Multilayer magnetic shielding

Hi, all,

I learned something recently that might interest the assembled multitude: several thin conducting layers do a much better job of low-frequency magnetic shielding than one thicker layer.

A couple of years back we did a very pretty diode laser controller that runs off +5V. On one credit-card-sized, 8-layer board, it has four switching regulators, an ultralow noise laser diode driver, a Class H Peltier driver and temperature controller, and an MCU for control and communications.

The switchers and MCU are on one side and the analogue stuff on the other. We put the laser driver under the MCU and the TEC stuff under the switchers, because the TEC leads can be filtered easily since they're so slow anyway. The switchers are underneath a tinned steel shield, but there's no iron underneath, just the PCB. The PCB was an eight-layer job with blind vias, which improves shielding a lot since the ground plane is featureless.

Despite switching a few amps at 2.15 MHz, there's no measurable switching junk in the laser supply, even with a 10-Hz IF bandwidth on the spectrum analyzer. (The switchers are locked to the MCU clock, so this isn't a silly statement.)

A similar circuit built on a 4-layer board was much worse. It turns out that having ground pours on six layers below the supply was the golden ticket. (We did that for belt-and-suspenders since we didn't need those layers in that part of the board.)

I took a bunch of data on Friday, suspending a B field loop above one of those cute Murata power modules with the embedded toroid that JL likes so well. The module is soldered to a my usual prototyping setup (a piece of 1-oz two-sided copperclad held inside the lid of a cast-aluminum stomp box by bulkhead BNC connectors). It has a 1.5" x

1", two-piece Leader Tech tinned steel can soldered over it.

The B field loop is a piece of RG-174 with a 3/8"-diameter loop in one end; the end of the shield is insulated but the centre conductor is soldered to the shield about an inch back from the end. It's a DC short, but at AC it's a fully-shielded magnetic dipole pickup. Works great, especially for the price. ;)

The module runs at 90 kHz, and the B-field that gets out of the can is basically solenoidal. (A progressively-wound toroid effectively has a

1-turn, air-core solenoid in series with it.) You can null out the field completely (50 dB or more) by rotating the loop by 90 degrees. The null angle depends on how far the loop is from the axis of the toroid--you have to tip the loop a bit as the direction of the B field changes. So far so hoopy.

I put the proto in a rubber-jaw Panavise and taped the loop on top of a piece of clear PET plastic sheet, fixed to the tops of the jaws so that there was about a 6-mm gap between the shield can and the plastic. That made it convenient to put in various bits of shielding and see what they did.

The spectrum analyzer displayed a forest of spurs going up to at least

10 MHz. (I was using an HP 89441A FFT analyzer without the RF section, and that's as far as it goes.)

The first thing that helped a lot was to solder the lid of the can to the frame. That was good for 15 dB or so.

I have a roll of 3-mil Kapton with 0.5-oz copper on one side, so I cut

2" x 5" strips of it and insulated the copper with packing tape so it wouldn't short out the input and output pi-network filters. I did the same with some 10-mil nickel plated steel from a 70-mm film can and some 1/16" 1100-T0 aluminum.

(Parenthetically, when I was looking at the kickout from the supply input, I noticed that it got much _worse_ when I closed up the stomp box! Apparently the eddy currents in the box material were coupling the stray field from the toroid into the input circuit.)

Getting back to the multilayer thing: each 0.5-oz (17 micron) copper layer knocked the measured B field down by about 11 dB, at least until other factors took over at around -40 dB. The 1.6-mm aluminum sheet was about equal to five layers of copper, despite being almost 20 times thicker overall.

The multiple layers seem to work best when they're insulated from each other, as you'd expect.

I thought I was pretty good a grounding and shielding, but this was an effect I'd never come across.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs
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Can you get deep enough into the Murata power module to stick a loop of wire on top of the toroid to counter-act the single turn formed by the embedded progressively wound toroid? It won't do a perfect job. but it could help quite a bit.

Ripping out the toroid, ripping off half the offending turns and putting them back on to make a non-progressive winding would be a lot more work but might be even more effective.

It's probably a silly question, but not all that silly.

--
Bill Sloman, Sydney
Reply to
Bill Sloman

I use the Murata converters on the bottom of my boards, with the jitter-sensitive parts on top. One ground plane and three power pours between. But I really use the Muratas for their very low output common-mode capacitance, which couples a fraction of the switching current of other converters.

Copper fights fields with eddy currents. PCB thickness copper is transparent at 60 Hz, basically no help at all. It's hard to shield 60 Hz fields.

Murata is doing radical things with PC boards, like that converter with PCB windings and the embedded toroid.

--

John Larkin      Highland Technology, Inc 

The best designs are necessarily accidental.
Reply to
jlarkin

A similar(?) effect is using higher order LC filters: to a point, less energy storage is needed (less total L and C) for a given attenuation at some frequency -- because Fc can be closer. Also may have better stopband attenuation due to more stages of parasitics dividing down (and also using smaller individual components, that are better behaved).

Still, nothing should beat that aluminum plate? I wonder if E field was uncontrolled in your test -- what would've happened if it was grounded to the coax probe, or stomp box?

The coax loop probe as described, isn't perfectly shielded because it's still sensitive to 2nd order effects: E-field coupling into the shield, dropping a voltage across its inductance (so, this way is aggressively more significant at HF) and thus reading a signal off the loop. Or for the best common case, shield split opposite the cable end: perpendicular field won't couple due to symmetry, but a sideways component still can.

But due to that cutoff asymptote, this probably shouldn't explain fundamental getting through.

Hmm, what were the "other things" at -40dB? You say the plate was about equivalent to five layers, but you say four layers stops working? How did you figure this out then?

