles. The charge balance closes separately on each side, taking local accumulation and displacement currents into account.
A net charge transport of zero over a period does not imply zero energy transfer. A current integral that vanishes over a period is compatible with non-zero net energy transfer, provided that the synchronous integral \(\int u(t)\,i(t)\,dt\) over the same period is non-zero. Oscillation alone does not guarantee net energy transfer.
The direct work on the carriers is done by the electric field component, not by the conductor. The conductor sets the geometry and the boundary conditions; energy is transferred by the electromagnetic field.
At this transition, the field energy is transferred to the electrical degrees of freedom of the pickup path’s charge-carrier ensemble and becomes available at its port.
What the working core boundary shows
Frame 1 is the boundary of the working core. It is drawn through the real input port of the excitation path.
Frame 1 encloses the excitation node, the coupled resonant node, the electromagnetic pickup path, the rectifier node and the output power stage up to and including the regulated DC output. The main DC bus, the BBMS branch that sustains the operating regime (Battery Boundary Management System), and the return path provide the input boundary condition for Frame 1; at the Frame 0 level, they lie inside the overall product boundary.
At this boundary there is a real measurement plane — the terminals of the excitation path. In the steady-state regime, a positive mean active power is transferred through this plane in the direction of the excitation node. This plane shows what directly supplies the excitation node and how the coupled field regime is sustained.
After the startup sequence has completed and the operating regime has been established, the terminals do not disappear. What changes is the source of their boundary condition: the external startup source hands this function over to the internal regime-feedback branch. The physical input to the excitation node remains; only its classification as external to the product ends.
In the steady-state regime, the internal regime-feedback branch sustains a positive input flow through the Frame 1 port; at the same time, with a load connected and the customer output enabled, the regulated output flow of the working core reaches the consumer and crosses the outer boundary Frame 0.
The flow formed at the main bus is divided: one part covers the excitation and the internal needs of the next operating cycle, the other passes through the output power stage to the consumer.
For Frame 1, the flow through the input plane is an input flow through the port of the working core. It represents that part of the flow formed at the main bus which has been returned to sustain the next operating cycle.
For Frame 0, however, it remains an internal flow of the product and does not constitute an additional energy input: the regime branch and the corresponding flow of the main bus belong to the same internal loop. When the balance of the complete device is consolidated, the two ledger entries of the same internal flow cancel each other out. It is not permissible to count this flow simultaneously as an internal output of the bus, as an input of Frame 1 and as an external input of Frame 0.
Frame 1 shows which field transfers energy, to which ensemble, and at which port the transfer reaches the output path.
Outside the enclosure — but inside the working topology
The familiar linear diagram depicts a power source as a box: energy must enter on one side and leave on the other towards the consumer. It is this visual geometry that creates the expectation of a continuing external energy input.
VENDOR.Max is not a linear transfer chain from an input to a load. It is a system of coupled charge circuits in which every galvanically separated ensemble has its own carriers, while the interaction between ensembles is carried by the field.
Before a load is connected, the internal regime charge route is already closed: the flow of the main bus is divided between internal needs and the regime branch that returns the boundary condition to the Frame 1 input. The customer port exists at that moment, but the customer charge circuit is not yet closed, and there is no directed charge flow through a load.
Connecting a consumer is not simply an increase of draw at the end of a linear chain. The working topology itself changes: the outgoing conductor, the load and the return conductor close another charge circuit.
output path → outgoing conductor → load → return conductor → output path
- Conducting route and charge circulation
- Internal regime feedback
- Field coupling
Internal regime route closed · customer circuit open.
The load closes another circuit of the coupled topology.
Connecting a load closes a new charge circuit and changes the working topology of the whole coupled system. Where, between its defined working planes, are the local increments observed?
Where Is the Plus? A due-diligence answer
The charge carriers of that circuit do not come out of VENDOR.Max and are not consumed by the customer. They are already present in the conductors and in the load itself. Once the circuit is closed, the electric field component does work on those carriers and sets the energy price per coulomb of their directed transport. The magnitude of the resulting charge flow is determined by the state of the whole closed circuit, including the impedance of the load.
