A balun puzzle asked several questions of this VK5AJL balun which was cited online.
An online expert quoted the following diagram from VK5AJL.
It is labelled as a simple 1:1 voltage balun, which is to imply that it is NOT a current balun (they are mutually exclusive). Continue reading A balun puzzle
I purchased two replacement batteries type NB-6L for a Canon camera.
Above, the batteries are labelled 1050mAh. They appear to be well made externally, and fit charger and camera fine.
Note that these have different labeling to that shown in the eBay listing. It is naive to expect that the supplied item matches either pics or description, bait and switch is a standard Chinese technique. Continue reading Capacity test of aftermarket NB-6L batteries
A correspondent having read my series Measuring balun common mode impedance – #1 related difficulties with his Rigexpert AA-230Zoom.
The articles showed some techniques for measuring common mode impedance of a current balun.
The following examples are of a test choke wound on a BN43-202 binocular core, and the results are quite similar to what might be expected of a broadband HF current balun. The measurements were made with a Rigexpert AA-600.
Above, the measurement result using RigExpert’s newest software Antscope2. Continue reading Measuring balun common mode impedance – #3
The project is design, implementation and test of a small common mode choke for use with an analyser for antenna measurements.
The choke must have medium to high Zcm from 1 to 30MHz. It is intended to be used with analysers supporting SOL calibration, so effectively any impedance transformation within the fixture is compensated and the reference plane is the load side terminals of the device.
The candidate core is a low cost #43 binocular ferrite core that is fairly easy to obtain.
Above is a first pass check of the likely Zcm at 1.8MHz using a Fair-rite 2843000202 (BN43-202) binocular core. These chokes have relatively low self resonance frequency so a value for Cs is supplied that delivers self resonance at around 5MHz. Zcm at 1.8MHz needs 8-9t, 8.5t will be used (ie the twisted pair enters one end of the binocular and leaves the other end for convenient layout). (8.5t is not strictly correct, but it is a close approximation in this case.)
Continue reading Small common mode choke for analyser antenna measurements using 2843000202 (BN43-202)
For a lot of experiments, knowledge of the Equivalent Noise Bandwidth (ENB) of a receiver is necessary. The ENB is the bandwidth of an ideal rectangular filter with the same gain as some reference frequency.
Though filters are often specified in terms of bandwidth at x dB down, that metric is of relatively little value, the x is often 6dB but not always, the filters depart significantly from ideal or even common response.
In brief, a white noise source is connected to the receiver input, Filter2 (nominal 500Hz bandwidth sharp response) selected and set to standard PBT, and the audio output captured on a PC based audio spectrum analyser, Spectrogram 16 in this case.
Spectrogram is set to integrate over 30s to average the variations due to the noise excitation. The resulting graph and text spectrum log are saved.
The method is explained in detail at Measure IF Bandwidth.
Above is the spectrum plots, as receivers go this is relatively flat.
Continue reading Equivalent noise bandwidth – IC-7300 CW Rx Filter2 – (500Hz sharp)
For a lot of experiments, knowledge of the Equivalent Noise Bandwidth (ENB) of a receiver is necessary. The ENB is the bandwidth of an ideal rectangular filter with the same gain as some reference frequency, 1kHz is usually specified for SSB telephony receiver sensitivity measurement.
Though filters are often specified in terms of bandwidth at x dB down, that metric is of relatively little value, the x is often 6dB but not always, the filters depart significantly from ideal or even common response.
In brief, a white noise source is connected to the receiver input, Filter2 (nominal 2400Hz bandwidth sharp response) selected and set to standard PBT, and the audio output captured on a PC based audio spectrum analyser, Spectrogram 16 in this case.
Spectrogram is set to integrate over 30s to average the variations due to the noise excitation. The resulting graph and text spectrum log are saved.
The method is explained in detail at Measure IF Bandwidth.
Above is the spectrum plots, as receivers go this is relatively flat, lacking the usual tapering off above 1kHz (a technique to cheat on sensitivity specs).
Continue reading Equivalent noise bandwidth – IC-7300 SSB Rx Filter2 – (2400Hz sharp)
The specifications of the DSZH WK-6889 – temperature sensor do not give accuracy or type of the temperature sensors used.
They are most likely to be one of: RTD, thermocouple, or NTC thermistor. Continue reading DSZH WK-6889 – temperature sensor
I am considering replacing the R134a refrigerant in my car aircon system with a hydrocarbon refrigerant. The candidate is Hychill Minus 30 (HC-30).
Comparison of R134a and HyChill Minus 30 gave a limited comparison of R134a and HC-30 from the point of view of pressure temperature behavior as it impact practical implementation and measurement.
This article is a post implementation report, and baseline for future system evaluation.
The vehicle uses a TXV and variable displacement compressor, so low side pressure should be controlled by the variable displacement compressor, and evaporator superheat controlled by the TXV.
The system was evacuated and charged with 240g of HC-30, being 30% of the R134a charge as advised by Hychill, and leak tested.
After settling, on the driveway with no supplemental air flow, fan on full, OAT 22°, on a digital manifold set for R134a, the low side pressure was 255kPa, evaporator outlet 12.9°, displayed superheat 7.2°. At this pressure, R134a calibration reads 2.0° high, so evaporator superheat is corrected to 5.2° which is quite within expectation for a TXV controlled expansion. Continue reading Post implementation review R134a replaced with HyChill Minus 30
Designing with some common Fair-rite binocular ferrite cores can be frustrating because different parameters are published for different material types, and some are controlled for different parameters.
An approach is to derive the key geometry parameter from the published impedance curves and published material complex permeability curves.
For example, the above curves for a 2843002402 (also common known as a BN43-2402) were digitised and iteratively Calculate ferrite cored inductor (from Al) used for find the value of Al that gives the observed value for Z at 10MHz on the chart above. Continue reading Geometry factors for some common Fair-rite binocular ferrite cores