A donut electromagnetic core comprises main section + movable section

In summary, the movable section of the O-ring magnetic core has two air gaps between it and the stator main section. The rotation does not change the outlook of the whole O-ring core, so the gaps keep the same volume.
  • #1
cairoliu
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TL;DR Summary
pure magnetism problem
There is a short movable section of cylinder shape in a O-ring magnetic core with DC coil, of course, there are 2 air gaps between the movable section and stator main section. My question: if rotate the movable section, is there a bunch of twisted magnetic lines?
The rotation does not change the outlook of whole O-ring core, so gaps keep same volume.
 
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  • #2
Can you upload a sketch? I'm having trouble visualizing what you are describing. Use the "Attach files" link below the Edit window to upload a PDF or JPEG copy of your sketch. Thanks.
 
  • #3
mag-fig.png
 
  • #4
Thanks for the drawing. If the cylinder is ferrous, the B-field lines from the C-core will just go right through it, with a little fringing at the two air gaps. The cylinder will be in an unstable position, so will need to be supported against thrust in the vertical direction. I don't see anything that will cause the cylinder to rotate about its dotted-line axis that you show.
 
  • #5
The field lines will readjust to minimize their path length (i.e. straight) almost instantly. Unless your spinning that think near the speed of light, LOL.

edit: Maybe the worst sentence I ever typed.
 
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  • #6
Though undrawn in the sketch, I can use a motor to drive the cylinder via belt, of course bearings are needed to keep stable.

Both the stator main section & the rotatable short section are made of same magnetic material, e.g. silicon steel etc.

Are you sure the MagnetoMotive Force (MMF) lines will not twisted within the gaps?
I remember textbooks state there are lots of magnetic domains inside magnetic materials, and MMF lines go through magnetic domains; so if the said section is rotating, then supposedly MMF lines should be twisted.

It seems experiment can be done like this:
scatter some ferrous powder on a hard paper, then insert the paper in a gap, hold at hand, and make sure the paper not touch the stator or the rotor. watch the powder during rotation.

Not test, just by theory imagination now.
 
  • #7
DaveE said:
The field lines will readjust to minimize their path length (i.e. straight) almost instantly. Unless your spinning that think near the speed of light, LOL.
I remember textbooks state there are lots of magnetic domains inside magnetic materials, and MMF lines go through magnetic domains; so if the said section is rotating, then supposedly MMF lines should be twisted.

So I guess regular speed can render the twisting effect.
 
  • #8
berkeman said:
Thanks for the drawing. If the cylinder is ferrous, the B-field lines from the C-core will just go right through it, with a little fringing at the two air gaps. The cylinder will be in an unstable position, so will need to be supported against thrust in the vertical direction. I don't see anything that will cause the cylinder to rotate about its dotted-line axis that you show.
see my reply in #6
 
  • #9
cairoliu said:
It seems experiment can be done like this:
scatter some ferrous powder on a hard paper, then insert the paper in a gap, hold at hand, and make sure the paper not touch the stator or the rotor. watch the powder during rotation.
The ferrous powder will be attracted to the nearest pole of the C-core. If you want to keep it in place, maybe put it between two microscope glass slides separated by a small 1-2mm spacer around the periphery of the slides. I'm guessing the experiment will not show any movement/drag of the powder between the slides as you rotate the slides in the gap.
 
  • #10
TLDR: EM waves move fast. Really, really fast.

Any sort of anisotropy or inhomogeneity in the permeability of the core will create a corresponding difference in the flux distribution. So yes, if you prefer, they do twist and then readjust at almost the speed of light*. Also If you move the material the flux distribution will move along with it. In the frame of reference of the spinning part, there should be no changes based on rotational speed within realistic limits.

* 99.999% BS. I have no idea what happens in this case near the speed of light. But I know what happens at normal speeds.
 
