Diagnose before you buy · the source-by-source verdict on chokes

Where received noise
actually gets in

Every dB of received noise enters through one of four doors. They have different causes, different signatures and different cures, and a common-mode choke only reaches one of them. This page is about finding out which door your noise uses before you spend money, because on a quiet station the honest answer is that you should buy nothing at all. Every claim carries a C for a checkable source or an 算式 for arithmetic you can redo on paper.

Four doors, and the cuts that separate them

Received noise enters an EFHW station through four paths. The ARRL’s own guidance for interference hunting is to ask “where is this coming from” before asking “what is producing it”, and the same discipline pays here: you cannot pick the right cure until you know the path.

Door Path Coupling How it shows up
① Element The antenna wire picks the noise up directly. Near-field electric, and far field Cut 2 barely changes it
② Shield Common-mode current on the outside of the coax braid, running through the noise field all the way from the feedpoint to the shack. Conducted along the braid, plus field coupling Cut 2 collapses it; a clip-on bead changes it
③ Mains Noise conducted in on the supply wiring, through the PSU, into the receiver’s ground reference. Conducted Cut 4 changes it
④ Near field The rig, the SDR, a USB lead or an Ethernet run is itself the receiving antenna. Near-field Cut 5 makes the noise follow the device
Read the last column as a pointer, not a proof. Each cut narrows the candidates; none of them identifies a culprit on its own. You are eliminating doors, one at a time, until one is left standing.

Five cuts, in the order they pay

All five fit in one afternoon and need nothing you do not already own. Cut 1 carries the most information per minute, so start there and stop as soon as a door is eliminated.

Cut What you do What the reading means
1 Screw a 50 Ω dummy load onto the antenna port and listen on the same frequency. Noise disappears → it arrives via the antenna system (door ① or ②). Noise stays → it comes in on the mains or from the near field (door ③ or ④). This one cut halves the search space.
2 Disconnect the antenna wire at the transformer but leave the coax connected and running to the shack. Noise stays → the braid is receiving it, and a choke has a target (door ②). Noise collapses → the antenna wire itself is doing the listening, and no choke will help (door ①).
3 Clip a ferrite bead onto the coax and A/B it in and out, several times. Level steps with the bead → you have confirmed a common-mode path, and a permanent choke is worth building. Level moves but not back, or moves only at some frequencies → you are shifting a resonance, not removing a current (see the divider section).
4 Run the radio from a battery and unplug every charger, every wall-wart and every Ethernet run in the room. Noise changes → door ③, and the cure belongs on the mains lead, not on the coax.
5 Walk the house with a portable shortwave receiver, holding it close to suspect devices. Noise rises sharply near one device → door ④, and you have found the culprit. Noise that is uniform everywhere points back at doors ①, ② or ③.
Two rules, or nothing below this line is trustworthy.
1. Relative readings only. An S-meter reading is not a noise power measurement. It moves with AGC, with preamp and attenuator settings, and — the part people miss — with the source impedance the receiver is looking at. Swapping in a dummy load changes that impedance, so part of the level shift in cut 1 is not a noise change at all. Compare, never measure absolutely.
2. Same hour, same frequency, same settings. The ambient noise field moves over minutes and hours as appliances and neighbours come and go. An A/B split across two evenings proves nothing.

A worked counter-example from this station

The advice to add a receiving loop is repeated everywhere as if every EFHW station needs one. On this station the opposite is true, and it is worth showing how a measurement settles the question rather than a reputation. Values below are from a full year of PSK Reporter records analysed for BG1SB (grid ON80da), and they describe this site only.

Basis: efhw-knowledge/measurements/bg1sb_20m_efhw_case_study.md §2.5 and §2.6 (2026-06-14). Relative values from PSK Reporter, not absolute noise power.
Quantity Measured value Reading
Weakest signal decoded, quietest direction −23 dB SNR The FT8 decoder’s limit is about −24 dB, so the station is within a dB of theoretical sensitivity
Noise floor by direction Uniform, no directional source No direction is being swallowed by a local noise source
DX share, receive vs transmit 29.9% RX against 20.6% TX Receive reaches further than transmit, so receive is not the bottleneck
So the conclusion is “buy nothing”, and it is a measured conclusion. The mechanism behind the popular advice is sound — a station buried in local noise really is deaf on receive, and a loop with a sharp null really can help. But the premise does not hold here, so the conclusion does not either. Measure your own noise floor before you accept somebody else’s cure.

