Ferrite resistivity

So following a comment by Mikko that ferrites stop working when cooled to liq. helium temperatures. I =91discovered=92 that ferrites have a phase change somewhere near 120 K. (at least magnetite does.) Google =93Verwey transition=94 Wiki is mostly silent on the subject though there is a bit here.

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So first I=92m a ferrite novice. I=92ve wound some RF transformers in the deep past, but that=92s about it. I found that I could measure the resistivity of some ferrite beads with just my DMM. I=92ve got two types of bead the 43 material and the

73 material. The reported resistivity=92s are 43 =3D 1E5 ohm-cm and 73 is 100 ohm-cm.

I made a little jig to squeeze the beads in. The brass screw has a cone turned on the end.

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So first off there seems to be a huge variation in the piece to piece resistivity. At least an order of magnitude in the few pieces I looked at. Second the resistivity was (most of the time) much higher than the reported numbers.

1E6 to 1E7 for the 43 material and 3E3 to 2E2 for the 73. (The 200 Ohm-cm for one piece of 73 was about right.)

And finally the 43 material was some older stuff in my parts box. I=92m not quite sure of it=92s provenance. So I got some new pieces out of stock. For the new material I couldn=92t measure the resistance with my setup. I even biased the bead from a 30 volt supply and used the

10Meg of the DMM as a voltage divider... I could measure a 1 G-ohm resistor that way, but not the beads! resistance greater than 10 G ohm or os.

I=92m wondering if anyone has some more in depth knowledge they might share. The ferrites look like they might be a =91model system=92 for some new solid state experiments. Besides looking at the Curie temperature the phase transition at 120K shows a peak in the heat capacity, change in resistivity and magnetic properties. What could be better!

Thanks,

George H.

Reply to
George Herold
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[and on resistivity of the ferrite material]

Probably the resistivity is quoted mainly because it affects inductor Q. Ferrites are, alas, composite materials; the magnetic grains (of hopefully uniform size, big enough to magnetize) are in a matrix of fired ceramic like kaolin clay. So, electric conduction depends on percolation through the ceramic matrix, or through contact between grains, or in the boundary layer where the kaolin is in contact with the hematite/magnetite. =20

It is dubious that resistivity repeats from batch to batch, or from one con= tact point to another. A bit of internal fracture might not change the magnetic properties much, but would kill a resistivity measurement. I've done impedance measurement on ferrites that had LOTS of internal movement, at some frequencies the internal fractures rang like a lossy bell.

Reply to
whit3rd

For a 2-terminal measurement, the contact footprint, down to the microscopic level, may matter.

What's soft, compliant, and has high conductivity?

4-wire would be better, with the sample points nearer the center, well away from the outer current contacts.
--

John Larkin         Highland Technology, Inc

jlarkin at highlandtechnology dot com
http://www.highlandtechnology.com

Precision electronic instrumentation
Picosecond-resolution Digital Delay and Pulse generators
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Reply to
John Larkin

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Farnell don't seem to stock it any more, so you may find it difficult get hold of.

The Kelvin connection scheme is always attractive.

-- Bill Sloman, Nijmegen

Reply to
Bill Sloman

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I did stick the extreme pieces of 73 on an SRS RCL meter. (1.2k and

25k) (wire through the bead) The 25k did show less resistance and higher Q consitent with the resistivity... but only a 10-20% difference.

So if most of the resistance is because of some random path... I still should be able to see any phase change in the resistivity.

George H.

Reply to
George Herold

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Sure, the resistance changed as I cranked on the screw. But only by maybe a factor of 2 or 3. I could tighten things up to within ~20% of the cracking point.... after I'd cracked a few beads.

Oh yeah this was very crude... the spinning of the screw was the worst part.

I tried using some 'gummy' copper tape as a 'gasket', but it spun off into a crumple ball.

Hmmm.. those beads aint so big, making two more (ring?) terminals would be real work.

George H.

ed text -

Reply to
George Herold

Although this is a useful method to differentiate the two materials, it's not going to give meaningful bulk resistivity information.

