Left Hand Rule Applied to a Winding

In summary, the direction of force in a DC motor is determined by the current in the coils and the direction of the magnetic field.
  • #1
jake jot
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17
TL;DR Summary
If the winding has equal current and directions in each side. They cancel out. So how do you determine the principal force directions?
All illustrations of direction of force in motor has this form.

motor inductor with left hand rule.JPG


For the following specifically the rotor. I'm confused where is the direction of force. It uses winding and there seems to be current and force in every side of the winding (applying left hand rule). So where does the principal force really point? I've been figuring this out for days. So hope someone can give aid.

where is motor force.jpg


This is video of the motor running.

https://d2y5sgsy8bbmb8.cloudfront.n...rm-Generic-480p-16-9-1409173089793-rpcbe5.mp4

It's from amazon science kit. https://www.amazon.com/gp/product/B073GXWQMV/?tag=pfamazon01-20
 
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  • #2
jake jot said:
If the winding has equal current and directions in each side. They cancel out. So how do you determine the principal force directions?
Is the current in CD really running in the same direction as in AB ?
 
  • #3
BvU said:
Is the current in CD really running in the same direction as in AB ?

Here is zoom of the center.

rotor left hand zoom__.jpg


Where is CD and AB?
 

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  • #4
DCmotor.png

BC and AD rotate in plane of field, so cross product (force ) is always perpendicular to that plane, ie axial and produces no rotation.AB and CD : currents may be equal in magnitude and direction, but as vectors they are opposite in sense. Field stays the same, current is opposite, so force must be opposite.

If in doubt, I draw in a few field lines then look at them as Faraday describes.
 
  • #5
Merlin3189 said:
View attachment 273403
BC and AD rotate in plane of field, so cross product (force ) is always perpendicular to that plane, ie axial and produces no rotation.AB and CD : currents may be equal in magnitude and direction, but as vectors they are opposite in sense. Field stays the same, current is opposite, so force must be opposite.

If in doubt, I draw in a few field lines then look at them as Faraday describes.

no problem about it, but how do you apply it to the following where the winding has 4 sides unlike the above?

rotor left hand zoom__.jpg
 

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  • #6
Merlin3189 said:
View attachment 273403
BC and AD rotate in plane of field, so cross product (force ) is always perpendicular to that plane, ie axial and produces no rotation.AB and CD : currents may be equal in magnitude and direction, but as vectors they are opposite in sense. Field stays the same, current is opposite, so force must be opposite.

If in doubt, I draw in a few field lines then look at them as Faraday describes.

I understand the above. No problem with this.

normal rotor directions.JPG


DC Motor, How it works? - YouTube

It's obvious. But in the following, the conductor is in form of windings at all sides, and they seem to cancel so where is the EMF force directions at the right and left?

where is motor force.jpg


zoom

rotor left hand zoom__.jpg
 

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  • #7
Again, the (now) vertical wires give axial forces, so irrelevant.
The now horizontal wires have up and down forces, top up and bottom down. But, that's because they are at the changeover position, when, in fact, there should be no current flowing.
If you imagine the rotor turned 90 deg ACW, so that the coils are top and bottom, and keep the direction of the current as shown here, then the wires on the LHS get an upward force and those on the RHS a downward force, giving a CW torque. If the current is in the same sense in both coils, that applies to all the wires in both coils.

You could of course simply imagine the rotor as an electromagnet. As shown in the pic, viewed from the right, the current is CW, so it looks like a S pole and is attracted to the N pole, which is where it is. From the left current is ACW and looks like an N pole being attracted to the S pole where it is. No reason to turn.

When the rotor is turned 90 deg ACW as above, the S pole is at the top and is attracted to the N pole on the right. Similarly the N pole of the rotor is now at the bottom and attracted to the LH S pole. A CW torque, just as produced by the, up on the left, down on the right, forces above.

