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Some secrets of Common Mode Chokes revealed.
pa0nhc 20200315. Update 20210209.
This is a small collection of K9YC info and my experiences.
Read
K9YC articles for more detailed information.

>> FairRite Flyer : Cable Cores For EMI suppression.
>>

CMCs, the influence of temperature changes. pa0nhc 20200530.

>> The all important dipole-end CMC in my Cobra antenna.
>> CMCs (and screening) make very high S/N possible in my wideband active receiving loop antenna.
>> CMCs improve reception with every Miniwhip active wideband E-field receiving antenna.


Some test CMCs wound on 29mm mix #31 cores, with RG58 and RG316 coax.

Only 1.07 Euro / piece.



Only 4,40 Euro / core.


Big transmission CMC  for Medium Wave.
Seven 61mm cores + one big "Snap It".

General rules :

A CMC (Common Mode Choke) with dominant resistive losses will always reduce common mode currents,
regardless of an inductive or capacitive system impedance.
Its bandwidth is large.

At least one CMC should be installed directly near the antenna feed point
(the mid point at a symmetrical dipole).

 

K9YC suggests the use of Fair-Rite mix #31 cores.
Easiest to use are "Snap It" cores, for instance a core with a large 19mm hole 04 31 17 64 51 
Large holes make winding more turns coax possible, resulting in a far more effective CMC.

Buy cheap, buy a larger number :
Order for more than abt. 60 Euros totally at   mouser.com .
Postage from The Netherlands (Europe).
Free postage and no customs costs.

The power of N2.

One 61mm #31 ferrite core with 10 turns 5mm coax cost 4.40 Euro.
It  is at least even effective CMC as
shifting 53 pieces 12.5 mm #31 cores (24.90 Euro) after each other over the coax feeder.

Here is why :

When winding a transmission line "N" times through the hole of a ferrite core,
the ferrite induction and loss resistance will be enlarged with the factor
"N" x "N"  or  "N2".
 
  

A larger loss resistance :
-  a larger reduction of  common mode current,
AND
-  a far larger quadratic reduction of heath generation inside the CMC.
AND
-  the CMC resonance frequency shifts DOWN (mostly a very positive phenomena).

More turns => far less current => (far x far)  less temperature rise in the CMC core.

CMCs in receiving systems.

Small receiving CMCs or transformers.
Order 10 pieces of these 12.5 mm
cores and they cost 0.47 Euro/piece.

In receiving systems are also transformers and CMCs used to suppress noise currents. Small and cheap #31 cores (13x13mm,  26 31 48 00 02) can be used to construct very effective CMCs. Thin wire (0.25mm lacquered coil wire), or a twisted pair retrieved from an UTP cable can be used. 
#31 ferrite is conducting. To prevent damage to the insulation of  lacquered coil wire, these small cores must FIRST be insulated with 2 layers transparent nail lacquer. A short circuit between wire and core results in a useless coil, which is difficult to detect afterwards. Measure the insulation between wires and core before installing the coil into the circuit.

See : http://k9yc.com/RXChokesTransformers.pdf   and  pa0nhc Active RXloop antenna 

CMCs in transmitting systems.


Coax choke on 61mm core..
Max 200W.

K9YC  describes in http://k9yc.com/630MTXChokes.pdf why CMCs should be used in transmit antenna systems.
K9YC advises at least 5 kOhm resistive choke impedance.
For short wave frequencies (2-30 MHz) only use ferrite material #31

As most used coax vary in thickness between 5mm and 11mm, and for instance 7 turns are needed, #31 cores with large holes are to be used.
            For instance :
  29mm core with 19mm hole 26 31 80 12 02
  50mm core with 25mm hole 26 31 62 62 02
 61mm  core with 35mm hole 26 31 80 38 02
101mm core with 76mm hole 26 31 81 40 02

At least one CMC should be installed over the feeder directly near the antenna feed point (near the center of a symmetrical dipole).


Problems by feed lines of 1/2 lambda length.

Due to 1/2 lambda resonance, feed lines having a length of 1/2 lambda (or a multiple :  1, 1.5, 2, 2.5 lambda etc.) will generate strong common mode currents in its center, and very high voltages on its ends.

While receiving, 1/2 lambda feeder resonance can cause strong amplified noises received at all 1/2 lambda feeder resonance frequencies.  See : pa0nhc Active RXloop antenna 

As damping of common mode currents is practically impossible, two measures are possible against 1/2 lambda feeder resonance  : 
1.  Change the length of the feeder, 
                and/or
2.  Install CMCs on the feeder.

     Start at the antenna feed point, and install CMCs over the feeder at distances of 1/4 lambda or less.

