Can saturation point be estimated by copper mass?

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The way I understand saturation...you take a given hub motor. Then, as you raise the number of amps you feed it in equal steps...you will get a roughly similar amount of torque added and heat added at each step.

Then...there is a certain point where "saturation" is reached. At that point, adding another step in raising the amps will result in additional torque, but also...not as much torque as the previous steps, and MUCH more heat compared to the previous additional-amp steps.

Is this way off, or fairly close to accurate? And, can that saturation point be estimated by measuring the copper mass of a given motor?
 
My understanding is it is a limitation of the iron, not the copper. As you say, the relationship between current and magnetic flux leaves the linear region (a knee in the curve) and you get a much small increase in flux for a given increase in current.

If you had a superconducting winding with no losses at all, the motor would still magnetically saturate at the same point.

The information out there on the 'net mostly concerns transformers, but the principles are the same :)

BTW you can also saturate the winding if it's inductance is too low and the frequency of the applied voltage too low (impedance then becomes only DC resistance and current is correspondingly very high), but this is a different phenomenon.
 
As I understand it,
Its the relation ship of copper to iron on the active tooth/teeth in the stator, the magnet & back iron.

Once the amperage level creates the maximum ellectro magnetic force the geometry allows, no gains will be had by pumping additional amperage.
If this amperage level is beyond the current carying value of the copper...it is just making heat & wasting energy.
 
If it is the steel in the laminations that gets saturated, can the saturation point in the amount of amps that can be applied be estimated from the diameter and width of the stator?

I notice that the Cromotor and QS 205/50H have stators that are roughly the same size, but the QS catalog claims it has deeper slots, and that accounts for the extra copper mass and heavier weight.

If its not the extra copper, is the extra copper mass in the windings engaging more steel in the laminations?

edit: posted at the same time as Thud, will read and ponder now...
 
There's definitely a way to calculate the saturation point. It's a function of Amp-turns in the windings and the type of iron.
Take the Amps multiplied by the number of turns will be proportional to the magnetic field strength (and torque).
 
spinningmagnets said:
The way I understand saturation...you take a given hub motor. Then, as you raise the number of amps you feed it in equal steps...you will get a roughly similar amount of torque added and heat added at each step.

Then...there is a certain point where "saturation" is reached. At that point, adding another step in raising the amps will result in additional torque, but also...not as much torque as the previous steps, and MUCH more heat compared to the previous additional-amp steps.
I had thought that the saturation described above was due to the permanent magnet flux being exceeded by the stator flux. After reading more since this thread started, I see that the two aren't isolated because the permanent magnets use the stator iron in their flux return path. I'm even more uncertain, now. :?
Jeremy Harris said:
Subject: Basic Motor Questions - Torque V. RPM
Maximum torque is a function of the radius of the rotor (the moment arm, in effect) and the force that the magnets and windings can exert on each other. There is a finite limit to this force, set by the strength of the magnets, the current through the windings and the number of turns in each winding. There's also the ultimate limit of the saturation flux density of the stator core, but that should normally be greater than the flux density from the magnets, at least with present neodymium magnets. As the maximum force is pretty much fixed by the magnet strength and current that the winding will take without overheating, the most effective way to increase torque is to increase the motor diameter.

Jeremy
 
Below is a graph of flux density vs. magnetic field strength. The magnetic field strength is our Ampere-turns (or just amps for a fixed motor configuration). The flux density translates to torque. Most motors will be operating below 1 Tesla.

As you can see the left hand part of the graph is sort of linear until you reach a point where it starts to flatten out. Different types of steel will have different curves.

 
if the cross section of one tooth and the number of tooth are known, as well easy the material, it should be possible to make a quite accurate estimation.

The tooth's cross section is most critical. Material of these motors is always a silicon steels. Most of them have similar saturation flux density, just different hysteresis properties
 
this is a really great thread. i hope it leads to a spread sheet like:
motor ...... saturates at ....... amp turns

if we use amp turns, it would be easy to convert the amp value to all different turn counts. right?

spinningmagnets said:
I notice that the Cromotor and QS 205/50H have stators that are roughly the same size, but the QS catalog claims it has deeper slots, and that accounts for the extra copper mass and heavier weight.