TBH I've no idea how to analyse this sort of rotor, with an iron cored rotor and shaped field poles. You probably need and electrical engineer for that. (I expect Jim Hardy would have known). I just knew the basic principle of the motor with wires in a uniform field, as taught in Physics textbooks. After that I just put my faith in Eric Laithwaite's principle that the more iron and copper, the more efficient the motor! It's actually always puzzled me that the wires in most motors don't seem to be in any magnetic field: nearly all the flux seems to go through the iron, bypassing the wires. The magnetic flux "links" the coils and I've seen analysis of transformers based on that idea, but not motors. It's probably my bad understanding of field and flux.
 
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  • #8
Merlin3189 said:
Again, the (now) vertical wires give axial forces, so irrelevant.
The now horizontal wires have up and down forces, top up and bottom down. But, that's because they are at the changeover position, when, in fact, there should be no current flowing.
If you imagine the rotor turned 90 deg ACW, so that the coils are top and bottom, and keep the direction of the current as shown here, then the wires on the LHS get an upward force and those on the RHS a downward force, giving a CW torque. If the current is in the same sense in both coils, that applies to all the wires in both coils.

You could of course simply imagine the rotor as an electromagnet. As shown in the pic, viewed from the right, the current is CW, so it looks like a S pole and is attracted to the N pole, which is where it is. From the left current is ACW and looks like an N pole being attracted to the S pole where it is. No reason to turn.

When the rotor is turned 90 deg ACW as above, the S pole is at the top and is attracted to the N pole on the right. Similarly the N pole of the rotor is now at the bottom and attracted to the LH S pole. A CW torque, just as produced by the, up on the left, down on the right, forces above.

TBH I've no idea how to analyse this sort of rotor, with an iron cored rotor and shaped field poles. You probably need and electrical engineer for that. (I expect Jim Hardy would have known). I just knew the basic principle of the motor with wires in a uniform field, as taught in Physics textbooks. After that I just put my faith in Eric Laithwaite's principle that the more iron and copper, the more efficient the motor! It's actually always puzzled me that the wires in most motors don't seem to be in any magnetic field: nearly all the flux seems to go through the iron, bypassing the wires. The magnetic flux "links" the coils and I've seen analysis of transformers based on that idea, but not motors. It's probably my bad understanding of field and flux.

In the amazon motor above. Do you think the entire curved blue and Red metal body is the magnet or is the magnet only at the top. I gave the product to a kid and it isn't with me now. But I'll borrow from the kid again later this week.
 
  • #9
Yes. The iron shell guides the flux from the magnet at the top and produces a horizontal field around the rotor.
Your first diagrams used two magnets one on each side of the rotor. The field can be strengthened by joining the outside faces with iron, completing the manetic "circuit".
Early motors sometimes used horseshoe magnets to have the same effect.
This idea is very economical because you need only one simple magnet, then the cheap shaped piece of iron brings the field to where you want it.
 
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  • #10
Hello Jake,

No need to re-post the same image five times. I do wonder who drew the blue current lines on it, though. If they are correct, the motor is in a stable stalled position. The current should be reversed to create a north pole on the righthand side of the coil. Like @Merlin3189 , I suspect the brushes are at or near the point of reversing the current direction.

Did you notice Amazon makes a mess of the pictures by attaching the red iron arc to the south permanent magnet pole in half of them ?
 
  • #11
BvU said:
Hello Jake,

No need to re-post the same image five times. I do wonder who drew the blue current lines on it, though. If they are correct, the motor is in a stable stalled position. The current should be reversed to create a north pole on the righthand side of the coil. Like @Merlin3189 , I suspect the brushes are at or near the point of reversing the current direction.

Did you notice Amazon makes a mess of the pictures by attaching the red iron arc to the south permanent magnet pole in half of them ?

I drew the blue current label. After i drew it. I got stuck thinking how it could move. So the secret lies in reversing the current. Thanks for the ideas.
 
  • #12
jake jot said:
secret lies in reversing the current
Yes. Basically you force the poles of permanent magnet and electromagnet to be equal at the moment shown in your picture, so they repel each other and the rotor keeps turning. The brushes take care of that.
 
  • #13
BvU said:
Yes. Basically you force the poles of permanent magnet and electromagnet to be equal at the moment shown in your picture, so they repel each other and the rotor keeps turning. The brushes take care of that.

