Eico 723 reverse engineering

The Eico 723 was a 1961 tabletop A1 Morse transmitter with self contained ACpower supply and rated at 60W using 3x6DQ6-B valves.

In the day, transmitters were commonly rated for plate DC input power, probably as it was thought by regulator authorities that it was too challenging to measure RF power output reliably (and for the same reasons the license limitations were cast in DC input. This inflated the capability in terms of todays practice of specifying RF output power.

So, the manual states it has a 500V power supply and to tune / load for 120mA DC plate current.

The operation goes beyond the curves given in the valve datasheet… so a bit of extrapolation is needed to construct a design load line. Continue reading Eico 723 reverse engineering

EFHW compensation, or those little blue capacitors

Constructors tend to copy popular designs, good or bad, and one of the components they see in pics online are the compensation capacitors connected across the 50Ω interface jack.

Single layer high voltage ceramic capacitors are popular, blue is the popular colour for high voltage ones, selected on specified capacitance and some very high voltage rating, often in the range of 3-6kV.

No, I didn’t forget Q, D, tan δ, or ESR… I left them out because constructors don’t seem to consider that part of the requirement.

So let’s review the sense of this. Continue reading EFHW compensation, or those little blue capacitors

Toro MX4250 spindle maintenance

The Toro MX4250 is a ZT ride on mower (riding mower).

I previously reported that after 200h, the original spindle bearings were in very poor condition, about 3mm of play at the blade ends, and they were replaced. There are lots of Chinese parts on this “made in the US made” mower, so the bearings might well have been Chinese in origin.

The original spindles are not greaseable, and were fitted with 6203RS (rubber seals on both sides) ball bearings.

There is lots of stuff online about mower spindles, they are a significant maintenance problem.

A grab bag of online expert advice:

  • No need for greasing, the bearings are sealed for life (that might be less than 100h).
  • Modify residential spindles by adding a grease nipple like commercial mowers use.
  • RS bearings cannot be greased, the seal will pop out.
  • Punch the bearings out, remove the inner seals and put them back.
  • Fit a grease nipple and remove the rubber seal from the inside of both bearings.
  • Some commercial mowers are fitted with a grease nipple and metal shielded (ZZ) bearings.

Since these spindles hold a lot of grease, I intend greasing with a pneumatic greaser, and they tend to inject very quickly and the risk of an RS seal popping should be mitigated.

Above is a 6203ZZ (metal shielded) bearing. There is a gap of about 0.5+mm between bearing inner ring and the shield, shields are on both sides. I note lots of online discussions that incorrectly refer to *RS bearings as shielded. Continue reading Toro MX4250 spindle maintenance

Transformers and magnetic saturation

It seems that even a basic but sound understanding of transformers challenges lots of hams, and even online experts that have been heard to brag of their qualifications so as to intimidate others who might question their words.

So at ARRL EFHW (hfkits.com) antenna kit transformer – revised design #1 – part 2 I estimated that at a current of 4Arms marked the onset of non-linear B-H response, ie the onset of saturation.

One online expert proposed a method that would rate this transformer at maximum 4^2*50=800W at which magnetic saturation would occur.

The referenced article estimated saturation at more like 17000W.

Some very basic transformer concepts

Let’s talk about some really basic transformer concepts.

The diagram above from Wikepedia shows a rectangular magnetic core with two windings, a primary and secondary on opposite limbs of the core.

Note the phase polarity markings (+ / -) and the direction of (conventional) alternating current. Continue reading Transformers and magnetic saturation

ARRL EFHW (hfkits.com) antenna kit transformer – revised design #1 – part 2

This article continues on from several articles that discussed the ARRL EFHW kit transformer, apparently made by hfkits.com, and the revised design at ARRL EFHW (hfkits.com) antenna kit transformer – revised design #1 – part 1.

This article presents a saturation calculation.

You will not often see saturation calcs (for reasons that will become apparent), though you will hear uninformed discussion promoting FUD (fear, uncertainty and doubt).

Lets assume that the core is capable of maximum continuous power dissipation of 10W (limited by factors like safe enclosure temperature, human safety, Curie point etc).

Now let’s estimate the magnetising current for 10W of core dissipation with 3t primary

Starting with the expected permeability above… Continue reading ARRL EFHW (hfkits.com) antenna kit transformer – revised design #1 – part 2

Fact check: “For an antenna, if it doesn’t resonate, it really doesn’t radiate!”

An example of the utter nonsense posted on social media.

My very first posting as a trainee was to Bringelly HF receiving station in 1970. It had Rhombic antennas every 30° of the compass, and a few other antennas, but the mainstay of operation was the set of Rhombics.