Cromotor V1 = QS 205 50H V1
Cromotor V2 and V3 = QS 205 50H V2
The new QS V3 has a different stator design. It has fewer but larger and deeper teeth, so different kT and kV.
 
Why not put this Saturation data in the motor comparison sheet ? it already has all the motor details in their. Maybe just add a column for material ?

Does the saturation point only have a relation to current or also voltage related?

Eg Crossbreak for the cyclone motor in that thread we were discussing the efficiency at 48v 100 amps vs 72v 68 amps is the same power, but maybe higher efficiency at 72v, is this related to the motor saturating and hence lower current is better ? Or is the saturation point of the motor above 100 amps and not relevant to this?
 
spinningmagnets said:
The way I understand saturation...you take a given hub motor. Then, as you raise the number of amps you feed it in equal steps...you will get a roughly similar amount of torque added and heat added at each step.

Torque goes up linearly with current at first, but heat goes up by the square of current. That makes saturation a pretty useless number, because you should never run a motor anywhere close to saturation.
 
because you should never run a motor anywhere close to saturation

Agreed, but...builders around here will continue to raise the amps until it becomes painfully obvious that they are running way too hot (wasted battery amps). If we can list the max amps per "X" on a given hubmotor, then builders can decide if they want to overheat a smaller hub occasionally, or make the jump to the next size up. Due to "bang per buck", these seem to be the direct drive hubs of interest?

28mm MXUS V2
35mm Leafbike 1500W
45mm MXUS 3000W V2
50mm QS 205/50H V3
 
Rough rule of thumb for the motors above I am working on for the motors above:
120 watts per mm of stator width.

Willing to debate to come up with a better figure for general advice.

What p*sses me off is people keep saying Mxus and Leaf are 92% efficient to noobs - but then in the next sentence declare they are riding it at 4 times the rated power. Can you say 50% efficiency? So they mount fans to remove the heat and assume the motor can now make more kinetic energy. Noob gets infected with the virus. Kill me now.
(Rant over).

Opinions of the 120 watts per mm idea?
 
All motors are capable of saturating at very low wattages.

Wattage is irrelevant - only amp-turns matters...

(Edit: forgot to account for phase resistance limiting maximum current)
 
Samd said:
Rough rule of thumb for the motors above I am working on for the motors above:
120 watts per mm of stator width.

Willing to debate to come up with a better figure for general advice.

What p*sses me off is people keep saying Mxus and Leaf are 92% efficient to noobs - but then in the next sentence declare they are riding it at 4 times the rated power. Can you say 50% efficiency? So they mount fans to remove the heat and assume the motor can now make more kinetic energy. Noob gets infected with the virus. Kill me now.
(Rant over).

Opinions of the 120 watts per mm idea?

watts say nothing. what we want to know are the max PHASE amps for a given turn count or a maximum torque rating.
yes you have right that often the motor opeartes below ist peak efficiency point (when ist laced into too large wheel or at very high speeds), but why should this have someting todo with beeing a noob?
the MXUS is in the Simulator and everyone can look how efficienct it will operate and FWIK if you ride 70-80kmh fast you can achieve easy the peak eff with the right wheel size.
 
PunxOr, the most popular Leafbike motors are the 4T and the 5T, both using a 35mm wide stator. Using amp-turns, how many max amps could these two examples use before saturating?

Lets assume both using 52V (14S), or...would voltage play some role (between 48V to 60V?)
 
No idea! If it could be determined from theory, simulation or measurement for the most common motors it would be a potentially useful addition to known motor data. I.e. an upper limit for peak torque.
 
spinningmagnets said:
because you should never run a motor anywhere close to saturation

Agreed, but...builders around here will continue to raise the amps until it becomes painfully obvious that they are running way too hot (wasted battery amps). If we can list the max amps per "X" on a given hubmotor, then builders can decide if they want to overheat a smaller hub occasionally, or make the jump to the next size up. Due to "bang per buck", these seem to be the direct drive hubs of interest?

28mm MXUS V2
35mm Leafbike 1500W
45mm MXUS 3000W V2
50mm QS 205/50H V3

Those aren't the best "bang per buck" DD hubbies...not even close.