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  • #11
DaveE said:
The field lines will readjust to minimize their path length (i.e. straight) almost instantly. Unless your spinning that think near the speed of light, LOL.
Instantly minimize their path length between magnetic domains?
Does it mean the so-called magnetic re-connection that often refers to solar surface magnetic phenomenon?
 
  • #12
cairoliu said:
Instantly minimize their path length between magnetic domains?
Yes.

cairoliu said:
Does it means the so-called magnetic re-connection that often refers to solar surface magnetic phenomenon?
Let's leave the sun out of this. It's a gas/fluid/plasma that changes in response to the EM excitation, unlike your core. Neither you, nor I, are ready for magnetohydrodynamics. If you want to know about that, start another thread.
 
  • #13
DaveE said:
TLDR: EM waves move fast. Really, really fast.

Any sort of anisotropy or inhomogeneity in the permeability of the core will create a corresponding difference in the flux distribution. So yes, if you prefer, they do twist and then readjust at almost the speed of light*. Also If you move the material the flux distribution will move along with it. In the frame of reference of the spinning part, there should be no changes based on rotational speed within realistic limits.

* 99.999% BS. I have no idea what happens in this case near the speed of light. But I know what happens at normal speeds.
If I paste a copper wire on top surface of the movable magnetic core, then the conductor wire will cut MMF lines during rotation.

My new question: is there the induced voltage between the two ends of wire?

Of course, I know there must be an induced voltage, if keep the movable section standstill and let the wire independently cut through the gap.

But now the wire and the movable section are bounded together, and move together, so the induced voltage may no longer exist? or not render the same voltage value as scenario of everything standstill except the wire?

In new scenario, the movable section can be imagined as an infinite area plate, not have to rotate, but simply linear move.
 
  • #14
The "ends" of your wire will be part of a loop (circuit), for example including your voltmeter leads. Any change in the total magnetic flux passing through that loop, either due to a time variation or spatial movement, will induce a voltage according to Faraday's Law. So I'm a bit unclear about how the field lines in your experiment are distributed throughout that entire loop.

BTW, you often get more or better answers if you start a new thread when your questions change. The only people likely to see this are those who responded to your original question.
 
  • #15
DaveE said:
The "ends" of your wire will be part of a loop (circuit), for example including your voltmeter leads. Any change in the total magnetic flux passing through that loop, either due to a time variation or spatial movement, will induce a voltage according to Faraday's Law. So I'm a bit unclear about how the field lines in your experiment are distributed throughout that entire loop.

BTW, you often get more or better answers if you start a new thread when your questions change. The only people likely to see this are those who responded to your original question.
Only the wire is in B field, and motion direction is vertical to B, the wire is a part of a loop, and other parts of loop is outside the B field.
So what's the result in this scenario of wire going with the magnetic plate?

BTW I will follow your advice in next topic, new thread for new subject. thanks.
 
  • #16
If the flux within the loop doesn't change, there will be no voltage induced. The concept is relatively simple compared to actually knowing where the magnetic flux is. It's sort of a bookkeeping problem. Sorry, I don't know what "vertical to B" means. Nearly every time you see a problem like this it comes with a sketch of the geometry and field lines (flux). That's one big advantage to magnetic cores; you know where the flux goes and can usually ignore the flux outside of the core.
 
  • #17
It seems to me that you are overthinking this. For the cylinder to start spinning, there needs to be a toque on it. A torque means that the energy at one angle φ is different from another angle. But, assuming isotropic materials, this is not the case. So no torque.

If you want to ask about anisotropic materials, draw how they were anisotropic. However, it is all but certain that the torque changes sign as the cylinder rotates, so it will rotate to some configuration and stop because of friction.
 
  • #18
Vanadium 50 said:
It seems to me that you are overthinking this. For the cylinder to start spinning, there needs to be a toque on it. A torque means that the energy at one angle φ is different from another angle. But, assuming isotropic materials, this is not the case. So no torque.

