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Re: Topband: Measuring Common Mode Chokes

To: topband@contesting.com
Subject: Re: Topband: Measuring Common Mode Chokes
From: Michael Tope <W4EF@dellroy.com>
Date: Thu, 26 Dec 2019 11:09:18 -0800
List-post: <mailto:topband@contesting.com>


On 12/18/2019 3:46 PM, Chuck Hutton wrote:
In the past, I have simply used my N2PK VNA to measure impedance of the choke 
by connecting the shield of the coax to the VNA ports.

Recently I've been discussing common mode chokes with others who have a 
different methodology.
They prefer to do a transmission test through the choke and report the "common mode 
rejection".
This is done by placimg a crossover cable between the VNA output and the choke. 
The choke output is connected in a normal fashion (center to center, shield to 
shield) to the VNA input.

This does not seem ideal to me.
First, the choke is being driven in differential mode rather than common mode.
Second, the measurement depends on (varying) isolation between the coax center 
and shield. So it's not truly common mode rejection.

Am I on thr right track?
A handful of Googles has not netted me any clear summary of test methodology 
for reportimg CMRR. I fimd a small number of tests reportimg impedance.

Chuck

Chuck,

I agree with your assessment of the "crossover cable" method. If understand your description correctly, that puts the choke into a transformer mode where the shield is the primary and the inner conductor is the secondary. IMO, that is not a good way to measure common-mode impedance since the common mode impedance will appear in parallel with the 50 ohm impedance provided by port 2  of the VNA. In principle, I suppose you could de-imbed the common mode impedance from the measured S11. In practice, I can't imagine that being very accurate since you are trying to de-imbed a very high impedance from a very low impedance. A small measurement error, would lead to very large errors in the estimate of the commode mode impedance.

Connecting the respective ends of the choke's coax shield to the respective center conductors of the two VNA ports is a much better method (i.e. VNA_P1--<<--|Zshield|-->>--VNA_P2). In that case the magnitude of the S21, (i.e. MS21dB) should equal 20*log[|50/(Z+50)|]. For large Z, this simplifies to ~20*log(50/|Z|). Thus, if the magnitude of S21 at some frequency is -40dB, then the magnitude of Z at that frequency is ~5000 ohms. If you do the math using the phase of S21, you should be able resolve the resistive and reactive components of |Z|. I think a method similar to this is what K9YC recommends in his app notes on ferrite chokes.

73, Mike W4EF.........

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