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Registered Member #2099
Joined: Wed Apr 29 2009, 12:22AM
Location: Los Altos, California
Posts: 1716
Years ago, I made a loop antenna configured much like the one described at My tuning capacitor, like Darrin's, is a good old 365 pF variable unit with air between the plates. The most obvious difference: my coil form is just a flat, square cardboard box. The widely spaced turns of wire rest on the four narrow faces of the box, secured with sticky tape of some kind. A better word would be rested, because the tape has dried up and the turns are falling off. Not yet tangled beyond recovery, but close.
I want to repair or rebuild this and connect a much larger capacitor, to tune for the national time-of-day station WWVB at 60 kHz.
Came here to shamelessly ask, at a forum, about the space between turns. Why not pack the turns closely together, as if one were making a degaussing coil? My guess is to keep the self-capacitance down, and to some extent the inductance, so the Self Resonant Frequency is well above the band of interest.
A hula hoop would make a handy loop-antenna enclosure, but I don't see an easy way to keep wire turns away from each other if they run inside the plastic tube.
Registered Member #72
Joined: Thu Feb 09 2006, 08:29AM
Location: UK St. Albans
Posts: 1659
A while ago I did a bit of head-banging about what influences coil self capacitance, and how to keep it down, starting with the fact that TC secondary calculators seem to give a self capacitance that depends on overall geometry rather than wire and turn-spacing details.
The lightbulb moment was when I found a reference that suggested computing the energy stored when the coil was at peak volts, and then using this to define an effective capacitance. This weights any pair of turns with the square of the voltage between them. What this quickly leads to is that it's not the adjacent inter-turn effects that are important, which it might appear that basket wound coils reduce, but it's the input to output layers and their polarity where you get the most bang for buck, which is what pancake windings are doing. The implication being that for single layer coils, the turn spacing is of much lower importance than the fact that you have a single layer.
I'm not trying to teach you to suck eggs, o granny, but just trying to help other readers understand what's important in the geometry of the coil.
I notice your X-shaped coil is single layer, kept that way by the former. A winding in a hula-hoop would of necessity be multi-layer, so regardless of the turn spacing, the self capacitance would be higher. If you want to wind the coil within the cross section of a hula hoop, and rate the SRF from the best to the worst configuration, most of the benefit will be had by, and in this order, for keeping it in layers ordered from one end to the other, then with the same layer polarity, then with good inter-layer spacing, and finally with good inter-turn spacing. Of course that doesn't make it any easier to compute from geometry and first principles.
If you start with an unloaded coil, it will have a particular SRF. As you increase the external capacitance, the loaded resonant frequency will fall with respect to the unloaded SRF. With a large enough external C, the spacing between the two can be made very large. How large is 'large enough' for any given receiver configuration?
It's long been an amusing thought experiment of mine to make a coil by using a length of flat N-way ribbon cable, soldered in a loop 'off by one', so there's a single conductor looping N times round. This would enforce a single layer geometry and stay flat as long as not forcibly scrunched up.
I must confess I've not figured out or found in a search the scaling laws for SRF of a coil as you increase turns, cross section or diameter, but then I've not applied myself seriously to that yet. These would allow you to perform a small-scale experiment and estimate what a larger hula hoop based coil would do, to see whether scramble wound would be 'good enough'. It's complicated by practical assumptions. Even something as simple as 'for constant cross section and diameter, how does changing the number of turns affect self capacitance?' cannot neglect the fact that inter-layer distance tends to be constant (wire insulation and tape) while wire diameter varies. I'll need to think about that.
I'm not sure yet how you intend to wind a coil inside a hula hoop? Perhaps cut a slot round the outside and simply wind into the former. This would at least achieve a gross input to output ordering, though not really layers. Pulling the wire through again and again with an increasing coil building up seems like awfully hard work, and would still leave an open bit of the hoop, and would probably randomise any hint of 'layer ordering' that you might have wanted to instill. Winding through an outer slot might be improved if for some reason you didn't need to fill the entire cross section with wire, so you wound wire and string together. This would 'bulk up' the winding and increase the inter turn and 'inter layer' spacing, so should reduce self capacitance.
Registered Member #162
Joined: Mon Feb 13 2006, 10:25AM
Location: United Kingdom
Posts: 3141
For a single layer coil, the inter-turn capacitance is not usually critical as it is of moderately high 'Q' it is the proximity effect causing an increase in the effective resistance of the wires I find significant, a winding pitch of 3x wire diameter is a good balance between 'loss' of effective wire csa (increase in resistive loss) versus good inter-turn magnetic coupling to maximise inductance. There are online calculators giving effective height, Q and impedance ... somewhere.
For 60 kHz (wavelength=5km) there are three options that I would consider;
1) An electrostatically shielded ferrite rod 'loopstick' SNR should be good enough for electronic amplification to compensate for antenna gain, and the antenna can easily be rotated to null out the strongest source of interference. This is the prefered commercial solution, using ferrite rods of one to three inches long. Longer = better.