If you want to ask about anisotropic materials, draw how they were anisotropic. However, it is all but certain that the torque changes sign as the cylinder rotates, so it will rotate to some configuration and stop because of friction.
cairoliu said:
Though undrawn in the sketch, I can use a motor to drive the cylinder via belt, of course bearings are needed to keep stable.

Both the stator main section & the rotatable short section are made of same magnetic material, e.g. silicon steel etc.

It won't stop unless his motor stops. I have no idea what the point of the apparatus is though.
 
  • #19
Vanadium 50 said:
It seems to me that you are overthinking this. For the cylinder to start spinning, there needs to be a toque on it. A torque means that the energy at one angle φ is different from another angle. But, assuming isotropic materials, this is not the case. So no torque.

If you want to ask about anisotropic materials, draw how they were anisotropic. However, it is all but certain that the torque changes sign as the cylinder rotates, so it will rotate to some configuration and stop because of friction.
From reply #13, then after, I assume the cylinder is replaced with an infinite area plate with thickness equal to original height of the solid cylinder, and no more rotation, but linear motion.

My only concern is whether the motion of wire (combined with plate), is affected by the plate in term of induction effect.

By my imagination, the contact area between wire and plate seems not to cut B flux, as the motion may stickily drag the MMF lines if not instant straightening (reconnect to nearest magnetic domains); only the wire upper portion causes flux change?

Following sketch illustrates the combined wire and plate moving towards reader.

If the plate is attached with the C core, and let the wire independently move, is there the same induction effect?
mag-induction.png
 
  • #22
cairoliu said:
university
Then you should be posting equations in support of your questions. Please use LaTeX to post math here at PF -- see the "LaTeX Guide" link below the Edit window to learn how to post math using LaTeX. Thanks. :smile:
 
  • #23
berkeman said:
Then you should be posting equations in support of your questions. Please use LaTeX to post math here at PF -- see the "LaTeX Guide" link below the Edit window to learn how to post math using LaTeX. Thanks. :smile:
BTW @cairoliu I don't mean my comments to be insulting at all. It's just frustrating when you throw out ideas that should be addressed in a straightforward way by writing the applicable equations and then asking questions about those equations. The more math that you can include with your questions and the more links to your reading about those questions, the better we can try to help you with understanding what will happen. Thanks. :smile:
 
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  • #24
berkeman said:
BTW @cairoliu I don't mean my comments to be insulting at all. It's just frustrating when you throw out ideas that should be addressed in a straightforward way by writing the applicable equations and then asking questions about those equations. The more math that you can include with your questions and the more links to your reading about those questions, the better we can try to help you with understanding what will happen. Thanks. :smile:
I understand you.

Seeking answer for my question is not for my theoretical interest, but serve my engineering need, I'm trying to reinvent the "wheel" of DC motor with slip ring.

I hate to let the magnetic media move, but have to wind wire to a rotatable magnetic media.

Now I think the moving magnetic media seems not to affect conductor's induction, as DaveE says the MMF lines probably instant straightening.
 
  • #25
cairoliu said:
Seeking answer for my question is not for my theoretical interest, but serve my engineering need, I'm trying to reinvent the "wheel" of DC motor with slip ring.
What reading have you done so far in your re-invention research for electric motors? What are the different electric motor types and their advantages/disadvantages/applications? That's a good place to start, IMO.
 
  • #26
berkeman said:
What reading have you done so far in your re-invention research for electric motors? What are the different electric motor types and their advantages/disadvantages/applications? That's a good place to start, IMO.
All brushed DC motors only use commutators, which generate nasty sparks and EM interference.
If using slip ring in DC motor, then no spark no EM interference, everyone will be happy, but I cannot find a DC motor with slip ring in market.
 
