Now and then, someone accuses the KAT500 of disturbing their impedance match 
even when it is bypassed. I wanted to see just how much residual mismatch the 
KAT500 has when it's in bypass mode, so I made a couple of measurements today. 

I took measurements at 3.6, 7.1 and 28.3 MHz; in other words, on 80, 40 and 10 
meters. I suspected that 10 meters would be close to a worst-case scenario, 
which is why I included it in this test.

In Step 1, I connected my dummy load to the VNA and measured its impedance on 
the three frequencies. In Step 2, I connected the dummy load to the ANT #3 
output of the KAT500 in bypass mode and measured the input impedance of the 
tuner.

Let us begin at 10 meters and get the bad news over with. The dummy load by 
itself, at 28.3 MHz, measured:

48.954 - j*0.032  Ω 

It's hard to digest this, so let's convert that impedance to SWR:  1.021.

Now, the same dummy load through the bypassed KAT500 measured:

46.866 + j*1.498  Ω, or in terms of SWR: 1.074.

Are you alarmed? Let's break this down a bit to understand if this is really, 
really bad, or just kinda bad. 

In an ideal world, when you put a KAT500 into bypass it should 'disappear'. It 
shouldn't change anything. It should feel as if the tuner wasn't there and you 
were directly connected to the dummy load or whatever is on the output of the 
tuner. And you should measure the same exact impedance as when the tuner really 
was out of the picture.

But in reality, this is impossible. Even when bypassed, a device like an 
antenna tuner adds length -- the distance between the input and output 
connectors-- and this length, like all conductors, has a little bit of 
inductance. The tuner is also going to add stray capacitance. Imagine shrinking 
down to the size of an electron and entering the tuner through the coax. The 
first thing you see is a coax connector, followed by a cable, a relay, a 
circuit board, another thingy maybe, and eventually you emerge from the tuner 
at another rear panel coax connector. By traversing this path, you were 
subjected to the stray capacitance and inductance of all the stuff you touched 
or passed by. By virtue of being in the real world, the tuner doesn't disappear 
but in fact adds a measurable perturbation to an otherwise pristine path.

How much did my KAT500 add in this real and imperfect world?

In order to bump the dummy load's impedance to the new value I measured, the 
KAT500 had to add the following: 

24.2 pF of stray capacitance -- a totally believeable value, and
64.1 nH of inductance from the path -- again, a value in line with reality.

In case you're still laboring under a pretty good shock right now, don't be too 
scandalized. Perhaps it's helpful to recall this: First, you've heard of 
LMR-400 coax, right? Well, LMR-400 coax has a capacitance of 24 pF per foot. 
That's right, just 1 foot of this pretty good coax has 24 pF (actually 23.922 
pF, according to renowned transmission line guru AC6LA). Second, that same 
piece of coax has 61.5 nH of inductance. Holy smokes, those numbers are darned 
close to the KAT500's!!

The KAT500, when all is said and done, looks pretty much like a short 1-foot 
section of very good coax when it is bypassed, with a tiny bit of mismatch 
thrown in for good measure.

In addition, I wish I could post a screenshot of my Smith Chart with the before 
and after impedance values plotted on it. The distance between the two points 
is far less than 1/100 of the diameter of the Smith chart. The two points are 
virtually on top of each other. It's only because of the resolution of the test 
equipment that we can even see the difference between 1.021 and 1.074.

(On 80 and 40 meters the difference is literally two-tenths of an ohm-- not 
even worth mentioning here.)

I hope that this put a new perspective on something that we see here on the 
reflector rather often. 

Regards,

Al  W6LX/4





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