In a broadband receiving antenna systems (like my 0-30MHz, 1m dia. active receiving loop) all feeder resonance should be de-tuned to a higher frequency OUTSIDE the used frequency range, that is above 30 MHz. Install the first CMC directly under the antenna, and the last CMC directly near the power/RF combiner. Then fill the rest of the feeder length with CMCs at max. 3m distances.

Antenna unbalance.

            Antenna unbalance results in :
-  Strong common mode currents.
-  High common mode voltages.
-  Heating of CMCs.
-  Radiation of RF in the radio room and houses.
-  RF feedback in microphones.
-  Receiving stronger noises from nearby.
-  Deformation of the antenna radiation pattern.

Antennas which are know for their unbalance and over-heathed CMCs are : FD3, FD4, end-fed, inverted V.  

Unbalance can also be caused by the capacitance introduced by nearby conducting objects, close to one half of the antenna. For instance other antennas, towers, masts, trees.

In a well balanced antenna system, the ferrite core of a good constructed CMC remains cold.
Only the COPPER WIRE inside the hole of the core can show some temperature rise.


Bi-filar (two wire) 61mm  choke.
Max. 700W

Maximal allowed power.

In well matched and well balanced antenna systems, in good CMC's (Z>5kOhms) little heath will be generated.
As long as the common mode voltage over, and the common mode current through the CMC, are small.

One coax choke is good for 100W. An air cooled bi-filar CMC can handle 800W !      ===>>

For larger power levels : connect CMCs in series.

        When connnecting two schokes in series :
-  The total choke-Z will be twice as large.
-  The choke current will be twice as low.
-  The heath developed over these two chokes will be 4x smaller (P = I x I x Z = 1/2 x 1/2 x Z = 1/4 x Z)
-  This heath will be divided over the two chokes.
-  Each single choke will therefore develop 1/8 amount of heath.
-  The allowed max. power will be up to 8x larger.
-  The -3dB bandwidth of the choke combination will be abt. 2x wider.
-  The antenna will therefore be useful over more frequency bands.

Choke winding tips.

        When winding bifilar (two wire) chokes
Twisting of the wires is not allowed. 
Wind both wires close together and in parallel.
Use different colored PTFE wire.

        When winding bi-filar and coax chokes :
Wind in ONE direction around the core, do not wind backwards.
Each turn should lay beside another, not running under or over another turn.

Some background theory.

            SKIN effect.
The conducting screening of a coax cable is divided by the "Skin effect" in two RF conducting layers.
These layers are VERY thin (some thousandths of a mm.).
Both skin layers are therefore isolated from each other for RF energy .

A ferrite Common Mode Choke (CMC) over the coax can only influence the OUTSIDE of the screening.

The first
skin is inside the coax screening (the  differential circuit).
The transport of energy between transmitter and antenna takes place here..

A second layer is at the outside of the screening (the common mode circuit).
This layer caries RF signals (and noises) picked up from surroundings, and RF picked up from the connected antenna.

Common mode current  is bad.

        Common mode current result into :
-  Radiating transmission lines.
-  Deformed antenna radiation pattern.
-  Receiving of noises from surroundings by the feeder line.
-  RF in the radio room.
-  RF feedback in microphones.
-  RF in the house.
-  RF in the houses of neighbors.

How a Common Mode Choke (CMC)  works :

The CMC impedance consists of a series circuit of (induction + capacitance + loss resistance).

A good CMC shows a lot of loss resistance, which will be inserted in series with the common mode circuit
(the OUTER skin of the coax screening) 

Imagine that, at the location of the ferrite choke, the outer skin will be broken u into two insulated parts. And the "loss resistor"  "Z"  is inserted in-between.

 

The higher the "loss resistance" of a CMC, 
the better the reduction of common mode RF current and voltage. 

This "loss resistor" weakens the RF common mode currents, and RF voltage on cable ends.
A good CMC reduces common mode currents and voltages vastly, and over a wide frequency range. 

Why not every ferrite mix performs well in a CMC.

Facts :
1. The common mode circuit of an antenna system can show a capacitive or inductive impedance
at any frequency, at any given point on the whole antenna system.

2. When the ferrite loss resistance of the CMC is to small, its inductance dominates (NOT wanted).


If at the location of the CMC the common mode impedance is inductive,
a dominant inductive CMC will help to weaken common mode currents.

If at the location of the CMC the common mode impedance is capacitive,
a dominant inductive CMC inductance will not reduce the common mode current.
Even resonance between common mode capacitance and the choke inductance could occur, 
possibly resulting in stronger common mode currents (NOT wanted).

A choke which "Z" is dominant RESISTIVE, will always weaken common mode currents.

 

The Q of good CMCs is very low (0.5 to 1)
Their wanted common mode reduction 
BANDWIDTH IS LARGE.
Ferrite material with dominant resistive losses
over a wide bandwidth
should be used. See table. ==>