The new circuit does not remain an independent appendage beyond the enclosure. The load impedance becomes a boundary condition of the output circuit. Through the sequence of coupled electromagnetic transitions its back-action propagates to the whole system and moves it to a new self-consistent operating point. The demand of the load is served inside this enlarged topology; it is not fed into it from outside.
The load is not added after the system. On connection, it becomes one more circuit of the system.
Frame 0 does not move in the process. The consumer remains physically outside the enclosure, and the power delivered to it remains an output of the product. But the boundary of the enclosure crosses the closed customer circuit in two places — on the outgoing and on the return conductor — and is therefore not the end of the electrodynamic topology.
The charge balance of the customer circuit is closed: as much charge leaves through the outgoing conductor as returns through the return conductor.
\[\left|\frac{dQ_\text{out}}{dt}\right| = \left|\frac{dQ_\text{ret}}{dt}\right|\]At the same time a positive average active power crosses the customer port outwards:
\[P_\text{customer,0} = \langle u_\text{port}(t)\,i_\text{port}(t)\rangle_{\Delta t} > 0\]Across Frame 0 the outgoing and the return conductor carry charge flows equal in magnitude, so the charge circuit is closed. But the potentials of those conductors differ: the energy price of the directed transport is set by the voltage between them, so their energy contributions do not cancel.
The two statements do not contradict each other, because they belong to two different systems of description: the first to the charge accounting of the circuit, the second to the energy accounting of the port. The charge returns; the energy is delivered to the load. A closed charge circuit does not turn the output into an energy input and does not require a symmetrical input arrow on the opposite side of the enclosure.
A connected consumer does not create a continuing external power input through Frame 0. It creates a new closed charge circuit whose demand becomes an internal condition of the coupled working topology. If a different external energy channel is assumed, it must be physically named, located and measured at Frame 0 — it cannot be inferred from the mere existence of a load.
The outer boundary of the product is not the outer boundary of the working circuit.
Why the outer boundary answers a different question
Frame 0 establishes the overall exchange of the whole device with its environment — and nothing else.
That is a different question, and it is not a deeper version of the first. This can also be checked on familiar systems.
- Asked how the energy reaches the output carriers of a solar panel, the physicist answers with the transfer of energy from the absorbed photons and the separation of the carriers by the internal field. Asked what pays for that transfer, the answer is the solar flux through the surface of the module. Two different answers, both correct.
- Asked how the energy reaches the secondary side of a transformer, the engineer answers with the work of the induced field on the secondary ensemble. Asked what pays for that transfer, the answer is the flow through the primary port.
The first question belongs to the boundary of the working core. The second belongs to the boundary of the product.
Frame 1 reveals the direct mechanism of energy transfer to the output ensemble, the local conversion of the charge flow and the internal route by which the regime is sustained. Frame 0 consolidates the overall exchange of the product with its environment. Together these boundaries give two consistent descriptions of the same architecture: the operational one and the system-level one.
Conflating these two boundaries is one of the main sources of apparent paradoxes around architectures of this kind. The quantities of the working core belong to that boundary alone; the quantities of the outer boundary belong to it alone.
| Frame 1 | Frame 0 |
|---|---|
| Sustaining of the working core | Consolidated exchange of the product |
| Real input flow through the port | The same regime branch — an internal transfer |
| Local conversion between working planes | Customer output across the enclosure |
What is not a source
Each item below is excluded for its own reason, not by declaration.
Not the charge. It is the carrier of the interaction, not a store of energy; it is not consumed like fuel.
Not the voltage. It shows the energy price per coulomb, not the presence of a store: a storage element of small capacity can hold little energy even at thousands of volts.
Not the field itself. The field transfers the energy and does work on the charge carriers — that is the transfer mechanism. What sustains the field regime itself, the field does not tell: that is a question for a different boundary.
