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Re: [time-nuts] "Shaking" of magnetic shields in atomic clocks

JG
Joseph Gwinn
Wed, Sep 2, 2020 11:32 PM

On Wed, 02 Sep 2020 17:49:47 -0400, time-nuts-request@lists.febo.com
wrote:

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Message: 7
Date: Wed, 2 Sep 2020 14:31:04 -0700
From: "Richard (Rick) Karlquist" richard@karlquist.com
To: Discussion of precise time and frequency measurement
time-nuts@lists.febo.com
Subject: [time-nuts] "Shaking" of magnetic shields in atomic clocks
Message-ID: f8b73f73-c2b1-75b0-6fbf-3aa02990b880@karlquist.com
Content-Type: text/plain; charset=utf-8; format=flowed

In the NIST paper available at the URL below:

At the beginning of page 2 (4th line) the paper
states:

"Note that the shield permeability is a nonlinear function of the
magnetization and increases to a maximum value of umax =400,000 at
higher applied fields. ?Shaking? the shields by continuously
applying an alternating magnetic field is a way to take advantage of umax."

Another paper "The effect of shaking on magnetic shields"
has this abstract:

"The increase of the shielding factor due to shaking was measured in a
scale model for a magnetically shielded room. The increase was found to
be 7 dB for a single-layer square cylinder biased by the Earth's
magnetic field. The shielding factor of a large-volume three-layer
Mumetal ? room was estimated to increase by a factor of 30, thus
confirming the feasibility of shaking in magnetic shields. The shaking
parameters, amplitude, and frequency are not critical according to the
experiments. Winding the shaking coils along the edges of the cubic
shield leads to minimum disturbances inside the cube, and the winding
can also be applied to demagnetize the shield by an alternating field of
25 A/m, 50 Hz. The relative incremental permeability of Mumetal was
studied as a function of the shaking and biasing fields. The
permeability was found to increase considerably by shaking and by
decreasing the biasing field. With zero biasing and with shaking field
of H s = 5 A/m root mean square (rms), 50 Hz, the permeability reached
its maximum value of 89 000, which is sevenfold the value without shaking."

In all my work on atomic standards, I never heard of this.  Has
anyone else heard of this?  I don't understand how a large
AC mag field can be applied to the shield without getting inside
and messing up the atoms by means of Zeeman effect.

BTW, the NIST paper has a nice exact formula for a spherical
magnetic shield (eqn 3 on page 1).  Good reading, as usual from
NIST.

Rick Karlquist
N6RK

I have not read the paper yet, but this reminds me of the use of AC
bias to linearize the magnetic coating of recording tape.  That has the
property of causing linear behavior right through zero average field.

Joe Gwinn

On Wed, 02 Sep 2020 17:49:47 -0400, time-nuts-request@lists.febo.com wrote: > Send time-nuts mailing list submissions to > time-nuts@lists.febo.com > Re: time-nuts Digest, Vol 194, Issue 4 > > Message: 7 > Date: Wed, 2 Sep 2020 14:31:04 -0700 > From: "Richard (Rick) Karlquist" <richard@karlquist.com> > To: Discussion of precise time and frequency measurement > <time-nuts@lists.febo.com> > Subject: [time-nuts] "Shaking" of magnetic shields in atomic clocks > Message-ID: <f8b73f73-c2b1-75b0-6fbf-3aa02990b880@karlquist.com> > Content-Type: text/plain; charset=utf-8; format=flowed > > > In the NIST paper available at the URL below: > > <http://pdfs.semanticscholar.org/47ac/742de238c0ece5e91ff7d12c515b9173eb60.pdf> > > At the beginning of page 2 (4th line) the paper > states: > > "Note that the shield permeability is a nonlinear function of the > magnetization and increases to a maximum value of umax =400,000 at > higher applied fields. ?Shaking? the shields by continuously > applying an alternating magnetic field is a way to take advantage of umax." > > Another paper "The effect of shaking on magnetic shields" > has this abstract: > > "The increase of the shielding factor due to shaking was measured in a > scale model for a magnetically shielded room. The increase was found to > be 7 dB for a single-layer square cylinder biased by the Earth's > magnetic field. The shielding factor of a large-volume three-layer > Mumetal ? room was estimated to increase by a factor of 30, thus > confirming the feasibility of shaking in magnetic shields. The shaking > parameters, amplitude, and frequency are not critical according to the > experiments. Winding the shaking coils along the edges of the cubic > shield leads to minimum disturbances inside the cube, and the winding > can also be applied to demagnetize the shield by an alternating field of > 25 A/m, 50 Hz. The relative incremental permeability of Mumetal was > studied as a function of the shaking and biasing fields. The > permeability was found to increase considerably by shaking and by > decreasing the biasing field. With zero biasing and with shaking field > of H s = 5 A/m root mean square (rms), 50 Hz, the permeability reached > its maximum value of 89 000, which is sevenfold the value without shaking." > > In all my work on atomic standards, I never heard of this. Has > anyone else heard of this? I don't understand how a large > AC mag field can be applied to the shield without getting inside > and messing up the atoms by means of Zeeman effect. > > BTW, the NIST paper has a nice exact formula for a spherical > magnetic shield (eqn 3 on page 1). Good reading, as usual from > NIST. > > Rick Karlquist > N6RK > I have not read the paper yet, but this reminds me of the use of AC bias to linearize the magnetic coating of recording tape. That has the property of causing linear behavior right through zero average field. Joe Gwinn
BB
Bill Byrom
Thu, Sep 3, 2020 6:00 AM