2) Multi-turn loop. Received signal is proportional to Area x #Turns .... wire length. You can choose a small area with lots of turns - easy to rotate but difficult to get high 'Q' or a large area with few turns for better 'Q' but at the expense of rotatability, portability and storage. The loop needs to be vertical, well clear of earth, and aligned to the transmitter. A single-turn pickup loop in the ventre of the main tuning coil can be used to supply a lower impedance (e.g. 300 Ohm ladder) cable and amplifier.
3) A vertical whip, as tall as possible, plus earth. (I use 2nd-hand fishing poles) The whip impedance will be high (e.g. 10m is only 1/500 wavelength) so 'earthing' impedance can be high too. This will be omnidirectional and wideband and very noisy, requiring significant filtering. but allows 'messing about' at other frequencies. (e.g. audio frequencies, or make it 1/4-wavelength at shortwave frequencies of interest - good 'earth' required)
... not Russel! Registered Member #1
Joined: Thu Jan 26 2006, 12:18AM
Location: Tempe, Arizona
Posts: 1052
Not to get too far off topic, but as a fourth option at 60kHz, a short whip with a high input impedance amplifier also works very well. PA0RDT's active whip design works well here, but I've had even better luck with one of the Trask designs, which basically uses a complementary pair of JFETs in push-pull, followed by a second push-pull stage of complementary Darlington BJT pairs. Reception on 60kHz is strong, but of course I'm only one state over from WWVB. VLF transmitters around 24kHz in Hawaii, North Dakota, and Maine are all readily receivable as well.
Still, if the goal is to receive WWVB and only WWVB, it's hard to beat a portable tuned loop or loopstick, if only for their rejection of AM broadcast interference, and the ability to rotate to null out local noise sources.
Edit: note that there's a mistake in the parts list. Q3 and Q4's descriptions should be swapped. Their appearance in the schematic is correct.
... not Russel! Registered Member #1
Joined: Thu Jan 26 2006, 12:18AM
Location: Tempe, Arizona
Posts: 1052
Mostly because the folks turning out well-documented, usable, builder-tested designs with measured IMD, OIP2, and OIP3 characteristics are still using discretes, unfortunately. It's one of the problems Amateur radio is facing: the older "Elmers" are not on the bleeding edge, and those that are on the bleeding edge tend not to be Elmers.
I'm sure there's better silicon out there, but if there are any designs for VLF to VHF active whip amplifiers with extremely good performance characteristics, I haven't seen them, and don't have the time/equipment/expertise to design and test them myself. Regardless, across the VLF and LF spectrum, atmospheric (and man-made) noise is, by far, the limiting factor.
For just receiving one LF frequency, though, I'm sure it wouldn't be hard to put something together with easier-to-source parts that would work well enough.
Registered Member #162
Joined: Mon Feb 13 2006, 10:25AM
Location: United Kingdom
Posts: 3141
Carbon_Rod - Great link ... Thanks. ..........................................
....... Chris Russell, an op-amp such as the LM833 that I mentioned would be good at 60 kHz but useless at VHF. (the amlifier that you showed looks excellent for up to VHF, but would be overkill here) This application of an op-amp specifically at 60 kHz should be simple for 4HV members to implement, basic application notes and 'standard' op-amp topologies, the LM833 is pin-compatible with most dual 8-pin dip op-amps, just a little faster and quieter there is no need to measure r.f. parameters .......................................
.............. I agree with Chris Russell that a short whip is as good as a long one when there is a lot of emi and noise, i.e. the SNR will not be significantly worsened by amplifier noise. (but I work in a shed with external antennas and I prefer a longer whip / larger signal / less amplification)
I have found that a parallel tuned circuit at the bottom of a short whip is best, the inductor shunts accidental d.c. and low frequencies directly to earth, and the capacitor does the same for very high frequencies and of course at the intended resonant frequency it is a tuned circuit that can be tapped for a low impedance amplifier, or fed directly (via protection) to a high impedance amplifier. (allow for c10 pF/m whip capacitance ... from memory, but like TCs, a nearby hand adds significant capacitance) I failed to get a good signal from my 'local' MSF 60 kHz, 75 kW erp at c276 km range, time transmitter, when using a whip in my shed, due to noise and insufficient shielding and filtering. So I still think that a ferrite rod loopstick is best - unless you WANT a huge antenna) (due to my location I mostly use Radio4 198 kHz as a reference)
OR, you could cheat, and buy a radio 'atomic' clock and tap off a signal, e.g. ? ...................................... Plasma, I don't understand the functioning of your circuit, could you elaborate ?
... not Russel! Registered Member #1
Joined: Thu Jan 26 2006, 12:18AM
Location: Tempe, Arizona
Posts: 1052
Sulaiman, my only caveat with not worrying too much about RF parameters would be to ensure that the circuit's response rolls off strongly not too far above 60kHz, so that MW broadcast intermodulation products don't become an issue. The 10kHz channel spacing unfortunately tends to place intermodulation products at nice round spots on the dial, often every 10kHz all the way up and down the band for quite a ways, if there are multiple strong stations nearby.
Personally, I'd also go for the loopstick. Ferrite bars are easily scrounged or found cheaply online. Loopsticks are easy to place in a waterproof enclosure made from PVC or ABS pipe, placed far away from noise sources and oriented for best reception, and even then remotely trimmed via varactor (or reverse-biased LED, in a pinch) if a little wiggle room is desired.
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