The energy a unity power factor doubles
Assumes: The current that does no work · The capacitor that was right once · The inductor that is an amplifier
The current that does no work computed one load’s reactive power three separate ways and said that a quantity computed three ways by routes sharing no arithmetic is very unlikely to be wrong. That is true. It is also not what those three routes establish, and the difference matters, because two of them agree for a reason that has nothing to do with the circuit being right.
The first sums over the sources. The second sums the same product over the elements. The third is — twice the frequency times the difference of the energies stored in the inductances and the capacitances — and it names no impedance and no source at all.
The first two cannot disagree. Not for this circuit: for any circuit whatever, correctly assembled or not, made of any elements at all. That leaves one independent route, and the interesting thing about it is that it computes a difference of two quantities that the other two never see separately.
Two things follow, and they point in opposite directions. The demonstration is weaker than it looked, because a three-way agreement in which two of the routes are one theorem is a two-way agreement wearing a third hat. And the third route is stronger than it looked, because a route that measures something the others cannot see is not a check at all — it is an instrument, and it has been pointed at nothing.
What follows points it at three things: a load being corrected, a circuit at resonance, and an inductance made of an amplifier. The first two say what the discarded sum is. The third is where the route stops agreeing with the other two, and is not wrong to.
The reproduction, which comes before the departure
An instrument that has never been made to agree with something already known is an instrument whose disagreements mean nothing. So the case to start from is the one where all three routes must give the same answer, and where that answer is known independently: a resistor and an inductor in series across a stiff supply, which is the load this whole field is quoted at.
Here the three agree to a part in 10⁹, which is the tolerance the figure asserts rather than the tolerance the arithmetic achieves. That agreement is the calibration, and it is worth being precise about what each half of it is evidence for. The first two agreeing says the netlist was assembled correctly. The third agreeing with them says that the inductor in the netlist behaves like an inductor — that the energy in it really is , and that this really is what the terminals report as reactive. Nothing else in the collection makes that second statement, and every number below leans on it.
Two routes that are one theorem
Tellegen’s theorem says that for any network satisfying the two circuit laws, the complex powers absorbed by the elements sum to zero. It uses the topology and nothing else: not what the elements are, not whether the stamps are right, not whether the answer means anything. Given a set of branch voltages consistent with a loop law and a set of branch currents consistent with a node law — of the same graph, not even of the same circuit — the sum is zero.
So the first route and the second route are one statement partitioned two ways. Summing over the sources and summing over the elements are the two halves of a sum that is identically zero, and their agreement is a restatement of the two circuit laws that what a network answers already imposes on every solve. It is worth having: it catches an assembly error, a sign reversed in a stamp, a current unknown attached to the wrong branch. It is a check on the arithmetic. It is not evidence about the physics, because it holds just as exactly for a circuit whose every element value is nonsense.
The distinction is easiest to see in what would have to go wrong for each to fail. To break the first two, the solved voltages and currents would have to violate a circuit law — which is what the solver imposes, so the failure would be in the linear algebra rather than in the model. To break the third, an element would have to store an amount of energy inconsistent with the voltage across it or the current through it, which is a statement about the element and not about the matrix. The two failures live in different places, and only one of them is about the subject.
The third route is a different kind of statement. It uses the constitutive laws of the reactances: for an inductor and for a capacitor, with the root-mean-square phasors this field uses throughout. Those are claims about what an inductor is. A network of resistors that has been mis-stamped as inductors passes Tellegen and fails this.
That is the whole reason the third route is worth running, and the reason the site’s habit of demanding two routes is not proof against a shared assumption — the same trap the assumption that is a geometry found in a winding, where three independent computations of an alternating-current resistance turned out to be one sentence written three times.
The difference, and the sum
is a difference. Nothing in either power route reads , and nothing in the collection had until now.
A correction capacitor drives the difference to zero. It cannot touch the sum, and the arithmetic of why is short enough to state. The capacitor sits across the supply, so the load branch still sees 230 V and its current is unchanged: is fixed at 2,044.9 mJ for the whole sweep. The capacitor’s own store is , which is 26.45 mJ for every microfarad added, exactly linear, and it only ever grows. At the point where the difference is zero and the power factor is one — and the sum is therefore exactly twice what it was, not approximately.
That identity does not depend on the load. It falls out of the definition of the correction: the capacitance chosen is , so its stored energy is , and was . Twenty millihenries gives 1,204 mJ becoming 2,407; a hundred and twenty gives 1,743 becoming 3,486. The generator asserts the ratio at 2.000000000 on every frame of the slider rather than checking it once.
