The USBasp is a really useful and quit inexpensive ICSP programmer that suits AVR 8 bit microcontrollers.
This article offers some hints on buying and using the USBasp.
There are lots of sellers of these on eBay, Aliexpress etc… but there are traps in buying them. I recall buying the USBasp with cable for less than $5, but they are more like double that now… or more. Continue reading USBasp – hints
I noted some online discussions where some people had troubles using an ICSP programmer to program the MCU.
I do not have a (tr)uSDX, but inspection of the schematic does hint what those users are doing wrong.
Loading the SCK, MOSI and MISO lines risks problems with operation of the SPI protocol used, but the effect depends to some extent on the driver, length and type of interconnecting cable etc.
Here are some measurements of a USBasp driving an Arduino board with 5V Atmega328P 16MHz chip using about 200mm of ribbon cable… AND the MOSI line is loaded with a 0.01µF capacitor (as in the (tr)uSDX schematic).
As mentioned, ISCP uses an SPI protocol and the capture above uses yellow for SCK and red for MOSI. Continue reading ICSP programming of the (tr)uSDX
Class-E RF power amplifiers have become quite fashionable in ham radio in the last decade or two.
One of, if not the main contribution to efficiency in a Class-E RF amplifier is the operation of the active device in switching mode where it is either not conducting, or conducting hard (saturated, with very little voltage across it). Both of these are very low dissipation conditions, but in the transition between these states there is significant current and voltage present, the product of which gives significant instantaneous power… so the idea is to make this transition very fast so that the average power is low.
This article discusses effect of slowed switching times on PA efficiency.
Above is a circuit above is from (Sokal 2001) which explains the amplifier and gives guidance on selection of components. Continue reading Switching times in Class-E RF power amplifiers
One method described online on YouTube and in social media is the
90° method as I will call it.
The reason why people make measurements at +/- 90 degrees on the smith chart is because the measurement accuracy using the shunt configuration when trying to measure the nominal value of an inductor or capacitor is highest at 0+j50 ohms (or 0-j50 ohms… OD).
To be clear, this is the phase of s11 or Γ being + or – 90° as applicable.
Is there something optimal when phase of s11 is + or – 90°?
Does the software / firmware / hardware give significantly more accurate response under such a termination?
Above is a diagram from a HP publication, slightly altered to suit the discussion. Continue reading NanoVNA-H4 – inductor challenge – part 7
The FNIRSI FNB48 USB meter is a flexible USB power meter that incorporates a facility to measure the resistance of a USB cable. The tested unit uses firmware v2.50.
The operation also needs a constant current load of 0.5 – 1A (for most cables).
The method is: Continue reading FNIRSI FNB48 USB meter – cable resistance measurement
There is a fashion of seeing s21 measurements as the answer to all things, and amongst the revelations is an explanation of measuring inductor Q using s21 shunt through configuration.
Let’s explore the use of s21 shunt through to directly find the half power bandwidth of a series tuned circuit and calculate the Q from that and the resonant frequency (as demonstrated by online posters).
To eliminate most of the uncertainties of measurement, let’s simulate it in Simsmith.
The simulation has a series tuned circuit resonated at 3400kHz, and the source and plot are set to calculate |s21| in dB. Though the model specifies Q independent of frequency, the D block adjusts Q for a constant equivalent series resistance (ESR) which simplifies discussion of resonance and Q. Continue reading NanoVNA – measuring Q of an inductor using s21 – fails?
It is not uncommon that ham designs for Sontheimer coupers (aka Tandem coupler, Grebenkemper coupler) fall short in the design of the magnetic components resulting in one or both of:
- high InsertionVSWR; and
- high core loss.
The above circuit is from (Grebenkemper 1987) and is an embodiment of (Sontheimer 1966). In their various forms, this family of couplers have one or sometimes two transformers with their primary in shunt with the through line. Let’s focus on transformer T2. It samples the though line RF voltage, and its magnetising impedance and transformed load appear in shunt with the through line. T2’s load is usually insignificant, but its magnetising impedance is significant and is often a cause of: Continue reading Sontheimer coupler – transformer issues
A VNA is usually calibrated by the user at some chosen reference plane using standard parts, commonly an open circuit, short circuit, and nominal (50Ω) load. As a result of this OSL calibration, the VNA is able to correct measured s11 to that reference plane, and display its results wrt that reference plane.
There are occasions where it is not possible, or not convenient to locate the DUT at the reference plane. This article discusses the problem created, and some solutions that might give acceptable accuracy for the application at hand.
The discussion assumes the VNA is calibrated for nominal 50+j0Ω.
Above is a diagram of a configuration where the unknown Zl is not located exactly at the reference plane, but at some extension. Continue reading NanoVNA – Port 1 port extension
This article explains the interworking of DiSlord NanoVNA-D v1.1.00 firmware and NanoVNA-App-v1.1.209-OD10 with respect to calibration.
This applies to the specific combination of versions of firmware and software client, do not assume it applies to other combinations.
DiSlord NanoVNA-D v1.1.00 firmware supports a scan_bin command where bit 3 of the outmask field is used to request raw measurement data, ie uncorrected measurements.
NanoVNA-App-v1.1.209-OD10 supports exploitation of that capability when it recognises that firmware version and command support.
Above, NanoVNA-App-v1.1.209-OD10 has a dropdown list to choose calibration mode. Continue reading NanoVNA – DiSlord NanoVNA-D v1.1.00 & NanoVNA-App-v1.1.209-OD10 calibration
I have tidied up and published a calculator I wrote quite some years ago to solve lossy parallel resonance problems.