The same phrase covers six different things

“Environmental interference” gets used as one problem. It is six. Read the cards as a comparison rather than as six essays: every card uses the same five headings, so the verdict on chokes can be read straight down the column and the differences are the point.

1 · Power lines C

Mechanism. Almost all power-line noise comes from a spark or an arc across utility hardware: a gap between two conductors, caused by fittings that are loose, broken or spaced too closely. Current crosses the gap, ionises the air, and radiates broadband energy.

Signature. On a 50 Hz grid the arcing fires 100 times a second, because every cycle has two voltage peaks and two zero crossings. On a 60 Hz grid it is 120 Hz. On an oscilloscope the noise appears as two horizontal bands drifting slowly upward, one from each half of the cycle. Two free tests confirm it: rain quietens it, because water bridges the gap, and wind makes it vary, because loose hardware moves.

A correction worth having. Corona discharge is rarely, if ever, the cause. The ARRL states it plainly: corona is confined to lower frequencies, it is a low-current phenomenon, and it does not propagate far from the source. Blaming corona sends you looking for the wrong thing on the wrong pole.

CMC verdict: no. The energy travels along the power wiring and reaches you by radiation into the antenna wire — door ①. A choke acts on the coax braid’s common-mode path, and this noise is not on it.

Remedy. Complain, with evidence. This is the one category where the fix belongs to somebody else, and in many jurisdictions that somebody is legally obliged to act.

2 · Switching supplies C 算式

Mechanism. A switching converter chops DC at tens to hundreds of kilohertz. The harmonics of that chop, and the ringing on every edge, run straight up through the HF spectrum. The noise leaves the box in two forms: differential mode between live and neutral, which an X capacitor suppresses, and common mode between the conductors and earth, which needs a Y capacitor and a common-mode choke. Cheap supplies cut cost by omitting precisely those last two parts — the only two that work at HF.

Signature. A comb of harmonics spaced at the switching frequency, drifting as the supply’s load changes. Often accompanied by a slow periodic wobble as the supply enters and leaves burst mode on light load.

What compliance actually buys you. Household equipment must meet the Class B conducted-emission limits. Here they are, with the voltage limit converted to the power it represents across 50 Ω:

Class B conducted disturbance at the mains port, quasi-peak. Basis: GB/T 9254.1-2021, which adopts CISPR 32. Power column is arithmetic: P = 10·log₁₀(V² / 50 Ω / 1 mW). The two rows marked for reference are typical noise-floor orders of magnitude, not limits, and are labelled as such on purpose.
Frequency Limit Voltage Into 50 Ω
0.15–0.5 MHz 66 → 56 dBμV 2.00 → 0.63 mV −41.0 → −51.0 dBm
0.5–5 MHz 56 dBμV 0.63 mV −51.0 dBm
5–30 MHz 60 dBμV 1.00 mV −47.0 dBm
for reference quiet rural HF noise floor typical order of magnitude ≈ −120 dBm
for reference suburban HF noise floor typical order of magnitude ≈ −100 dBm

Read the gap, not the rows. A device that passes the standard with no margin is putting a signal at the mains port comparable to the first three rows. A quiet band sits at the last two. That gap is the whole problem, and it is why compliance is not the same thing as not interfering — the limit is a compromise between commerce and spectrum, not a promise that your HF reception will be usable. The bottom two rows are typical orders of magnitude rather than a standard, which is exactly why they are labelled that way.

CMC verdict: no, for the coax. Noise entering on the mains never touches the coax, so a choke there is decoration.

Remedy. The same device, on the right conductor: a common-mode choke on the mains lead or the DC lead. Also check USB and Ethernet runs, which are the most commonly missed members of this family.