The capacitance that does it is not monotonic in the load, which is worth a line because it is the kind of thing a formula hides. Twenty millihenries wants 45.51 µF, fifty wants 77.31, eighty wants 77.55, and a hundred and twenty wants 65.89 — the requirement peaks near the inductance whose reactance equals the resistance and falls away on both sides, because past that point the load’s own reactance throttles the current that produces the reactive power in the first place. A designer sizing a bank from a nameplate sees a single number and not a maximum.
The cable current is the one quantity of the three with a genuine optimum. It falls from 9.044 A to 7.113 A at the correction point and rises again afterwards, reaching 17.593 A at 300 µF — nearly twice the uncorrected figure, in copper sized for the uncorrected figure. That is what the correction buys, and it is bought against the sum rather than for nothing: less current in the cable, more energy in the installation.
So the corrected installation is a resonant circuit at the supply frequency, which is exactly what the reactance cancelled, and the resonance it buys is about in the series position and what the capacitor that was right once prices in the shunt one. Cancelling a reactance and building a resonator are the same act described twice, and only one of the two descriptions makes it obvious that something is now storing twice as much energy and exchanging it internally rather than with the supply.
The supply, taking it back
Past the correction point the difference changes sign rather than getting smaller, and the element-by-element reading keeps the sign rather than taking a magnitude, so the condition is visible in the solve instead of having to be inferred from it.
A meter that reads a magnitude reports 0.8044 with the 150 µF fitted and 0.7864 with none, and cannot say that the first of those is leading and the second lagging. That is the fault an installation carries for years, and it is now three separate readings rather than one: the power factor is no worse, the cable current is worse, and the stored energy is worse still — 2.94 times the uncorrected figure at 150 µF, rising to 4.88 at 300.
The third of those has a consequence the first two do not. A supply absorbing reactive power is a supply whose own impedance sits across a capacitance large enough to have resonated with something, and the energy available to that resonance is the sum rather than the difference. The difference reads 1,208 var and the sum reads 6,012.4 mJ, and it is the second that decides how much there is to ring with when a contactor opens. Nothing in a power-factor calculation contains that number.
What the discarded sum turns out to be
The sum is not an abstraction. Divide it by the power dissipated and multiply by the frequency and it is the quality factor.
That is the standard energy definition of arriving from the power field rather than from the frequency one, and it is worth noticing which of the three routes it came out of. A power meter on that circuit at resonance reads 2,645 W, 0 var, power factor 1.000000, and has no access whatever to the 6,612.5 mJ the inductor and the capacitor are passing back and forth between them. Whether that matters is the subject of resonance, and the bandwidth it sets exactly and of the Q the components allow; the point here is only that the number is in the solve and that two of the three routes to reactive power throw it away by construction.
The minimum is at resonance and not at either end, and the reason is a race between the two stores: below resonance the capacitor holds most of it and above it the inductor does, and the crossover is where the total per watt is least. At 20 Ω the floor is 0.785398, at 5 Ω 3.141593 and at 2 Ω 7.853982 — π/4, π and 5π/2, since ω₀L is 5π for the parts drawn. The generator finds it by golden section and then checks the located frequency against the one the components predict, rather than evaluating at 50 Hz and asserting that the answer is a minimum.
Where the third route stops agreeing
A gyrator is an inductance made of resistors, a capacitor and two amplifiers. The inductor that is an amplifier measures it as an inductance and says in passing that nothing in it stores energy in a magnetic field. That sentence has a number, and the third route is what reads it.
Drive that node and read the reactive power at it, then read the reactive power the stored energy accounts for. With ideal amplifiers the two are the same size and opposite in sign, to nine figures, at every frequency in the band.
The magnitudes matching is the surprising half. It is not obvious that a capacitance held at the right voltage by an amplifier should store exactly what an inductor of the designed value carrying the terminal current would need — the arrangement was derived to produce an impedance, and an impedance is a ratio of two phasors that says nothing about energy. It comes out at 1.000000000 anyway, which says the equivalence is stronger than the derivation claimed: the synthetic inductor is not merely an impedance imitation but an energy-accurate one, in the wrong element and with the wrong sign.
Both facts are exact rather than approximate, and neither is available to a power meter. An instrument at the terminals reports an inductance absorbing reactive power. The energy route reports a capacitance of exactly the right size delivering it. Both are right; they are answering different questions, and in a passive one-port the two questions have the same answer because there is nothing in the circuit that can move energy between the two kinds of store without holding it.
An amplifier can. That is what the two controlled sources in the arrangement do, and it is why the third route is the only one of the three that carries information: Tellegen locks the first two together whatever is in the network, while the energy route asks each element what it is and gets a different answer here. The same asymmetry underlies the reading that does not care which way round — reciprocity is a property of the elements, and the elements that break it are exactly these.
