The CADWELDPLUSCU is the igniter for the Cadweld Plus line of electrically initiated thermite weld capsules. The plug seen on the end of the cable slides over the flat connection strip to the capsule.
The environment around the weld crucible is subject to a sudden ejection of hot gases and smoke, much of which is emitted out of the slot in a Oneshot crucible intended for the connection strip, and this is only a 45g capsule. There is probably less gas emitted towards the connector on reusable moulds as the gap for the connection strip is very narrow.
Despite dressing the plug away from the stream of hot gasses emitted, it can be seen above that the plug has suffered heat damage. Of particular concern is deformation of the parts at the cable clamp rendering it less effective. The plugs come on a new lead set that is relatively expensive.
Since one wants to be able to yank the cord away from the crucible as soon as possible to minimise heat damage, the cord grip needs to be effective.
This article describes two measures taken to protect the plug and ensure the cord grip works. Continue reading Cadweld Plus Control Unit
The MFJ-993B auto antenna tuner includes an internal balun, this article is a review of that balun.
The schematic shows the balun as a Guanella 4:1 balun with the usual external link to one of the coaxial antenna sockets. (The label “Z balanced” is misleading, clearly one of the terminals is grounded and this is the unbalanced connection to the coax connector via a link.)
Unlike almost all ATUs with an internal balun, this is a current balun (to their credit), but a 4:1 balun.
There are two aspects of balun behaviour that are of particular interest:
- choking or common mode impedance; and
- impedance transformation.
Continue reading MFJ-993B internal balun review
At MFJ-993B on my G5RV with tuned feeder I discussed first impressions of the replacement ATU.
This article documents the physical layout.
The antenna is a G5RV with tuned feeders (Varney 1958). The tuned feeder is home made two wire line using 2mm diameter copper spaced 50mm.
Above at the right, the open wire line terminates on a home made balun on the feed line entrance panel, see
Design / build project: Guanella 1:1 ‘tuner balun for HF’ – #4 for details of the balun. This is all under the building eaves, but it is waterproof… the area is regularly jetted with high pressure water to clean insects away. Continue reading Shack entry / ATU configuration for my G5RV with tuned feeder
I was given one of these cheap Chinese compression connector tool because “it didn’t work any good”. Continue reading Cheap Chinese compression connector tool
I saw a recent discussion where the blind were leading the blind on the dimensions of a twisted two wire line for Zo=50Ω for use in a balun.
The poster had used an online calculator which used the well known log function for estimating Zo of an air spaced two wire line… the calculator, like most quotations of the formula do not state clearly that it is only an approximation of limited validity, and the calculator returned results for ridiculous inputs (like negative spacing).
The graph above (Duffy 2008) shows the log approximation, and the underlying acosh based estimate. I say estimate because the acosh function does not account for proximity effect which becomes significant at the very closest spacings, and internal inductance which becomes significant at lower frequencies. Proximity effect depends on more than just the spacing/diameter ratio and so cannot be shown on the above graph.
So how did our poster find dimensions for wires for Zo=50Ω when the log graph above shows that as the wire centre to centre spacing approaches the wire diameter, it the wires approach touching, Zo approaches 83Ω? Continue reading Zo of two wire line
I was browsing a ham forum recently when I came across a Return Loss plot apparently from a ham grade miniVNA Tiny.
Lets just remind ourselves of the meaning of the term Return Loss. (IEEE 1988) defines Return Loss as:
(1) (data transmission) (A) At a discontinuity in a transmission system the difference between the power incident upon the discontinuity. (B) The ratio in decibels of the power incident upon the discontinuity to the power reflected from the discontinuity. Note: This ratio is also the square of the reciprocal to the magnitude of the reflection coefficient. (C) More broadly, the return loss is a measure of the dissimilarity between two impedances, being equal to the number of decibels that corresponds to the scalar value of the reciprocal of the reflection coefficient, and hence being expressed by the following formula:
where Z1 and Z2 = the two impedances.
(2) (or gain) (waveguide). The ratio of incident to reflected power at a reference plane of a network.
Return Loss expressed in dB will ALWAYS be a positive number in passive networks.
Return Loss according to the miniVNA Tiny
Above, the miniVNA Tiny presents Return Loss as a negative value. Continue reading The sign of Return Loss
Upon reading Rationale for sizing of lightning down conductor a correspondent asks whether his premises 4mm^2 main earthing conductor ok as a lightning down conductor.
Intended purpose of electrical installation ground electrode
The usual source of current on the premises main earth conductor would be a fault energised by the incoming supply. To understand the implications, lets review the supply system. Continue reading Is the premises main earthing conductor ok as a lightning down conductor
It seems a new version of Rigexpert Antscope has been released, and although it does increase the scale limits available for R,X plots to +/-2000Ω, it still does not allow the range permitted by v4.2.57 (+/-5000Ω).
Back to v4.2.57.
The lightning ground conductor shown at Mast ground rework might at first seem excessive, this article sets out the rationale.
The connection to a 2.4m copper clad steel driven electrode (under the green cover) is 35mm^2 copper.
The nature of lightning protection sizing
Lightning protection sizing is a risk management regime driven by the mechanisms of lightning and variation in distribution.
It is not surprising then that regulatory standards in different distributions broadly use similar design methods but set different practices for implementation in the jurisdiction.
So, let’s go standards shopping… what we are looking for is guidance on the energy (or work) that is directed to heating the down conductor, and choosing a conductor size that will sustain not just a single stroke, or an average stroke, but most events that may include many strokes in a short period of time. Continue reading Rationale for sizing of lightning down conductor
EA2BQH described an adapter to use a JRC NFG-170 NFG-230 ATU.
The description is in Spanish, and a Google translation doesn’t help me much, his published HEX file for a PIC12C508A helps more.
Building the device and observing the output, it seems to have two input pins and when one is high OR the other is low, it sends a ASYNC command string at 1200Bd on its output pin. The command string is repeated every 2.5s if the input condition remains. This string appears to command the ATU to review / retune.
The 12C508A is a very old chip, still available, but in low cost form, an OTP.
I have written some code for a PIC12F510 from the ground up to do a similar thing as far as I can see, and built an adapter for testing by VK1EA.
My redesign uses different pins to the original to better cater for ISCP and to utilise weak pullup as much as feasible. IN1 is pin3 (GP4), IN2 is pin4 (GP3), TX is pin5 (GP2). IN1 OR /IN2 causes the adapter to send the configuration command. The output (TX) is open collector.
Above, a view of the adapter from chip side encapsulated in heatshrink and a patch of double sided adhesive foam to fix it in the ATU. Pin3 is wired to ground, Pin4 (IN2) is green, TX is yellow, ground is black and VDD (5V) is red. Continue reading Command adapter for JRC NFG-170 NFG-230 ATU