A previous article discussed attenuators, the three resistors within them and the need for some of them to be higher power than you'd typically find in your junkbox. Looking at signals up to a watt or two was ok with the attenuators made of smaller low power resistors and I use these to protect my NanoVNA and spectrum analyser. Once the power goes up to 10W you need more expensive resistors, which is why I bought a 10W 40dB attenuator. This allowed me to test my 10W linear Power Amplifier. But it was expensive - I paid nearly £30 for mine.
What to do about testing amplifiers at higher powers? Luckily Wes Hayward W7ZOI designed a "Power Sampler" as part of his 6 page article in ARRL June 2001 entitled "Simple RF-Power Measurement" (Pages 38-43). In it he uses a simple resistive tap and creates a small box with three connectors, Power in, Power Out and Sample out. The sample is 40db below the input. The key to understanding this device is to think of the RF passing through the device, but a tiny portion of it gets passed to the third port. For it to work you need 50 Ohm loads everywhere - a high power dummy load on the power out port and, usually, an instrument with a 50 Ohm input impedance on the sample out port. If 10mW is too high for it you can insert an attenuator between the sample out port and the instrument.
To understand the theory of the sampler you need to know about potential dividers.
I did a spreadsheet to calculate the exact values, these will need confirmed by measurement and calibration. The resistors are 5% and I don't have 51 Ohm resistors at the moment, I can either parallel two 100 Ohm resistors or use a 47 Ohm one. This gives 40.12 dB or 40.39 dB
The spreadsheet is in Figure 3 below and stored on my google drive at Blogfiles folder /Resistive_tap.ods
It is easy to design a low frequency power sampler, at higher frequencies the inductance of even a straight bit of wire, and the capacitance from the resistors matters, the physical layout is critical. To avoid spending ages experimenting I tried to imitate Wes's layout exactly. Though his design is good to 500MHZ, he did use N-type connectors, I choose to use SO237 sockets as I was happy to work with lower frequencies. Wes linked the Power in and Power out with a flat piece of Brass sheet to reduce inductance, a 1 inch by 1.5 inch piece just fits a Hammond 1590A die cast box (the box is fairly small and available from Mouser.com at under £7 or from Amazon at £13 with free postage.). I had some one inch wide thick copper band which would do instead of the brass and I had to purchase half watt, 820 Ohm Carbon Film resistors. (if you want some copper and some resistors free, just ask as I ended up buying 20 for £3!)
Here is Wes's schematic and a drawing of his assembly
Note the flat plate forms L1 and a tiny piece of insulated wire forms C1, it is probably about a third of a picofarad,
C1 extends just over half an inch (0.6") from the plate and is kept parallel and touching R1A and a bit of R1b
Use #22 AWG insulated hookup wire.
Fig 4: Schematic of constructed Power Sampler
(From June 2001 QST © ARRL)
Fig 5: Drawing of the 40dB power Tap assembly. A 1x1.5 inch piece of brass links Power in and out
(From June 2001 QST © ARRL)
Here is a photograph of my case and the tool I used to make the holes for the UHF SO237 and BNC connectors.
Fig 6, the parts of my resistive power tap
The eagle eyed among you may see two 100 Ohm resistors in parallel instead of a single 51 Ohm value - I have none at present so I am making a power tap of -40.12 dB instead of -40.04dB - close enough...I made up the unit with the compensating "capacitor" that the original article describes (a 0.6 inch of 22AWG wire conneced physically close to the first 820 Ohm resistor. I then connected my NanoVNA to the Power in port and the BNC sample port. Most importantly I connected a dummy load to the power out port. I swept the NanoVNA from 3.5MHz to 30MHz for my first test and observed S21. The readings on a poorly calibrated NanoVNA were -40.35dB but more importantly they were flat across the entire HF band. A second sweep to 500MHz showed a 2dB flucuation.
Fig 8: Sweeping from 3.5MHz to 500MHz showed some fluctuations, (this is with no Capacitor)