Why is that in most motor teachings. They use the lorenz force in emphasizing it is how motor rotates and not concept of north and south? Which has more contribution to the rotation? See for example

20201130_230206.jpg
 
  • #14
jake jot said:
Which has more contribution to the rotation?
It is one and the same thing. The Lorentz force is the much more fundamental concept.
 
  • #15
BvU said:
It is one and the same thing. The Lorentz force is the much more fundamental concept.

But notice in the following rotor that the north and south pole depicted in the right and left side label is 90 degrees off the lorentz force which comes out of the conductor (remember all the up and down arrows in the conductors depicting the directions of the lorentz force?

20201201_014551.jpg
 
  • #16
What are we looking at ? Current in top horizontal part of the coil is coming towards us, lower away from us. Where is the permanent magnet field and which way is it pointing ?
 
  • #17
BvU said:
What are we looking at ? Current in top horizontal part of the coil is coming towards us, lower away from us. Where is the permanent magnet field and which way is it pointing ?

Even without the stator or permanent magnet. The rotor has north and south that is perpendicular to the wires. It is the wires which is source of direction in the left hand rule and the lorenz arrows come from wires. This means north, south is not identical to the force direction. Right? Let's say it doesn't produce any force directions. Can the rotor rotate if there is present of stator or permanent magnet around it?
 
  • #18
jake jot said:
Even without the stator or permanent magnet. The rotor has north and south that is perpendicular to the wires. It is the wires which is source of direction in the left hand rule and the lorenz arrows come from wires. This means north, south is not identical to the force direction. Right? Let's say it doesn't produce any force directions. Can the rotor rotate if there is present of stator or permanent magnet around it?

Here is to illustrate the point. Some demo in youtube only uses north, south and not the direction of force. I think you are saying it's two side of a coin. But let's say we won't use the "direction of force" explanation. Can one explain completely the action of the north, south, commutator in the rotor with respect to the permanent magnet? So the reason the rotor rotates is because the magnetic pole is attracted to the opposite side and this rotates the rotor? But the magnets kinda too far, is the north/south style of explanation able to stand alone (by suppressing the more powerful lorentz force explanation (i drew the violet lorentz force directions in the following)?

20201201_105659.jpg


How DC Motors Work - YouTube
 
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  • #19
jake jot said:
I think you are saying
Correct, that is what I am saying.
We can go round in circles infinitely, but by now I don't think I still understand what your core question is.
jake jot said:
is the north/south style of explanation able to stand alone
Yes, because it is the same thing
 
  • #20
BvU said:
Correct, that is what I am saying.
We can go round in circles infinitely, but by now I don't think I still understand what your core question is.
Yes, because it is the same thing

Is it like:

General relativity = lorentz force and left hand rule
Newtonian gravity = Rotor north south

Meaning one is a better explanation. Or like

Space = lorentz force
Time = North and South

Spacetime meaning they occur at the same time?

My core question is. Does a bar magnet necessary have current and lorentz force if it is made to rotate in a permanent magnet?

Imagine you are in the ISS space station or just space that has weightlessness. You put a permanent magnet but instead of using a rotor with commutator. You use a theoretical bar magnet where the polarity can change every half revolution just like having a commutator. This can make the rotor turn indefinitely. But without any lorentz force or left hand rule in the theoretical pole changing magnet rotor (just for sake of illustration).
 
  • #21
Don't get carried away in space and time. Weightlessness does not come into this anywhere. Stay with feet on ground.

jake jot said:
Does a bar magnet necessary have current and lorentz force if it is made to rotate in a permanent magnet?
Magnets tend to align.
 
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  • #22
BvU said:
Don't get carried away in space and time. Weightlessness does not come into this anywhere. Stay with feet on ground.

Magnets tend to align.

Is the velocity to keep it align the same velocity as the lorentz force?

This is the only way they can be equivalent. Any equation or something to equate either has the same value?
 
  • #23
jake jot said:
the same velocity as the lorentz force?
I can't think you meant to say it that way. It doesn't make sense to equate different quantities.
 