The nearby transmitting station at Doonside had a similar antenna arrangement of Rhombics fed with two or four wire open transmission lines to transmitters in a central building, for most operations, no coax involved between transmitters up to 30kW and antenna feed points. Continue reading Fact check: “For an antenna, if it doesn’t resonate, it really doesn’t radiate!”

nanoVNA – are you fazed by phase?

The NanoVNA can measure and display “phase”, is it useful for antenna optimisation?

Some authors pitch it as the magic metric, the thing they lacked with an ordinary SWR meter.

In a context where it seems most hams do not really have a sound understanding of complex numbers (and phase is one ‘dimension’ of a complex quantity like voltage, current, S parameters, impedance, admittance etc), lets look at it from the outside without getting into complex values (as much as possible).

The modern NanoVNA can display three phase quantities, only two are applicable to one port measurements as would commonly be done on an antenna system:

  • s11 phase; and
  • s11 Z phase.

Let’s look at a sweep of a real antenna system from the connector that would attach to the transmitter (this is the reference plane), plotting the two phase quantities s11 phase and s11 Z phase, and SWR (VSWR) and a Smith chart presentation of the s11 measurement.

Above is the measurement of the antenna system.

Like most simple antenna systems (this is a dipole, feedline, ATU), the most appropriate optimisation target is SWR, and minimum SWR well above 7.1MHz.

The SWR is 2.568 at the desired frequency, it is poor.

Do either or both of the phase plots give useful information on the problem, and leads to fix it?

s11 phase

s11 phase is -179.62° at the desired frequency (the marker).

Some authors insist optimal s11 phase is zero, some with a little more (and only a little more) knowledgeable insist it should be either 0° or 180°, take your pick. In fact the latter criteria essentially means the load impedance is purely resistive… but let’s deal with that under the more direct measurement s11 phase of Z.

Phase of -179.62° is approximately -180°=180°.

This metric is not very useful in this case.

s11 phase of Z

s11 phase of Z is -0.4°, approximately zero, which means the load impedance is almost purely resistive.

Of itself, s11 phase of Z does not identify the shortcoming.

So, what is the shortcoming?

If SWR is the optimisation target as proposed for this type of antenna, the SWR is poor, and the minimum is at a significantly higher frequency.

The SWR plot is revealing.

For more information, the value of Z is reported for the Smith chart marker as 19.47-j0.140Ω.

The reason that SWR is not 1.0 is that the feed point impedance is not exactly 50+j0Ω, and the main reason is that the real component is quite low at 19.47 and less importantly there is some very small reactance.

So, this provides information that to improve the match, the real component needs to increase significantly, and some minor trimming of the imaginary component.

Let’s make some matching adjustments

The sweep above is after some adjustment seeking to optimise the match.

Overall, the SWR plot shows that SWR is now fairly good at 7.1MHz, the Smith chart shows the marker just left of the prime centre so R is a little low and X is close to zero, the marker detail shows that Z is 45.57-j0.426Ω, so a little more information than the SWR curve, and with more resolution than reading the Smith chart graphically, R is a little low, X is close to zero. This is good information to guide the next matching steps if one wanted to refine the match.

The phase plots are of almost no value.

Conclusions

  • Neither of the available s11 derived phase plots are of much use for this matching task.
  • The SWR plot gives the best high level indication of the match.
  • Knowledge of R and X components of Z can be helpful in understanding more detail of the match and guiding matching adjustments.
  • This article has not explained the Smith chart in detail, it requires an understanding of complex quantities, so outside the scope and prerequisite knowledge set out for this article. In fact the Smith chart provides insight well beyond any and all of the other plots.

A low Insertion VSWR high Zcm Guanella 1:1 balun for HF – coax bend radius

I see online discussion of specification bending radius for coax cables, and their application to ferrite cored common mode chokes.

A low Insertion VSWR high Zcm Guanella 1:1 balun for HF and follow on articles described a balun with focus on InsertionLoss.

Let’s remind ourselves of the internal layout of the uncompensated balun.

The coax is quality RG58A/U with solid polythene dielectric. The coax is wound with a bending radius of about 10mm, way less than Belden’s specified minimum bending radius of 50mm.

So, the question is does this cause significant centre conductor migration that will ruin the characteristic impedance: Continue reading A low Insertion VSWR high Zcm Guanella 1:1 balun for HF – coax bend radius

Return Loss Bridge – Dunsmore’s bridge

Jeff, K6JCA, kindly sent me a paper, (Dunsmore 1991) which gives design details for a variation of the common resistive Return Loss Bridge design.

This article expands on the discussion at Return Loss Bridge – some important details, exploring Dunsmore’s design.

Dunsmore’s design

Above is Figure 3a from (Dunsmore 1991). Continue reading Return Loss Bridge – Dunsmore’s bridge