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#11 | |
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diyAudio Member
Join Date: Nov 2002
Location: Netherlands
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Quote:
The force a magnetic field applies onto two poles with an air gap in between can be expressed as: F = B^2 x A / (2 x µ_0) Where F in Newton, A in m2 and B in T (or Wb / m2). Taking into account a max saturation flux density of the necessary iron of 1.5 T, the max force you can get is then app. 100N/cm2. This is equivalent to a pneumatic force of 10 bar. Cheers
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#12 | |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Quote:
Can't see anything wrong with the approach, especially for an experimental set up, I'm now thinking along the line of something that could use a coil or permanent magnets. sreten.
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#13 | |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Quote:
I can see this sort of force in attraction. But I don't think we would be dealing with saturated poles. One of the problems seems to be the "springyness" of the repulsion, a geometry is needed that rapidly varies the air gap as you approach the surface to "stiffen" the bearing. I've got an idea that I'll draw up and post later. sreten.
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#14 |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Hi,
I've pondering what could work well as magnetic bearing but a given is that the "stiffness" of an air bearing is not possible. Also thought it would be nice to include a magnetic vertical bearing in the basic idea as well, though knife edges could still be used if a v block is used top and bottom. The basic principle is shown in the diagram, I'm not suggesting this is the best way to do it, just trying to show the idea. The slide consists of two hollow steel tubes energised by two small high power magnets placed each end. (For weight considerations these could be steel tube sections at each end mounted on aluminium supporting hollow tubes) The guide is fairly self evident and a DC field coil could easily replace the ceramic magnet(s) shown. Now as I see it the top is inherently unstable and the slide would simply fly out sideways, to stabilise this the arm is underhung from the slide, the length of the underhang being enough to provide the classic slight increase of tracking of force as the arm lifts from horizontal, for improved tracking. Seems to me it would only work if the bottom slide piece sits at equilibrium very close to the V-groove wall, I'm thinking the \o/ interface would cause this to happen as long as the pole piece field is not too strong. Do you think the \o/ interface would be quite stiff ? The upper |o interface I envisage having quite a gap. (Some mileage in adding a concave section to the pole piece , i.e. an "(o" interface ?) Obviously the whole thing would need to be made overlength so the ends do not affect field strength, theoretically bucking magnets at each would help even the magnetic field. Stiffness in all planes would be pretty good, my only concern would be the vertical resonant frequency, not sure about this. Don't bash me too hard if there is something fundamentally wrong with this, I'd like to know what that problem is. Just seems to me getting rid of the airpump is a great convenience, at the cost I admit of rigidity, but I assume there would be be some noise advantages over an air bearing arm - there must be ? sreten.
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#15 |
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diyAudio Member
Join Date: Feb 2002
Location: Belgium
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Don't think the stray DC fields are a problem on the leads. They might upset the cartridge, but that can be far-far away.
As for damping, making the carrier out of copper should give nice magnetic damping without adding much weight. While supplying the air to the carrier in a conventional Ladegaard may have advantages, the stiffness of the feeding hose will be a problem. I was amazed when I found out how low friction this arm bearing was. Even my phono leads (two 0.1mm Cu twisted pairs) have influence. |
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#16 | |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Quote:
Though I'm having a hard time seeing the induced current flow that would provide some damping. I can see that an aluminium oval placed as shown would provide lateral damping and could be incorporated into the construction. Nice point though ! I wasn't considering it. sreten.
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#17 |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Just realised the aluminium oval will not provide damping in
that position, the induced currents would cancel each other. sreten.
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#18 |
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diyAudio Member
Join Date: Feb 2002
Location: Belgium
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In order to provide damping, the fieldlines have to cross the material at right angles. A eddy current or foucault brake for a rotating axis works by putting a copper disk on the axis, and then have a C-type coil former with the disk running through the gap. Don't know if I'm clear, but the fieldlines would go through the thin disk section, the C-section going over the rim like a disc brake caliper.
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#19 | |
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diyAudio Member
Join Date: Nov 2003
Location: Brighton UK
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Quote:
minimal, but I stand to be corrected on this. I was initially thinking of induced shorted turn damping, but not possible as far as I can see. sreten.
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#20 |
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diyAudio Member
Join Date: Jan 2002
Location: Munich, Bavaria
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sreten,
i would not be happy concerning the hanging architecture, i prefer to have my vertical pivot axis as close to the records surface as possible; warps and pressing bubbles have the fewest effect on effective stylus speed then. Nevertheless i think you should try out if your idea works Ready, steady, go! If you think this doesn't affect sonics. Maybe it's me only who is incompatible to the sonic effects caused by a small magnet or a piece of iron located in close proximity to a signal-conducting wire (or worse: around that wire, add to that list: faintest trace of magnetic attractability in any passive or active component except Xformers). If you have read my last post in the Nagaoka MP-50 thread, you may have wondered why i waste my energy in designing RCA connectors and such. That's why. BTW, i also use a magnetic bearing inside my tonearm's lateral force compensation mechanism but the magnetic circuit is tinytiny and closed (not much stray field) and far apart from the phono leads.
__________________
Greets, Bernhard |
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