3 · Electric vehicle chargers C

Mechanism. AC charging runs the mains through an on-board charger in the car — a switching converter of 3.3 to 11 kW. DC fast charging does the conversion in the post itself, at even higher power, increasingly with silicon-carbide devices and their steeper switching edges. Either way the charging cable is several metres of multi-conductor cable running from a building to a vehicle, and its protective earth conductor is exactly as long as the common-mode antenna it forms. A kilowatt-class switching converter driving a long unshielded conductor, with no RF reference ground at either end, is the mechanism written out in full.

Signature. Broadband, strongest while a car is actually charging, and gone when it unplugs. That on/off correlation is the most useful thing about it, because it dates and fingerprints the event even when you cannot see the charger.

No public HF measurement exists for this. Every reachable published case about EV chargers concerns conducted-emission test failures, or the 125 kHz band where charging posts interfere with keyless-entry systems. Nothing we could retrieve measures a charger at 1.8–30 MHz. What you have just read is mechanism only. We will not print a number we cannot show, and neither should anyone else selling you a solution.

CMC verdict: partly. The dominant path is door ① — the charging cable radiates into your antenna wire. A coax choke reaches only the fraction that arrives on the shield.

Remedy. Negotiation and geometry, in that order. Establish the on/off correlation first; that is the evidence that makes a conversation with the owner or the property manager possible. Then move your own antenna further away, or accept the hours.

4 · Solar inverters C

Mechanism. Modern string inverters are usually transformerless, so the panels and the grid share a common-mode path with no isolation between them. Add the long DC run down from the roof, which forms a large common-mode loop, and switching devices with steep edges, and you have a strong common-mode source bolted to the same building as your antenna.

Signature. Correlated with daylight and with inverter output. Often strongest at midday, absent at night, and it changes when a cloud crosses.

CMC verdict: partly. Mixed paths. The fraction radiated into the antenna is out of reach; the fraction conducted into the building wiring is reachable, but with a choke on the mains, not on the coax.

Remedy. Almost entirely source-side, which means not yours: LCL filters, common-mode reactors, active filtering, and gate-drive optimisation all live in the inverter. What you own is the same on/off evidence, and the same conversation.

5 · Power-line communication (PLC / BPL) C

Mechanism. Broadband over Power Line is defined as carrying data over power wiring in the 2–30 MHz band. That is not adjacent to the amateur HF bands. It is the amateur HF bands, plus everything between them.

Signature. This is the one entry in this list that is not a by-product. It is a modulated, deliberate signal inside your band, and it sounds like one.

CMC verdict: no, and a choke will never help. The signal arrives in band, on the antenna, as the wanted signal would. There is no common-mode path to interrupt.

Remedy. Frequency coordination and complaint. This is a regulatory problem, and treating it as an antenna problem wastes money.

6 · LED lighting and grow lights C

Mechanism. Every LED lamp has a driver, and the driver is a small switching supply built to the tightest possible budget. The same cost pressure described in card 2 applies, at a smaller scale and with less room for filtering. High-power ballasts for grow lights are the industrial version of the same story, and the ARRL names them as a category it fields a steady stream of questions about.

Signature. Tied to a switch. The noise appears when a lamp is on and vanishes when it is off, which makes cut 5 the decisive test and makes this the easiest source on the list to identify.

CMC verdict: partly. Whether a choke helps depends entirely on which door the noise used to get in, which is why the diagnostic comes first.

Remedy. Replace the lamp with a better-behaved one. Cheaper and more reliable than filtering the consequences.

The verdict, in one table

Eight rows, and only the last one is where a coax choke does its full job. This is the whole page in one object.

Source Dominant door Does a coax choke help? Where the fix lives
Power-line arcing ① via re-radiation No Complaint, and antenna geometry
Your own switching supply ③ No A choke on the mains or DC lead
Your own PC, USB and Ethernet ④ No Ferrites on those cables
A neighbour’s LED or supply ① mostly Partly Source side, plus geometry
EV charger ① mostly Partly Negotiation, plus geometry
Solar inverter ① and ③ Partly Source side, plus the mains
PLC / BPL ① in band No Frequency coordination, complaint
Near-field noise the braid picks up ② Yes, fully The coaxial choke — this page
One rule generates the whole table. A choke acts only on the common-mode path in the conductor you put it on. Three consequences follow, and they explain every “no” above:
1. It does nothing about noise the antenna wire picks up directly, because that noise is not on the coax.
2. It does nothing about noise conducted in on the mains, because that noise never reaches the coax either.
3. It does nothing once mode conversion has already happened, because by then the noise has left the path the choke can reach.