The measure you need to look at is the phase-to-phase resistance, because that tells you the heat generated for a given current. Core losses are small enough to ignore except at high rpm where BEMF forces lower current, so they really only come into play when looking at efficiency at cruise and having no relation to current limits.

So you have heat created in the copper as one part of the equation and is easily calculated. The other is how much heat the motor can dissipate, but since the motors you list have quite similar outer shell dimensions they are very comparable in heat dissipation with the larger motors having a slight edge due to greater width at the perimeter.

Rules of thumb would be useless, because load, terrain, riding style, wheel size, and even length of a typical ride are all critical parts of heat equation. That's before considering motor or bike mods to increase heat dissipation.

Saturation is a useless number for hubmotors, so teach people something useful instead. ie Copper losses (heat generated in the copper) is current squared times phase-to-phase resistance, and copper resistance goes up by about 0.4% per degree C of temperature increase in our operating range. Tie that in with the baseline heat dissipation of an unmodified motor in Justin's testing and you get both sides of the equation.

If you really want to give people something useful to ponder, point out that going from a 26" wheel to a 29" wheel increases heat generated by 24% for the same acceleration, so putting DD hubbies in 29ers should always be discouraged. In fact, geared hubbies should be discouraged for 29ers too, since no manufacturer is installing a different gear reduction for use in the larger wheels. That's small compared to going down from a 26" to a 20" wheel, which decreases heat by over 40%. If you compare results for a 20" wheel to a 29", for the same acceleration over twice as much heat is generated in the motor. That discussion isn't complete without pointing out that changing the winding turn count of the motor will make exactly 0 difference in how much heat is generated.

Note that these differences are actually low, since with greater heat comes higher temperature, and in turn higher resistance, which creates even more heat. If a 20" wheel is too small for your taste, fine, simply use the smallest wheel size you can live with. Just make your decision armed with accurate info. I've seen people debating the weight of tires and rims as if it really matters, but that effect is insignificant compared to the wheel diameter, which is almost never discussed.
 
fechter said:
There's definitely a way to calculate the saturation point. It's a function of Amp-turns in the windings and the type of iron.
Take the Amps multiplied by the number of turns will be proportional to the magnetic field strength (and torque).

Than why all motor manufacturer hide this key specification from the buyer ?
Is there no room for improvement with the iron/silicon steel ?
 
The motors with thinner laminations and/or a thick aluminum stator support cost more, so these might skew the "buck" part of the equation, but...without those upgrades, a motor under consideration would have to be larger to be in the same power/heat category. Maybe bang for your buck was the wrong phrase, but those four are the ones I am interested in right now.
 
Punx0r said:
If it could be determined from theory, simulation or measurement for the most common motors it would be a potentially useful addition to known motor data. I.e. an upper limit for peak torque.
Unfortunately we dont know the material of those motors. Sure we could suppose it to be 3%-FeSi which seems to be most common. No idea if this is really true for most motors

John in CR said:
I've seen people debating the weight of tires and rims as if it really matters, but that effect is insignificant compared to the wheel diameter, which is almost never discussed.
+1

leafmotor dyno test https://endless-sphere.com/forums/viewtopic.php?f=30&t=66489&start=675#p1111391
liveforphysics said:
I dyno'd it today. Will hopefully have time to edit the videos together tomorrow. It made a peak of 4.9hp output when feeding it ~8kW input. It's pretty efficiency from 500w to 2000w, falls off pretty sharply in efficiency above ~3500w input.
That was measured around 40mph with a 26" tire from what i can see in the video. So i assume 510rpm. T=9.55*P/n=9.55*3500/510= ~65 Nm. That 4.9hp were at lower speed i assume.
kV for the 4T is 12.5, which makes kT 0.764. Phase amps = 65Nm/0.764= 85A or 340 Amp-turns
this is ~10Amp-turns per mm of lamination
This is the point where the line starts to be non-linear, the point where good efficiency ends. it seems like saturation start at round about double that figure. But not double that torque figure, of course (as current and torque are no more linear related here). Saturation torque seems to look like maybe somewhere 20% above that 65Nm from here, say 80 Nm. That is ~2.3 Nm per mm of lamination
this would be my very rough rule of thumb :D

absolute maximum torque
65 Nm__28mm MXUS V2
80 Nm__35mm Leafbike 1500W
104 Nm_45mm MXUS 3000W V2
115 Nm_50mm QS 205/50H V3

max reasonable phase-amp-turns
280 At__28mm MXUS V2
350 At__35mm Leafbike 1500W
450 At_45mm MXUS 3000W V2
500 At_50mm QS 205/50H V3
 