Rick, there appears to be interest in "shaking" the magnetic field for both atomic clocks and medical devices which operate at very small magnetic fields (such as magnetoencephalography). Shaking is mentioned here:
https://en.wikipedia.org/wiki/Magnetoencephalography#Active_shielding_system

I believe that the effect of shaking is to change the average portion of the ferromagnetic material B-H curve the weak external field affects. The incremental permeability (change in magnetic flux density B produced by a small change in magnetizing force H) for a ferromagnetic material is often much larger when the H field is not too close to zero. See this curve:
https://upload.wikimedia.org/wikipedia/commons/thumb/3/3a/Permeability_of_ferromagnet_by_Zureks.svg/996px-Permeability_of_ferromagnet_by_Zureks.svg.png

The incremental permeability (slope of the B-H curve) is highest at a H field value greater than zero. An AC shaking H field component will allow very weak external fields to interact with the high slope portion of the B-H curve. If the shaking field was not present, the external field would interact only with the low permeability area of the B-H curve (near zero). There is best value for the shaking field which corresponds with the peak in the incremental permeability. The shaking frequency should be much greater than the frequencies of interest to reduce interference.

============================
Here are some other references:

Design, construction, and performance of a large-volume magnetic shield
https://www.researchgate.net/publication/3105787_Design_construction_and_performance_of_a_large-volume_magnetic_shield

The best way to achieve good shielding at low frequencies is to combine several methods. Ferromagnetic shielding and active compensation are standard methods for very low frequencies. In ferromagnetic shielding, the walls of a shield are made of high permeability material, and active shielding uses a closed loop control system that controls the field within the shield by special coils driven by a magnetic field sensor. The feedback control system counterbalances the disturbing field by generating a field equal in magnitude and opposite in direction to the disturbance. At higher frequencies, it is possible to use eddy current shielding that takes place when the walls of the shield form a closed enclosure of high electrical conductivity.

Still, one method, so-called shaking, can be used in connection with ferromagnetic shielding. It effectively increases the permeability of a ferromagnetic material by generating a relatively strong alternating field into it. However, it generates extra interference at the shaking frequency.

Separable Magnetic Shield with Magnetic Shaking Enhancement
https://core.ac.uk/display/37850118

Effect of magnetic anisotropy on magnetic shaking
https://ui.adsabs.harvard.edu/abs/1999JAP....85.4645P/abstract

Effective shielding for low-level magnetic fields
https://kyushu-u.pure.elsevier.com/en/publications/effective-shielding-for-low-level-magnetic-fields

Bill Byrom N5BB

On Wed, Sep 2, 2020, at 6:32 PM, Joseph Gwinn wrote:

I have not read the paper yet, but this reminds me of the use of AC
bias to linearize the magnetic coating of recording tape.  That has the
property of causing linear behavior right through zero average field.