A choke is a mode selector, not a filter

This is the section that most choke articles skip, and it is the one that decides whether the device can work at all. Get the mechanism right and the placements, the failures and the recipes all follow from it.

The sentence that explains everything

A receiver responds to one thing only: the differential voltage between the inner conductor and the inside surface of the braid. Common-mode current flowing on the outside of the braid cannot reach the receiver by itself. It first has to be converted into a differential voltage, and that conversion happens at an asymmetry — the imperfect balance of the 49:1 transformer, the feedpoint, the rig’s chassis ground. The braid is a receiving antenna that is wired straight into a mode converter you cannot remove.

An ideal choke presents almost zero impedance to differential mode and a high impedance to common mode. Your wanted signal travels in differential mode and passes through untouched. The noise riding on the braid is blocked. That is the whole mechanism. It also explains what a choke does not do: it does not improve your match, raise efficiency or change SWR, because none of those have anything to do with the common-mode path. A choke that changed your SWR was changing something else, and you should find out what.

How much it actually removes

Inserting a series impedance into the common-mode loop divides the current down. To first order:

A ≈ 20 · log₁₀( 1 + Z_cm / Z_loop )

Z_loop is not 50 Ω. It is the impedance of the noise source’s own common-mode loop — the house wiring, the neighbour’s appliance, the building’s ground path. It varies wildly with frequency and you usually do not know it. The table below is therefore a divider calculation, not a measurement; every cell is that formula evaluated, and you can redo any of them.
Basis: the divider formula above, evaluated at Z_loop = 50 Ω and 200 Ω. Arithmetic only — no measurement is implied.
Z_cm of the choke Noise reduction, Z_loop = 50 Ω Noise reduction, Z_loop = 200 Ω
50 Ω6.0 dB1.9 dB
100 Ω9.5 dB3.5 dB
250 Ω15.6 dB7.0 dB
500 Ω20.8 dB10.9 dB
1000 Ω26.4 dB15.6 dB
2000 Ω32.3 dB20.8 dB
5000 Ω40.1 dB28.3 dB
Read the left column as a shopping warning. A clip-on bead has a Z_cm in the tens of ohms across most of HF. Look at the top row: that buys you a handful of dB at best. To do anything serious the choke needs a Z_cm in the kilohm range, and that means a proper core with a proper number of turns.

Three limits of that model

The divider is a first-order picture and it is wrong in three directions that matter in the field.

1. Z_cm is complex. It is R + jX, and the resistive part is the useful part. A choke that is purely reactive absorbs nothing; it stores energy and returns it somewhere else, which is how you get resonances rather than attenuation.

2. Inserting Z_cm changes the current distribution. The model pretends the loop is fixed and you are just adding a resistor. In reality the coax is electrically long, current maxima move, and a single choke often relocates a resonance instead of removing a current. The classic symptom is “it is better on 7 MHz and now worse on 5 MHz”. If you see that, you moved the problem, you did not solve it.

3. Which is why there are two chokes, not two options. One at the feedpoint, one where the coax enters the shack. Between them the line is broken into sections, and if each section is shorter than a quarter wave none of them can resonate. The two are not alternatives; they do different jobs.

Z_cm is a function of frequency, and it is not flat

Turns give you impedance as Z_cm ∝ N², but the material’s permeability is itself a function of frequency. Measured values from the Fair-Rite material data, for the two mixes you will actually use:

Frequency Mix 43 μ′ Mix 43 μ″ Mix 51 μ′ Mix 51 μ″
7 MHz——364156
10 MHz293340——
14 MHz——235186
28.6 MHz——129163
30 MHz117202——
One choke covering 1.8–30 MHz is a fiction. Note where Mix 43 goes: from about 7 MHz upward, μ″ — the loss term — approaches and then exceeds μ′. For a transformer that is bad news. For a choke it is good news, because a lossy choke absorbs the energy instead of storing and returning it, which is exactly the behaviour you want at point 1 above. Different job, different verdict on the same material.