  • #24
sophiecentaur said:
I can't think you meant to say it that way. It doesn't make sense to equate different quantities.

20201201_105659.jpg


Let us focus the above (let me share it the last time to aid in the discussion).

The velocity of the lorentz force is the speed of light.
I wasn't referring to it. Instead, depending on the value of the lorentz force by way of the current strength, it can make the rotor run faster.

Yet someone explained how the magnet tending to align themselves can stand alone as explanation. But something is not right. First since they are the rotor is solid unit, the alignment of the (electro)magnet is related to the lorentz force acting on the wire. I was asking whether without this lorentz force acting on the wire and pushing the rotor making it rotate, whether the magnet aligning can stand alone as explanation. Someone said yes. So can you share a design where only the magnet is present without any lorentz force acting? This is the only way to prove the aligning alone of the magnets can make rotor rotate as it is. This can happen if there is no current from batteries. But is it not a magnet has some current or electrons align inside. So kindly illustrate some sort of setup where the lorentz force is missing and only the aligning of the magnets make the rotor turn. Thank you.
 
  • #25
jake jot said:
Yet someone explained how the magnet tending to align themselves can stand alone as explanation.
That sort of explanation seems to be in a style of several hundred years ago. To get anywhere with that approach, you would first need to have a good understanding of ferromagnetism at a molecular level and then apply it to a large number of molecules in a piece of steel.
If the time (hardly 'speed') that a (solid) permanent magnet takes to react is not what you might expect from a simple free-space situation then perhaps it might be because of the very finite delay involved in propagation of EM 'effects' through a solid. It would relate to the speed of sound through the material, which is how quickly the molecules interact and re-arrange themselves.
I really don't understand the context of the OP. It seems to be trying to find some sort of contradiction between two approaches to EM. If an alternative to the Lorenz force appears to disagree with it then I suggest that the Lorenz force wins and the other approach needs to be re-examined / explained.

This particularly applies in a thread that is full of lower-school diagrams of electric motors. If those diagrams don't seem to fit in with theory then perhaps they are best ignored (at least one of them seem to be wrongly drawn). I'd recommend starting all over again with some basic EM theory or, if the maths is too hard, come to terms with the simple school-level ideas like the LH motor rule and try to apply them to motors more complex than simple loops. That's in the realms of Engineering and Technology and not basic Physics.
 
  • #26
sophiecentaur said:
That sort of explanation seems to be in a style of several hundred years ago. To get anywhere with that approach, you would first need to have a good understanding of ferromagnetism at a molecular level and then apply it to a large number of molecules in a piece of steel.
If the time (hardly 'speed') that a (solid) permanent magnet takes to react is not what you might expect from a simple free-space situation then perhaps it might be because of the very finite delay involved in propagation of EM 'effects' through a solid. It would relate to the speed of sound through the material, which is how quickly the molecules interact and re-arrange themselves.
I really don't understand the context of the OP. It seems to be trying to find some sort of contradiction between two approaches to EM. If an alternative to the Lorenz force appears to disagree with it then I suggest that the Lorenz force wins and the other approach needs to be re-examined / explained.

You mentioned "two approaches to EM". I thought they occurred at the same time. One is the Lorentz force that makes the whole rotor rotate. The second is the tendency for the magnets to align N/S and S/N. Why do you say they are two approaches. In a motor. How much is the contribution of the Lorentz Force and the contribution of the tendency of the magnets to be aligned, both of which take part in making the rotor rotates? Maybe 50% 50% each? If anyone else understood me. Kindly help frame my statements. Or correct my misconception. Thanks.

This particularly applies in a thread that is full of lower-school diagrams of electric motors. If those diagrams don't seem to fit in with theory then perhaps they are best ignored (at least one of them seem to be wrongly drawn). I'd recommend starting all over again with some basic EM theory or, if the maths is too hard, come to terms with the simple school-level ideas like the LH motor rule and try to apply them to motors more complex than simple loops. That's in the realms of Engineering and Technology and not basic Physics.
 