Joe Gwinn

On Wed, Sep 2, 2020, at 4:31 PM, Richard (Rick) Karlquist wrote:

In the NIST paper available at the URL below:

http://pdfs.semanticscholar.org/47ac/742de238c0ece5e91ff7d12c515b9173eb60.pdf

At the beginning of page 2 (4th line) the paper
states:

"Note that the shield permeability is a nonlinear function of the
magnetization and increases to a maximum value of umax =400,000 at
higher applied fields. “Shaking” the shields by continuously
applying an alternating magnetic field is a way to take advantage of umax."
... ...
Rick Karlquist
N6RK


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Rick, there appears to be interest in "shaking" the magnetic field for both atomic clocks and medical devices which operate at very small magnetic fields (such as magnetoencephalography). Shaking is mentioned here: https://en.wikipedia.org/wiki/Magnetoencephalography#Active_shielding_system I believe that the effect of shaking is to change the average portion of the ferromagnetic material B-H curve the weak external field affects. The incremental permeability (change in magnetic flux density B produced by a small change in magnetizing force H) for a ferromagnetic material is often much larger when the H field is not too close to zero. See this curve: https://upload.wikimedia.org/wikipedia/commons/thumb/3/3a/Permeability_of_ferromagnet_by_Zureks.svg/996px-Permeability_of_ferromagnet_by_Zureks.svg.png The incremental permeability (slope of the B-H curve) is highest at a H field value greater than zero. An AC shaking H field component will allow very weak external fields to interact with the high slope portion of the B-H curve. If the shaking field was not present, the external field would interact only with the low permeability area of the B-H curve (near zero). There is best value for the shaking field which corresponds with the peak in the incremental permeability. The shaking frequency should be much greater than the frequencies of interest to reduce interference. ============================ Here are some other references: Design, construction, and performance of a large-volume magnetic shield https://www.researchgate.net/publication/3105787_Design_construction_and_performance_of_a_large-volume_magnetic_shield > The best way to achieve good shielding at low frequencies is to combine several methods. Ferromagnetic shielding and active compensation are standard methods for very low frequencies. In ferromagnetic shielding, the walls of a shield are made of high permeability material, and active shielding uses a closed loop control system that controls the field within the shield by special coils driven by a magnetic field sensor. The feedback control system counterbalances the disturbing field by generating a field equal in magnitude and opposite in direction to the disturbance. At higher frequencies, it is possible to use eddy current shielding that takes place when the walls of the shield form a closed enclosure of high electrical conductivity. > > Still, one method, so-called shaking, can be used in connection with ferromagnetic shielding. It effectively increases the permeability of a ferromagnetic material by generating a relatively strong alternating field into it. However, it generates extra interference at the shaking frequency. Separable Magnetic Shield with Magnetic Shaking Enhancement https://core.ac.uk/display/37850118 Effect of magnetic anisotropy on magnetic shaking https://ui.adsabs.harvard.edu/abs/1999JAP....85.4645P/abstract Effective shielding for low-level magnetic fields https://kyushu-u.pure.elsevier.com/en/publications/effective-shielding-for-low-level-magnetic-fields -- Bill Byrom N5BB On Wed, Sep 2, 2020, at 6:32 PM, Joseph Gwinn wrote: > I have not read the paper yet, but this reminds me of the use of AC > bias to linearize the magnetic coating of recording tape. That has the > property of causing linear behavior right through zero average field. > > Joe Gwinn > On Wed, Sep 2, 2020, at 4:31 PM, Richard (Rick) Karlquist wrote: > > In the NIST paper available at the URL below: > > http://pdfs.semanticscholar.org/47ac/742de238c0ece5e91ff7d12c515b9173eb60.pdf > > At the beginning of page 2 (4th line) the paper > states: > > "Note that the shield permeability is a nonlinear function of the > magnetization and increases to a maximum value of umax =400,000 at > higher applied fields. “Shaking” the shields by continuously > applying an alternating magnetic field is a way to take advantage of umax." > ... ... > Rick Karlquist > N6RK > > _______________________________________________ > time-nuts mailing list -- time-nuts@lists.febo.com > To unsubscribe, go to http://lists.febo.com/mailman/listinfo/time-nuts_lists.febo.com > and follow the instructions there. >