The asymmetry that receive work hands you

Received levels are microvolts. A ferrite on a receive path never saturates, so the entire power-handling and heating discipline that governs transmitter-side chokes simply does not apply.

That cuts both ways. If a choke serves only receive — a separate receiving antenna, a T/R-split front end — you can pile on turns and use a high-permeability mix, and reach a Z_cm far above anything a transmit path could survive. If the choke sits in the main path it must carry transmit current too, and it is bound by saturation and heat.

The best choke for receive may be one that would burn on transmit. Keep that in mind before copying somebody’s recipe: ask which side of the T/R switch their numbers came from.

Counterpoise is a premise, not an option

First the counterpoise, then the choke. An end-fed antenna needs a return path. With no return path, adding a choke just turns the choke into part of the antenna’s load, and the common-mode current finds a third route out — through the chassis, down the mains, into everything you were trying to protect. A choke does not replace a counterpoise; a counterpoise is what lets a choke do its job.
The feedpoint trap. If the coax itself is the counterpoise, then choking at the feedpoint cuts the antenna’s own return path: SWR shifts and efficiency drops. In that arrangement the choke has to sit away from the feedpoint — the ARRL Handbook figure is at least 10 feet, about 3 m. If instead you have a separate counterpoise wire, the feedpoint is the best place to choke, because the current you are intercepting is exactly the current the antenna wanted to drive onto the braid.

Working recipes, all of them quoted rather than invented:

Covers Mix Form
80–20 mMix 31FT240-31, 5–9 turns of RG-8X
40–10 mMix 43FT240-43, 6–10 turns of RG-8X
PortableSnap-on Mix 313–5 spaced along the coax — convenient, and markedly worse
And one design that keeps coming back, which does not work. The air-wound choke — six to eight turns of coax on a 4 to 6 inch PVC pipe — works above about 40 m and does very little below it. With no core, its Z_cm is neither high enough nor lossy enough where the low bands need it. It is a fine mechanical former and a poor choke.

When the choke is the wrong tool

Three of the four doors are out of a coax choke’s reach. Each has its own signature and its own cure, and none of the cures is a ferrite on the feedline.

Door ③: mains and ground loops

The noise source sits on the same supply as your rig. Its rubbish travels down the wiring, through the power supply, into the chassis — and the chassis is the reference against which the receiver measures everything. Nothing about this route involves the coax, which is why cut 1 does not clear it.

Signatures. Cut 1 leaves the noise standing (a dummy load changes nothing) and cut 4 changes it. Those two results together are the diagnosis.

Cure. The same device you were about to put on the coax, moved to the conductor that is actually carrying the noise: a common-mode choke on the mains lead or on the DC lead. Check the USB and Ethernet runs as well; they are the most commonly missed members of this family.
Never lift the mains protective earth to quieten a noise problem. A common-mode choke passes mains frequency and DC while blocking RF, and that is exactly the behaviour you want: the safety earth stays connected and the noise still gets stopped. Removing the protective earth removes the protection that exists to keep you alive, and in our experience it does not even fix the noise reliably.

Door ①: antenna geometry

An end-fed half wave is fed at a voltage antinode — the point of maximum electric field on the wire. A high-impedance node is inherently sensitive to near-field electric coupling, which is exactly how lamp drivers and small switching supplies mostly couple. The topology that makes the EFHW convenient to hang is also the topology that makes it a good listener for everything in the building.

Signature. The choke makes almost no difference, but moving the antenna changes the noise substantially. Cut 2 collapses the noise, which tells you the wire is doing the listening rather than the braid.

Cure. Geometry, and only geometry: raise it, move it away from the building, change its heading, or add a separate receiving antenna. No amount of ferrite treats this door, and no purchase will either.

