Overunity.com Archives is Temporarily on Read Mode Only!



Free Energy will change the World - Free Energy will stop Climate Change - Free Energy will give us hope
and we will not surrender until free energy will be enabled all over the world, to power planes, cars, ships and trains.
Free energy will help the poor to become independent of needing expensive fuels.
So all in all Free energy will bring far more peace to the world than any other invention has already brought to the world.
Those beautiful words were written by Stefan Hartmann/Owner/Admin at overunity.com
Unfortunately now, Stefan Hartmann is very ill and He needs our help
Stefan wanted that I have all these massive data to get it back online
even being as ill as Stefan is, he transferred all databases and folders
that without his help, this Forum Archives would have never been published here
so, please, as the Webmaster and Creator of this Forum, I am asking that you help him
by making a donation on the Paypal Button above
Thanks to ALL for your help!!


Laminated Cores - Any difference in Being Parallel or Perpendicular?

Started by rukiddingme, December 01, 2010, 07:47:54 PM

Previous topic - Next topic

0 Members and 1 Guest are viewing this topic.

rukiddingme

I am wondering if there is any difference in the orientation of the laminations of a core of an electromagnet. If I were to make a "C" shaped core, can I make the laminations parallel to the flat of the "C", as well as perpendicular to the flat of the "C"? Is there a benefit to one over the other orientation?

TinselKoala

Yes, there is a difference.
Whenever you have a conductor moving across mag field lines, there is a current induced in the conductor. In a transformer, you have varying field line densities moving across the conductive material of the core, back and forth as the AC in the primary switches back and forth, which is the same thing--relative motion of field lines (or densities) and conductors. If you are moving a flat plate or a chunk of metal at 90 degrees to the field lines, or vice versa, there will be "eddy currents" induced in the metal that circle around the field lines in closed loops. The resistance of the metal causes these eddy currents to dissipate power in the metal---heating it up, and also these eddy currents make their own fields that oppose the relative motion of the lines and conductor.
So the laminations are oriented as to interrupt the eddy currents and reduce power losses to core heating. If you can imagine the direction of the field lines, the laminations should be parallel to them, because the eddy currents will try to be in circles around the field lines, and thus will encounter a stack of separate, insulated (by varnish or oxide coating) plates instead of a conductive plane to swirl around in freely.

If you are making a DC electromagnet, you may not need laminations at all, but all magnets are most effective if your design provides a complete, high-permeability "circuit" for the field lines, just like an electric circuit. This is the reason for "horseshoe" magnets or magnets that have pole pieces close together: to make a tight magnetic circuit so as to concentrate the field lines where they can be most useful, rather than spreading out into space.

I laugh at Bedini's "monopole" designs, and all other designs that only use one end of the magnet, letting the other end drag past metal bits or just spread out into space.

Oops...sorry, /rant.

rukiddingme

Thanks for the reply.

This coil will be an AC coil.

I'm not clear enough to figure out which is better, the parallel or the perpendicular.

gyulasun

Hi,

I edited a picture taken randomly from the web how the laminations are oriented in a transformer, see the attached picture. In Figure 1 I show only 3 laminations, just for clarity but there are many more of them next to each other of course.  Then I cut the core and rotated it to be about like your would-be electromagnet core, see Figure 2. I hope it shows now how your laminations should be in the electromagnet.
The magnetic flux should be guided in thin cross-sectional area: the thinner the lamination the lower the loss by eddy currents. So here comes as TinselKoala explained:
"If you can imagine the direction of the field lines, the laminations should be parallel to them, because the eddy currents will try to be in circles around the field lines, and thus will encounter a stack of separate, insulated (by varnish or oxide coating) plates instead of a conductive plane to swirl around in freely."

In the picture the dashed lines show the flux and the laminations are parallel with the flux lines. I assume your near C shaped electromagnet core will have a nearly closed flux path when the yoke part (that surely will have an I shape area) approaches the ends of the C core.

Gyula

Quote from: rukiddingme on December 01, 2010, 10:19:22 PM

I'm not clear enough to figure out which is better, the parallel or the perpendicular.

TinselKoala

Yup, thanks gyulasun, the drawing explains it better than words. So, as I see it, in both the core design from rukiddingme (coil wound around the core, right?) and in gyulasun's image, the long axis of the cores go along the direction of the field lines so the eddys will be in the short directions...but in both designs, as far as I can tell, the two short directions are both the same as far as experiencing eddys. So it becomes a matter of ease of construction. In the square design, it's easier to stamp out flat square outlines like picture frames, than it is to make concentric nesting squares of ribbon (although some transformers are indeed made this way, by wrapping steel ribbons into core shapes). For rukiddingme's design it might be easier to cut the lengths of uniform ribbon, stack them, and bend them in the "flat" direction into the core shape, rather than stamping out a bunch of c-shaped plates and stacking them flatwise. But from the eddy loss perspective, my first guess is that either way is the same.