The higher resistivity material is sintered in a fairly crystaline structure, with insulator/semiconductor type relationships between domain groups. You can't count on it functioning as an insulator in-circuit, because this characteristic is uncontrolled - but you sure can count on the low resistivity stuff causing shorts, if misapplied in a higher voltage circuit.

Some materials are not formed as individual beads, but are machined from tubular structures, or finished into their final dimensions by grinding, The machined parts provide a more reliable contact to the bulk material, but their function is also marginally affected due to the reduced bulk impedance at the machined surface.

It used to be that low resistivity, low frequency parts also had noticably lower currie temperatures. This restricts uses of parts in places where significant power loss is expected - they become loss-self-regulating, much like an NTC resistor - which is no good if a loss must be absorbed and the site of application isn't heatsunk in some way.

RL

Reply to
legg

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Thanks, If this works I can try looking for better samples. The ferrite beads are probably the 'low end' of the production run.

A low Curie temperature would be attactive. (easier to reach) I like this melamine foam which is good to?? (at least 140 C)

George H.

Reply to
George Herold

Cylindrical, flat contacts would be best. Lead or solder foil might be a nice, soft, sorta compressable contact. Or mercury!

--

John Larkin         Highland Technology, Inc

jlarkin at highlandtechnology dot com
http://www.highlandtechnology.com

Precision electronic instrumentation
Picosecond-resolution Digital Delay and Pulse generators
Custom laser drivers and controllers
Photonics and fiberoptic TTL data links
VME thermocouple, LVDT, synchro   acquisition and simulation
Reply to
John Larkin

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Hmm, I think the first thing I need to get rid of is the twisting motion of the screw. I don't quite see how to do that. (And keep the large adjustment range.)

Now here's a question for your four point measurement suggestion.

If I've got some random walk conduction through the sample... (to explain the large resistance) Then when I put on my two voltage probes, do they make random walks through the sample too? In which case the position of the volatge probes becomes only an approximate measure of the distance along the conduction channel.

Hey, can I do some sort of AC measurement that probes shorter range conduction? Or is that at a very high frequency?

George H.

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Reply to
George Herold

My ferrite knowledge is about 40 years old, from the Philips plant where I worked as ferrite lab engineeer, so there are probably newer compositions on the market.

Ferrites are solid solutions of either manganese or nickel and zinc and iron oxides, sintered to form micro crystals around 1 micron size. Each crystal is intended to be one magnetic domain, for lowest losses. There are minor but well controlled additions of silica and/or calcium oxides which act as glassy insulators between the ferrite grains. In the manganese-zince ferrites there is also a critical amount of FeO in the inter-grain spaces, whereas the grains themselves are MnO2-ZnO-Fe2O3. ( Magnetite, Fe3O4 is really a solid solution of FeO in Fe2O3, ie its a 'ferrite' without the manganese, nickel or zinc components ).

Basically there are two formulations:

Manganese zinc ferrites For low frequency, say 1 KHz to 200 KHz. High permeability, around 2000 and up, low resistivity, around 100-1 kohm-cm or so. Curie temp around 150-200 degC, depending on formulation ( manganese-zinc ratio ).

Nickel zinc ferrites For high frequency, say 500 KHz to 50 MHz. Permeability around 50-500, high resistivity, around 1e9 ohm-cm or higher. Curie temp 200-500 degC, again depending on formulation ( nickel-zinc ratio ).

Resistivity is not well controlled, and only has a small part in ferrite losses. It also has very high negative, and very uncontrolled, temp coeff.

Ferrites are optimised for work around -20 to about +100 deg C. Below that, the permeability falls rapidly, and there may well be phase changes, as you already discovered.

--
Regards,

Adrian Jansen           adrianjansen at internode dot on dot net
Note reply address is invalid, convert address above to machine form.
Reply to
Adrian Jansen

Yes, we had some offline discussion with George about the phenomenon. The microscopic mechanism behing Verwey transition is quite intriguiging, and its existence does not seem to be widely known

- at least I had never heard about it before (well, if its covered in Kittel that is just my ignorance, we followed Aschroft-Mermin...). The ferrites I have tested in LHe have all been the standard MnZn or NiZn spinel types (it seems hard to find other types, like garnets, sold in small quantities) and it sounds likely that it was exactly the Verwey transition which killed them - assuming the transition also happens in mixed spinels, the papers I've found only describe pure magnetite.