  • #27
jake jot said:
You mentioned "two approaches to EM". I thought they occurred at the same time. One is the Lorentz force that makes the whole rotor rotate. The second is the tendency for the magnets to align N/S and S/N. Why do you say they are two approaches. In a motor. How much is the contribution of the Lorentz Force and the contribution of the tendency of the magnets to be aligned, both of which take part in making the rotor rotates? Maybe 50% 50% each? If anyone else understood me. Kindly help frame my statements. Or correct my misconception. Thanks.

To rephrase the above. There are two forces involved in making a rotor rotates, the Lorentz force from the current in the conductor, and the tendency of magnets to align, right?

Or is only one involved? But it appears to be two. Is it not?
 
  • #28
jake jot said:
The second is the tendency for the magnets to align N/S and S/N.
That is not a modern theory. It is just an observation. Lorenz is a theory which gives the magnitude and direction of the force due to a current and a magnetic field. If the "tendency" doesn't give a numerical answer then it is of no real use; it may be used as a rule of thumb when you first look at a motor design. But, in the case of anything but a simple motor (one with multiple coils at different angles around the axis) it tells you very little. You would need to break it down into individual planes of the winding. That can be done using the Lorenz force but how would your 'tendency' help with finding the torque due to all the windings?

Your "tendency" statement is a great simplification of what Lorenz tells you quantitatively.
 
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  • #29
Is there some quantitative law which tells you the torque on a bar magnet in a magnetic field?
Surely it would be possible to measure the "tendancy" of a magnet to align with a field. Then it would be quantitative.
The problem for me would be, how to characterise the magnet. It might depend on shape and size as well as magnetic strength(?)
 
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  • #30
Merlin3189 said:
The problem for me would be, how to characterise the magnet.
Exactly. A conventional bar magnet will have a strange distribution in its internal field. I imagine that modern magnets, made of fancy alloys, could be much more uniform so it might be easier to characterise. I don't think the OP is aware of the practicality of trying to approach magnetism via bar magnets. Wound electromagnets are probably difficult enough - considering that they will have magnetic cores.
 
  • #31
I'm not feeling confident in this, particularly since I don't understand ferromagnetism. So perhaps others might correct me.

Jake seems to be thinking there are two different ways of getting a force between magnets, depending on whether they are made of coils of wire, or are permanent magnets.

jake jot said:
...There are two forces involved in making a rotor rotates, the Lorentz force from the current in the conductor, and the tendency of magnets to align, right?

Or is only one involved? But it appears to be two. Is it not?

I would say no - that whatever combination you have, ultimately the forces arise between charges and follow Lorenz's law.
That in permanent magnets, the permanent field comes from permanent movement of charges either within atoms, or domains (whatever they may be.) (That I think gets modeled as an equivalent surface current, much like its being surrounded by a solenoid.)

So

There is only one force - the Lorenz force.
There may be different ways of modelling and calculating the actual forces in different configurations, but they must a priori give the same result as would be given by applying the Lorenz relation, were that mathematically feasible.
 
  • #32
sophiecentaur said:
That is not a modern theory. It is just an observation. Lorenz is a theory which gives the magnitude and direction of the force due to a current and a magnetic field. If the "tendency" doesn't give a numerical answer then it is of no real use; it may be used as a rule of thumb when you first look at a motor design. But, in the case of anything but a simple motor (one with multiple coils at different angles around the axis) it tells you very little. You would need to break it down into individual planes of the winding. That can be done using the Lorenz force but how would your 'tendency' help with finding the torque due to all the windings?

Your "tendency" statement is a great simplification of what Lorenz tells you quantitatively.

Yes you hit the head on the nail.

Can you share an actual circuit where "one with multiple coils at different angles around the axis" that can't be explained by tendency to align? I just want to see the picture of what it could look like.
 
  • #33
jake jot said:
Can you share an actual circuit where "one with multiple coils at different angles around the axis" that can't be explained by tendency to align? I just want to see the picture of what it could look like.
I can't think of any good reason to try that and I couldn't even begin to work out how I could add up the different 'tendencies' of each of the coils to point in a direction. You can't add up 'tendencies' because you haven't quantified them (unless you have some pretty revolutionary Maths) so afaics, it's a waste of time - except for the most elementary of elementary treatments of the Motor Effect.