Tim

-- Seven Transistor Labs, LLC Electrical Engineering Consultation and Design Website:

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Reply to
Tim Williams

Agreed. Two picofarads is really slick.

Well, the skin depth formula has a 1/sqrt(mu) in it, so a bit of magnetic stainless (mu ~ 1500) or low-carbon steel (mu ~4000) can help a lot at low frequency. (Mu metal is generally disappointing because if you look at it crossways it has to be hydrogen-annealed all over again.)

But with nonmagnetic shields at least, multilayer does a massively better job per gram of metal--it's the magnetic equivalent of superinsulation in a vacuum chamber.

It's sort of like the Dick Garwin big-box effect that Win talks about--if the shield is really continuous it works roughly like a metal sheet with thickness

t_eff ~ sqrt(t_shield * D_box),

where D_box is a typical dimension of the box (e.g. its length). That's quite a startling improvement with thin metal.

If they'd just use a non-progressive winding, birds would really chirp.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

Works amazingly well below 10 MHz, for sure. The loop is only 7x12 mm, which isn't a very large fraction of 30 metres. Also you're neglecting the skin effect--ambient HF E fields will induce current on the outside of the shield but not the inside, so it won't couple to the centre conductor.

I admit that hardline would probably work better--a millimetre of solid copper is pretty impermeable to RF--but this gizmo I built out of a dead patch cord is pretty slick, I think.

The main test is that I get a really deep null by orienting the loop correctly. A monopole E-field probe doesn't do that.

The aluminum plate was slightly larger, and it influenced the (small) coupling from the input and output inductors.

The main line of evidence is that the skin depth in copper at 90 kHz is

220 microns, and I'm seeing 10-11 dB attenuation per 17-micron layer, that adds until other stuff takes over at about the -40 dB level. 20*log10( exp(17 um / 220 um)) = 0.67 dB 20*log10( exp(4 * 17 um / 220 um)) = 2.7 dB, not 35-40 dB.

So it ain't skin effect that's doing the heavy lifting at 90 kHz. (The high harmonics die out much more rapidly, so skin effect is having more of an impact out there, as you'd expect.)

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

Could you test with grafoil? Graphite sheets are a 2-D conductor, might have a multilayer effect that goes into the nanoscale, and it's cheap.

Reply to
whit3rd

Possibly. They don't bend or solder as well as copper, though. ;)

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

As you say later, the closed box of conductor effect is pretty useful. It works both ways.. I put a copper tape box over a three terminal SM regulator, and interference took a big drop when I tacked the copper tape to the ground plane.

Your new thing with conductive planes sounds a bit different. Are the dimensions such that the plane looks ~ infinite to the source and detector. (I always need pictures.)

George H.

Reply to
George Herold

Your wish, etc.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

That should be free and easy on the PCB layout.

Youtube has x-rays, with music.

--

John Larkin      Highland Technology, Inc 

The best designs are necessarily accidental.
Reply to
jlarkin

Am 14.02.21 um 20:39 schrieb Phil Hobbs:

This one is broken?

Gerhard

Reply to
Gerhard Hoffmann

Fixed, thanks.

Cheers

Phil Hobbs

-- Dr Philip C D Hobbs Principal Consultant ElectroOptical Innovations LLC / Hobbs ElectroOptics Optics, Electro-optics, Photonics, Analog Electronics Briarcliff Manor NY 10510

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Reply to
Phil Hobbs

The steel is actually 10 mils, i.e. 0.25 mm, not 0.1 mm.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

Thanks... GH

Reply to
George Herold

Phil Hobbs needs to learn to trim.

=================================

** Nonsense - those materials have SFA effect at low magnetising forces.

Mu-Metal is up to 100 times better.

** Is "look at it crossways" an engineering term ??

Millions of audio transformer casings and scope tube shields would disagree with your pessimism

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..... Phil

Reply to
Phil Allison

Have you ever looked at a B-H curve for those steels? You're quite right that mu = dB/dH changes, and its maximum often isn't at H=0, but H_0 is around 100 for carbon steel and 1500 for good magnetic stainless.

The formula is correct, so it does in fact reduce the skin depth accordingly.

Well, you folks seem to think that your own primitive plumbing is somehow a lethal insult to Americans, so who knows?

The shielding effectiveness of mu metal gets trashed if you bend it, and is seriously reduced by just dropping it on the floor. The only cure is re-annealing.

If you have a high volume application and are very careful, mu metal is terrific.

Cheers

Phil Hobbs

--
Dr Philip C D Hobbs 
Principal Consultant 
ElectroOptical Innovations LLC / Hobbs ElectroOptics 
Optics, Electro-optics, Photonics, Analog Electronics 
Briarcliff Manor NY 10510 

http://electrooptical.net 
http://hobbs-eo.com
Reply to
Phil Hobbs

Phil Hobbs wrote: Phil Hobbs needs to learn to trim. =================================

** Yes, plus I have ACTUALLY used the materials.
** Crap.
** What a rude prick you are.
** The second is nonsense - an old wives tale.
** If you have to shape it, then you need re-anneal it. Got nothing to do with how you eyeballs are pointed.

** Shame how the link proves my simple point and negates your mad bullshit.

Go try some carbon steel or magnetic stainless shielding on a scope tube and see how wrong you are.

Fuckwit.

..... Phil

Reply to
Phil Allison

I bet you say that to all the boys. ;)

Cheers

Phil Hobbs

Reply to
Phil Hobbs

Phil Hobbs is an Evil POS narcissist:

========================

** Of course, I wrote much more than that.

All of it apparently too real for the Hobbs prick to answer.

** Bet Hobbs has lots of relations with little boys He's definitely the type.

..... Phil

Reply to
Phil Allison

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