The mechanism is worth stating as a theorem rather than as an observation, because it says exactly which circuits are exempt. For a resistor, an inductor or a capacitor, the reactive power absorbed is times that element’s own store with a fixed sign — zero, plus, minus. Sum those over a passive one-port and Tellegen turns the terminal reactive power into with no further assumption: the two routes coincide because every element in the sum obeys the same relation between what it absorbs and what it holds. A controlled source obeys no such relation. What it absorbs is set by a gain and a voltage somewhere else, and it holds nothing, so it enters Tellegen’s sum and not the energy sum. Every circuit on this site containing a nullor, a gyrator or a controlled source is therefore a circuit where the two quantities are free to differ — and where the difference between them is a measurement rather than an error.
What is inside the amplifiers
Ideal amplifiers are a limit. Real ones have a dominant pole, and a dominant pole is a capacitor.
The compensation that makes an amplifier stable is the largest energy store in the circuit by three or four orders of magnitude, and it is a store nobody put on the schematic. The ideal amplifier, and where it stops being one prices that pole in gain and phase; this is the same pole priced in joules, and the price is much larger than the thing the circuit was built to make. A slower amplifier costs more of it, in exact proportion, which is the opposite of the direction the bandwidth argument pushes and is one more reason one inductor, and ten components is a trade rather than a substitution.
None of this makes the gyrator a bad inductor. It makes the phrase stores energy in a magnetic field a measurement rather than a description, and gives it a number.
What it does not say
It does not say the first two routes are worthless. They catch the errors they were written to catch, they cost nothing, and a solve that fails them is broken beyond interpretation. What they cannot do is corroborate the third, and quoting three agreeing routes as three independent confirmations overstates the evidence by exactly one.
It does not say reactive power is the wrong quantity. It is the right one for the thing it decides — the current in the cable, the rating of the transformer, the bill — and none of those cares how much energy is stored anywhere. The sum matters for different questions: how long a circuit takes to settle, how sharply it selects, how much a capacitor bank rings when something upstream switches, which is the pair that is worse than either arriving at its own frequency.
And the sign reversal at the gyrator is not a failure of the energy route. It is the honest report of a circuit where the terminal behaviour and the stored energy have genuinely come apart, and it can only happen where a controlled source is present. Nor is the ideal-amplifier case a convenience: a nullor is the element that constrains its input to zero volts and zero amps and lets its output take whatever the rest of the network needs, so a netlist built with nullors is the arrangement with the amplifiers’ own limits removed and nothing else changed. It is the calibration for the second half of the argument in the same way the passive load was for the first, and the exact 1.000000000 it returns is what entitles the 3,272 to be quoted as a property of the parts. In a network of resistors, inductors and capacitors the three routes agree, always, and their agreement is then a check on all three.
Every number above assumes one sinusoid at one frequency. A current that is not a sinusoid has no single phasor, and are not single numbers either, and the whole apparatus stops applying — a limit every model has an edge states in general and which this field’s own rectifier essays measure.
The number worth carrying
Two thousand and forty-four millijoules becoming four thousand and eighty-nine, exactly, at the point where the reactive power reads zero.
The habit with it is shorter, and it is two habits rather than one.
When a quantity is defined as a difference, find out what the sum does before treating the difference as a description of the circuit. A null in a difference is a statement about a balance and says nothing whatever about the size of the things being balanced, which is why unity power factor and twice the stored energy are the same operating point.
And when several routes to one number agree, count how many of them could have disagreed. Two routes locked together by a theorem about topology are one route with two names, however different their arithmetic looks — the same reading a winding’s three alternating-resistance calculations turned out to deserve. Here the count was one, and the one that could disagree was also the only one that ever did.
Part 2 on reactive power
One argument about Reactive power, and one of 2 essays on it so far, each part numbered by how much of the idea it assumes. What sits either side of it:
What links here
Essays that reach for this one mid-argument — the half of a link its own author cannot write down.
The objects named here
The third axis, after the field and the idea: the things themselves, and every essay that touches each one.
Complex powerEnergy-storageGyratorNullorPower factor correctionQuality factorReactive powerSeries resonanceSynthetic inductorVerification
- The boundary that improves when the part gets worse gyrator, nullor, quality factor, synthetic inductor
- The reading that does care which way round energy-storage, gyrator, nullor
- Eight amplifiers, and what they add gyrator, synthetic inductor
- The arrow that goes past where it settles quality factor, verification
- The floor and the ceiling move apart quality factor, verification
- The half a switch keeps energy-storage, verification