Door ④: near field

Your rig, your SDR, a USB lead, an Ethernet run: any of these is a small antenna sitting on your desk, listening to whatever is switching next to it. It is the least exotic door and the easiest to overlook, because the culprit is often something you installed yourself and therefore trust.

Signature. Cut 5 makes the noise follow the device as you walk the house.

Cure. Distance first, ferrites second. Moving a switch-mode wall-wart two metres away from the rig routinely outperforms anything you can do to the antenna system.

How to know, without fooling yourself

The two rules from section 01 apply here in full, and they are the whole method. Everything below is about making them easy to obey.

Compare, do not measure absolutely. And hold everything else still while you compare. Same hour, same frequency, same AGC, same preamp, same attenuation. Change one thing at a time and put it back.

Instruments you may already own

You do not need a laboratory. If your station runs through the MRRC stack, you already have an S-meter feed and a DSP spectrum display — both are sufficient to A/B a choke, provided you keep the receiver settings frozen. A receiver’s spectrum display is the better instrument of the two, because it shows you the shape of the noise as well as its level, and a choke that moves a resonance looks obviously different from one that removes a current.

For an objective, repeatable number that survives across days, the same PSK Reporter analysis this station uses is available to any station with a callsign and some patience: it produces a noise-floor figure from which stations you can hear, and the method is documented on the measured antenna profile page. Run it before the change, run it after, and compare the two.

What you may not claim. A single daylight A/B cannot establish an improvement of any specific size, because the ambient noise field changes underneath you between the two halves of the test. What you can claim is bounded and still useful: the noise was reproducibly lower with the choke in, at these frequencies, at this time of day, with settings frozen. Anything stronger than that needs a longer baseline than most of us are willing to collect, and you should distrust anyone who produces a confident figure from one afternoon.

The same rule, seen from the other side

Section 02 built a verdict table. This is the same table read as a list of things not to waste a ferrite on.

The honest case for a second antenna

The standard answer for a station buried in local noise is to split transmit from receive: keep the EFHW for transmitting, add an active magnetic loop for receiving, aim its null at the noise source, and switch between them with a T/R relay or the rig’s own receive antenna port. It works, it is well established, and the products exist.

But it only helps if you have the disease. Section 01 shows a station that measured its own noise floor, found it clean, and concluded — from data — that a receiving loop would have been money spent on a problem it did not have. Do that measurement before you buy anything. It costs less than the loop, and it might save you the whole purchase.

When the fix belongs to somebody else

Power-line arcing and a neighbour’s charger are the two categories where you cannot treat the source yourself. Both need evidence and a channel. In China the channel is the 12381 hotline, opened on 20 March 2023 as the radio-interference complaint centre under the MIIT public-service platform.

The detail that decides whether your complaint goes anywhere: shortwave and satellite complaints are not handled by local radio administrations. Local offices forward them to the National Radio Monitoring Center and the ministry’s radio bureau. An HF complaint travels upward, not sideways.

Build the log before you call: when it started, which bands, which modes, what it sounds like, and a 30 to 60 second recording in both AM and SSB. This is the same list the ARRL recommends to its own members, and it is what turns “my radio is noisy” into a case.

The one rule with no exceptions. Never lift the mains protective earth, and never advise anyone else to. Every cure on this page works with the safety ground intact, because a choke passes mains frequency and DC while blocking RF. Anything that requires defeating the protective earth is not a cure; it is a hazard.

How to read the labels on this page

Every quantitative statement above carries one of two labels, or it carries a dash.

Label Means
C An engineering claim with a checkable source. The sources are listed below.
算式 Arithmetic you can redo. The formula is always printed next to the numbers, so you can reproduce every cell yourself.
— Not measured, and not guessed at either.
There is no [M] on this page. We did not measure a choke here, so we do not display a measured badge. The one place we cite our own measurements is section 01, and it is labelled with its source file rather than with a badge — which is the honest way round.

Sources

No number on this page was invented. Where we could not find a source, we said so in the card rather than filling the gap — the electric-vehicle section is the clearest example, and it is written that way on purpose.