John in CR said:
Those aren't the best "bang per buck" DD hubbies...not even close.
not even close?
man, what motor would you take instead of the ones he listed?
this is a serious question so i want a serious answer, but i think you have NO :p


John in CR said:
Saturation is a useless number for hubmotors, so teach people something useful instead. ie Copper losses (heat generated in the copper) is current squared times phase-to-phase resistance, and copper resistance goes up by about 0.4% per degree C of temperature increase in our operating range. Tie that in with the baseline heat dissipation of an unmodified motor in Justin's testing and you get both sides of the equation.

i believe most people looking into this thread already know about copper losses, wheel size and all that important things, but they want to know MORE.
knowing the point where the correlation between phase amps and produced torque ends to be linear would be useful to know.
we could set the controller to operate below this value (in boost mode for instance on adaptto controllers) to not "waste" more amps than necessary.

there is a great thread about saturation from Justin:

https://endless-sphere.com/forums/viewtopic.php?f=2&t=14494&start=25#p218312

It looks like saturation or 2nd order effects start to happen at around 70 Newton-Meters, exactly the same torque where the BMC hub started to show this behaviour. In the case of the 9C hub, the motor constant K decreases by about 40% after this point, while the BMC motor it decreased just a little more, by 46%.

this was with a 28mm 9C motor and trapezoidal controller. FOC should improve things.
the Leaf, MXUS and Cromotor have similar stator design (same pole count and same air gap diameter) so if we extrapolate from this test the numbers we get should not be far off.

@ crossbreak

the QS V3 has a different stator design as the other motors, so i believe it has a different saturation point.
 
madin88 said:

John in CR said:
Saturation is a useless number for hubmotors, so teach people something useful instead. ie Copper losses (heat generated in the copper) is current squared times phase-to-phase resistance, and copper resistance goes up by about 0.4% per degree C of temperature increase in our operating range. Tie that in with the baseline heat dissipation of an unmodified motor in Justin's testing and you get both sides of the equation.

i believe most people looking into this thread already know about copper losses, wheel size and all that important things, but they want to know MORE.
knowing the point where the correlation between phase amps and produced torque ends to be linear would be useful to know.
we could set the controller to operate below this value (in boost mode for instance on adaptto controllers) to not "waste" more amps than necessary.

there is a great thread about saturation from Justin:

https://endless-sphere.com/forums/viewtopic.php?f=2&t=14494&start=25#p218312

It looks like saturation or 2nd order effects start to happen at around 70 Newton-Meters, exactly the same torque where the BMC hub started to show this behaviour. In the case of the 9C hub, the motor constant K decreases by about 40% after this point, while the BMC motor it decreased just a little more, by 46%.
You left out the more pertinent information from Justin's post:
justin_le said:
So there you have it folks! One thing that became clear to me in these tests though, was that even if there wasn't any saturation/demagnetization effects going on, just the I^2R consequence of pushing the motors this far means we are in a domain that is totally outside of any useful operating zone. The windings get hot, FAST, and that has huge effect on the motor performance. I had the current going through for just 10-15 seconds in order to get a peak torque reading, then would have to put the motor outside in the subZero weather and wait a good amount of time for it to cool off.
 
think people who read this kind of thread are aware of this

zener said:
fechter said:
There's definitely a way to calculate the saturation point. It's a function of Amp-turns in the windings and the type of iron.
Take the Amps multiplied by the number of turns will be proportional to the magnetic field strength (and torque).

Than why all motor manufacturer hide this key specification from the buyer ?
Is there no room for improvement with the iron/silicon steel ?

It's that simple, it's not a key specification:
because you should never run a motor anywhere close to saturation
There are very rare situations you would really think about doing something that stupid. Emergency brakes for example.
 
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