The point of Science is to build models that represent physical reality and which will allow you to predict and explain things interns of actual values. That always involves some Maths. The Lorenz force can be calculated in principle for any situation and it can (could) tell you the torque on any motor design that you can specify.
 
  • #34
sophiecentaur said:
I can't think of any good reason to try that and I couldn't even begin to work out how I could add up the different 'tendencies' of each of the coils to point in a direction. You can't add up 'tendencies' because you haven't quantified them (unless you have some pretty revolutionary Maths) so afaics, it's a waste of time - except for the most elementary of elementary treatments of the Motor Effect.

The point of Science is to build models that represent physical reality and which will allow you to predict and explain things interns of actual values. That always involves some Maths. The Lorenz force can be calculated in principle for any situation and it can (could) tell you the torque on any motor design that you can specify.

Yes I believed you. And I've looking for different motor designs at google images to see example of "one with multiple coils at different angles around the axis". Are you talking of DC motors or induction AC motors? An example is this:

many motors.JPG


What kind of motors should I look for that satisfy "one with multiple coils at different angles around the axis". Can someone share? Merlin3189? Thanks.
 
  • #35
jake jot said:
What kind of motors should I look for that satisfy "one with multiple coils at different angles around the axis".

Those images are examples. The windings are not all in one plane. Their planes are all at different angles and the axis of rotation doesn't pass through the planes. I can't imagine how that could be re-drawn with equivalent bar magnets in their place.
 
<h2>1. What is the left hand rule applied to a winding?</h2><p>The left hand rule applied to a winding is a rule used to determine the direction of the magnetic field in a solenoid or coil. It states that if the left hand is held with the thumb pointing in the direction of the current flow, the curled fingers will point in the direction of the magnetic field.</p><h2>2. Why is the left hand rule used in windings?</h2><p>The left hand rule is used in windings because it helps to determine the direction of the magnetic field, which is important in understanding how a solenoid or coil will interact with other magnetic fields.</p><h2>3. How is the left hand rule applied to a winding?</h2><p>To apply the left hand rule to a winding, hold the left hand with the thumb pointing in the direction of the current flow in the winding. The curled fingers will then point in the direction of the magnetic field created by the winding.</p><h2>4. What is the significance of the left hand rule in electromagnetism?</h2><p>The left hand rule is significant in electromagnetism because it helps to determine the direction of the magnetic field, which is a key factor in understanding the behavior of electromagnets and other devices that use magnetic fields.</p><h2>5. Are there any variations of the left hand rule for different types of windings?</h2><p>Yes, there are variations of the left hand rule for different types of windings. For example, the left hand rule for a single loop of wire is slightly different than the rule for a solenoid or coil. It is important to use the correct version of the left hand rule for the specific type of winding being analyzed.</p>

1. What is the left hand rule applied to a winding?

The left hand rule applied to a winding is a rule used to determine the direction of the magnetic field in a solenoid or coil. It states that if the left hand is held with the thumb pointing in the direction of the current flow, the curled fingers will point in the direction of the magnetic field.

2. Why is the left hand rule used in windings?

The left hand rule is used in windings because it helps to determine the direction of the magnetic field, which is important in understanding how a solenoid or coil will interact with other magnetic fields.

3. How is the left hand rule applied to a winding?

To apply the left hand rule to a winding, hold the left hand with the thumb pointing in the direction of the current flow in the winding. The curled fingers will then point in the direction of the magnetic field created by the winding.

4. What is the significance of the left hand rule in electromagnetism?

The left hand rule is significant in electromagnetism because it helps to determine the direction of the magnetic field, which is a key factor in understanding the behavior of electromagnets and other devices that use magnetic fields.

5. Are there any variations of the left hand rule for different types of windings?

Yes, there are variations of the left hand rule for different types of windings. For example, the left hand rule for a single loop of wire is slightly different than the rule for a solenoid or coil. It is important to use the correct version of the left hand rule for the specific type of winding being analyzed.

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