Not resonance in itself. Resonance sets the scale of the internal circulation and of the amplitudes. A large charge circulation characterises the intensity of the internal motion, not the active power.
Not the frequency. It sets the tempo at which events repeat and links the single event to the average process — but it does not determine what pays for each event.
Not the feedback. The loop is a route, not a store. It redistributes the formed flow and sustains the Frame 1 input; at the level of the complete product it is an internal transfer, and it is eliminated from the balance only on consolidation at Frame 0.
Not the buffer. A storage element in the regime branch buffers transient exchange but is not an energy source: over a sufficiently long steady-state window, its source-neutral condition \(\Delta E_{\text{battery}} \approx 0\) is subject to direct measurement.
Not the discharge event in itself. It compresses the release time of a previously established charge separation. An increase in the instantaneous power of the pulse is not an increase in the energy of the event.
Not the atmosphere. The surrounding air is not treated by the project as a working energy channel.
What VENDOR.Max actually does
Three functions — and none of them amounts to creating energy or charge.
It organises the field regime
Pulsed excitation forms a coupled resonant regime with high-amplitude field states and a stable event repetition rate.
It sets the energy price per coulomb for the output ensemble
The electromagnetic coupling induces an electromotive force in the pickup path and thereby determines how many joules correspond to each coulomb transported there.
It turns the alternating exchange into a directed flow
Rectification gathers the individual charge packets into a stable reservoir of separated charge; the power stage brings the flow into the form required by the user.
The architecture as a whole is described by classical electrodynamics and standard power electronics. The protected structural solution concerns the excitation node and is set out in independent claim 1 of patent ES2950176B2 (Granted).
The transfer route and functional coupling of the nodes Patent family and jurisdictions
The boundary of public disclosure
What this page establishes publicly, and what remains protected engineering know-how.
This page establishes the public physical model of VENDOR.Max: initiation of the operating regime; sustaining of the Frame 1 input by the regime branch; the discharge-resonant organisation of charge motion; field transfer between galvanically separated ensembles; formation of the energy price per coulomb at the output; conversion of the charge-domain result into power at the DC port; division of the formed flow between sustaining the regime and supplying the consumer; the closing of the customer charge circuit when a load is connected, and its impedance as an internal boundary condition of the coupled topology.
The hypothetical numerical example illustrates the arithmetic of this conversion and is not an operating characteristic of VENDOR.Max. The real values of the internal coefficients, phase relations, control parameters and inter-circuit flows are protected engineering know-how. The quantitative data required for independent verification are made available to authorised laboratories, certification bodies and industrial partners under controlled conditions.
Frequently asked questions
Short answers to the questions this page is most often opened with.
Does the startup battery supply the consumer after startup?
No. It only initiates the regime; after startup the Frame 1 input is sustained by the internal regime-feedback branch.
At which stage does the charge-domain description become power?
The physical energy transfer takes place at the electromagnetic pickup stage; at the DC port the power is calculated as C/s × J/C.
Do coulombs turn into energy?
No. Coulombs describe the quantity of charge transported; voltage gives the joules per coulomb, and multiplying that figure by C/s yields watts.
Why can no end-to-end efficiency be calculated from the startup battery?
Because startup and the steady-state regime belong to different phases, and the local coefficient \(G\) connects two working planes and is not the efficiency of the complete device.
What does the local coefficient G show?
The combined change of the charge flow and the energy price per coulomb between two defined working planes.
How can the resulting power both sustain the operating regime and supply the customer?
At the main DC bus, the established power flow is divided: one part returns to the Frame 1 input, while the other is routed through the power stage to the customer output.
Does connecting a consumer create an external energy input?
No. With customer output enabled, connecting a load closes another charge circuit that galvanically continues the output ensemble. Its impedance becomes a boundary condition of the whole coupled topology, while the average active energy flow through the customer port is directed from VENDOR.Max to the load.
Where to go next
The reading route continues with the transfer architecture, the accounting rules and the validation framework.