Anyone knows an easy small-quantity source for microwave ferrites, by the way?

Regards, Mikko

Reply to
Mr Stonebeach

I read a paper where someone 'measured' the precession rate of the 'available magnetic molecules and it was in the range of 1 to 2 GHz, which the author used to explain why there are no microwave ferrites.

In my experience, 1 GHz was about the upper limit, air core above that was far more effective, and for EMI graphite..

Reply to
Robert Macy

Hi Robert, thanks for your insight. Do you happen to remember a reference to the paper?

To me it looks that Mini-Circuits transformers do use magnetic cores, see e.g. http://217.34.103.131/pdfs/TC1.5-1X+.pdf http://217.34.103.131/pdfs/TCM2-33X+.pdf http://217.34.103.131/pdfs/TC4-14+.pdf

There are also all sorts of tuneable microvawe thingies which make use of YIG garnets.

Then there are circulators available for a wide variety of frequencies, those must utilize ferrite cores, no?

Regards, Mikko

Reply to
Mr Stonebeach

MCL mostly makes transmission line transformers, so the cores are there to extend the low-frequency response. TLTs are also pretty well completely insensitive to core loss, since their main operating mode produces zero core magnetization.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC
Optics, Electro-optics, Photonics, Analog Electronics

160 North State Road #203
Briarcliff Manor NY 10510
845-480-2058

hobbs at electrooptical dot net
http://electrooptical.net
Reply to
Phil Hobbs

Minicircuits makes both TLT:s and ordinary ones. Eg. http://217.34.103.131/pdfs/TC1.5-1X+.pdf is an ordinary transformer (judging by the 'Config D' in the data sheet), and the in the photograph it looks to me like having a magnetic core.

An example of their TLT's is http://217.34.103.131/pdfs/TC4-25+.pdf which is clearly indicated as 'Config. H' in the datasheet.

There are a large variety of companies like

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but I still haven't found one with a small-quantity webstore. My first guess was RELL but I wasn't able to find the stuff there.

Regards, Mikko

Reply to
Mr Stonebeach

I always thought this was very cool,

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but then I'm easily amused. Slipping some ferrites over the coax, anywhere, extends the LF response.

PSPL sells this in a box for big bucks.

--

John Larkin                  Highland Technology Inc
www.highlandtechnology.com   jlarkin at highlandtechnology dot com   

Precision electronic instrumentation
Picosecond-resolution Digital Delay and Pulse generators
Custom timing and laser controllers
Photonics and fiberoptic TTL data links
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Multichannel arbitrary waveform generators
Reply to
John Larkin

Adrian - great to hear something from the horses mouth for a change. Copied to my magnetics article index, with your permission, I hope.

RL

Reply to
legg

Interesting point. 1.5 isn't an available impedance ratio, so I expect it's actually 5:4 or 6:5 turns. You could do that as a mostly-bifilar winding with one extra turn--maybe that green wire in the foreground. Not as good as a real TLT, but not as bad as a split-winding toroid.

The place I mostly buy cores is Amidon, but they don't go up that high.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC
Optics, Electro-optics, Photonics, Analog Electronics

160 North State Road #203
Briarcliff Manor NY 10510
845-480-2058

hobbs at electrooptical dot net
http://electrooptical.net
Reply to
Phil Hobbs

So why not undercut them? Some microwave things would be pretty cool if you could make them work well in the time domain, e.g. splitters, directional couplers, isolators, and so on. I wonder what the BW limit for practical 90 degree splitters really is?

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs
Principal Consultant
ElectroOptical Innovations LLC
Optics, Electro-optics, Photonics, Analog Electronics

160 North State Road #203
Briarcliff Manor NY 10510
845-480-2058

hobbs at electrooptical dot net
http://electrooptical.net
Reply to
Phil Hobbs

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