  • #27
cairoliu said:
All brushed DC motors only use commutators, which generate nasty sparks and EM interference.
If using slip ring in DC motor, then no spark no EM interference, everyone will be happy, but I cannot find a DC motor with slip ring in market.
Please always post links to your reading on your questions in the technical forums. Otherwise we have to do our own searches:

https://www.moflon.com/showen127.html

Paging @anorlunda
 
  • #29
I'm having trouble figuring out the question in this thread. @cairoliu, can you restate the question from scratch?

cairoliu said:
Instantly minimize their path length between magnetic domains?
That sounds reminiscent of a reluctance motor.
 
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  • #30
@cairoliu

I believe what your asking in the first post of this thread is "do magnetic field lines move together with a perfectly symmetrical magnet that is rotated around it's axis of symmetry and that is also polarized along the same axis of symmetry.

The answer is NO! Magnetic field lines are a human made construct to help aide thinking, their not real, there is just a physical phenomenon called magnetic field.
Magnetic field doesn't move, it only has a quantity named "field strength" and this quantity changes if you change your distance to the field source.
If you are at a static non changing distance from a round disc magnet that is axially magnetized and that rotates around it's symmetry axis of polarization then you won't notice a single thing, the field won't change. There are no hairy field lines sticking out of the magnet disc surface that are dragged along as the magnet moves as if they were human hair dragged along the wind, no such thing exists.So if you take a magnetic core like you showed and insert a cylindrical and symmetric part in it and keep it perfectly steady radially but just spin it axially and the spinning material has an almost perfect structural isotropy then the "field lines" won't be altered in any way I think, the field in the core won't "notice" so to speak.
 
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  • #31
cairoliu said:
From reply #13, then after, I assume the cylinder is replaced with an infinite area plate with thickness equal to original height of the solid cylinder, and no more rotation, but linear motion.

My only concern is whether the motion of wire (combined with plate), is affected by the plate in term of induction effect.

By my imagination, the contact area between wire and plate seems not to cut B flux, as the motion may stickily drag the MMF lines if not instant straightening (reconnect to nearest magnetic domains); only the wire upper portion causes flux change?

Following sketch illustrates the combined wire and plate moving towards reader.

If the plate is attached with the C core, and let the wire independently move, is there the same induction effect? View attachment 321629
I think I know what your trying to do. Creating a motor where the rotor is a single magnetic pole with field lines extending outwards or inwards along the whole rotor surface and the stator being the opposite magnetic pole , then you can put a wire in the airgap between the stator and rotor or attach it to rotor surface , pass current through that wire and it will continually be pushed around as it cuts the never ending single direction flux between the stator /rotor.I can say immediately that the first problem is that the magnetic loop has to be long , the longer a magnetic loop is the more lossy it becomes so you will need more energy to create the same strength field, or more permanent magnets, second problem is unless you wish to put slip ring on the periphery of the rotor where there is high angular speed you will have to use the rotor axis as a magnetic field return path, rotor axis are usually made from hardened ferrous steel which is not nearly as great in terms of magnetic permeability as soft magnetic steel used in laminations for transformer cores and electric motors.In theory it works, in practice it's worse in power to size/volume ratio, it's more complicated and it doesn't surpass existing motors/generators in the parameters.
Sorry to say but this is not a new idea , it's just not practically efficient or better therefore it's not used.

One additional note is that such a motor would have only a single turn in the rotor, so a very low resistance path which would be impractical for almost all applications and energy sources.
For more than single turn in the rotor you would need additional slip rings, so 1 turn needs 2 slip rings , 10 turns would require 20!!! slip rings one for each turn start and end.

It's essentially a faraday disc just with different geometry.
Did I got your idea? Is this a good answer ?
 
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  • #32
artis said:
I think I know what your trying to do. Creating a motor where the rotor is a single magnetic pole with field lines extending outwards or inwards along the whole rotor surface and the stator being the opposite magnetic pole , then you can put a wire in the airgap between the stator and rotor or attach it to rotor surface , pass current through that wire and it will continually be pushed around as it cuts the never ending single direction flux between the stator /rotor.I can say immediately that the first problem is that the magnetic loop has to be long , the longer a magnetic loop is the more lossy it becomes so you will need more energy to create the same strength field, or more permanent magnets, second problem is unless you wish to put slip ring on the periphery of the rotor where there is high angular speed you will have to use the rotor axis as a magnetic field return path, rotor axis are usually made from hardened ferrous steel which is not nearly as great in terms of magnetic permeability as soft magnetic steel used in laminations for transformer cores and electric motors.In theory it works, in practice it's worse in power to size/volume ratio, it's more complicated and it doesn't surpass existing motors/generators in the parameters.
Sorry to say but this is not a new idea , it's just not practically efficient or better therefore it's not used.

One additional note is that such a motor would have only a single turn in the rotor, so a very low resistance path which would be impractical for almost all applications and energy sources.
For more than single turn in the rotor you would need additional slip rings, so 1 turn needs 2 slip rings , 10 turns would require 20!!! slip rings one for each turn start and end.

It's essentially a faraday disc just with different geometry.
Did I got your idea? Is this a good answer ?
You really catch my idea.
But how do you think one turn need one pair of slip rings? If you are right, my idea will become junk.
I thick multiple turns can use one pair of slip rings.
 
  • #33
artis said:
It's essentially a faraday disc just with different geometry.
Yes, mine looks like Faraday disc, but I don't use the disc-itself as conductor, but use multiple turns copper wire coil pasted on surface of disc. So the disc should be an good soft magnetic steel which is almost non-conductor.

Generally speaking, if a material is a good electric conductor, it must be a bad magnetic conductor, so the Faraday electric disc is very different with my magnetic disc.

The induction force firstly drive the copper wire, then the disc is passively driven by glue that hold wire & disc together.
 
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  • #34
cairoliu said:
You really catch my idea.
But how do you think one turn need one pair of slip rings? If you are right, my idea will become junk.
I thick multiple turns can use one pair of slip rings.
Think about it, it's simple, if your rotor to stator flux is all in one direction all around the rotor surface then you can't pass wire back and forth, you can only pass wire in one direction and current also in one direction.
If you put two wires next to each other and pass current in opposite direction then one wire will try to turn left while the other right, you will have a perfectly canceling torque and no movement.

Therefore for a design like this you can only pass current in one direction and then use a return path for the current that is OUTSIDE!!! of the flux that you are working with.

So yes you need two slip rings for each loop/turn of such a motor.

It does work in theory and would also work in practice it's just extremely inefficient to do a motor this way.

It has too long magnetic field path and needs alot of slip rings , or the other way is to do it like the faraday disc is done instead of many turns, have just a single turn but then you need huge amperage to get any real torque.
I'm talking kilo amps!

Sorry buddy, but this idea doesn't fly.
 

FAQ: A donut electromagnetic core comprises main section + movable section

What is a donut electromagnetic core?

A donut electromagnetic core is a type of magnetic core that is shaped like a toroid or donut. It is used in various electromagnetic applications, such as inductors and transformers, to confine and guide magnetic fields efficiently within the core material.

What are the main components of a donut electromagnetic core?

The main components of a donut electromagnetic core are the main section and the movable section. The main section is the fixed part of the core, while the movable section can be adjusted or repositioned to alter the magnetic properties or the configuration of the core.

How does the movable section impact the performance of the core?

The movable section allows for adjustments in the magnetic path length and the distribution of the magnetic field within the core. By repositioning the movable section, one can fine-tune the inductance, magnetic flux, and other electromagnetic characteristics, making the core more versatile for different applications.

What are the typical applications of a donut electromagnetic core with a movable section?

Typical applications include adjustable inductors, variable transformers, and tunable magnetic circuits. These components are used in power electronics, radio frequency (RF) circuits, and other areas where precise control of magnetic properties is essential.

What materials are commonly used to construct a donut electromagnetic core?

Common materials include ferrite, laminated silicon steel, and powdered iron. These materials are chosen for their high magnetic permeability and low core losses, which are crucial for efficient electromagnetic performance.

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