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#11 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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I checked the Kepco ATE 500 Watt power supply xfmr lams, and they are indeed M6, so this is premium long E stuff for winding OTs. (checked using a variac and a current probe to scope)
For those who might wish to consider this route (instead of using powdered iron!) to getting a premo core (enough for making 2 xfmrs with square winding cores), here are the core dimensions: Overall: 6 inch x 4.5 in. x 2.8 in. thick stack tongue: 1.5 in. x 2.8 in. thick stack winding windows: 4.5 in. x .75 in. Also, I checked on a Kepco ATE 250 Watt power supply and it has the exact same xfmr. but with 1/2 the stack thickness, 1.4 inch. This is just right for making 1 OT with a square winding core. Using the 1.4 inch stack, 250 W core, this will give about 250/3 = 80 Watts at 20 Hz bottom (flux up to saturation), 250/2 = 125 W for guitar amp rating at 30 Hz (Hammond rating too), and for a true high fi rating at 7500 gauss at 20 Hz, this would give 40 Watts audio power. These are all Push Pull amplifier ratings. For SE you will have to put a spacer in the lamination E to I gap. This will typically reduce audio power ratings by about 1/4 from P-P rating. Don
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Ohms Law V = I R |
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#12 | |
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diyAudio Member
Join Date: Apr 2005
Location: Naches,WA
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Don, come now.
Quote:
If it works, it will have been more than worth it. If not, the knowledge I gained will have been just worth it. From my viewpoint its a win-win. Casey
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Experience is a wonderful thing. It enables you to recognize a mistake when you make it again. |
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#13 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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Wow! I hadn't thought of all those fun benefits. Now you've got me excited. Could you send a truck load of the stuff over so I can fill up our sand box with it?
When I get tired of playing in it (and I can use a magnet to clean up), the cats can use it. Maybe can use a magnetic separator and sell it as cat litter. The possibilities are endless! Could put it on the snow in winter for traction, then pick it up again with a magnet in the Spring. How about as an additive to radiator fluid, just put a magnet near any leak and it will automatically plug it up. Think of the military uses! and they pay big money. Put it on a road in a magnetized state. Well, just think of what ordinary dust does to tank treads. And I'll bet it will work for radar absorbing stealth coatings too, can even leave the carbon in. Ya know, I'll bet it would even increase octane in gasoline. Why run the exhaust thru a catalytic convertier when you can just mix the catalyst in the gasoline. And diesel. Whoa! The soot would probably coalesce right around the iron dust. Then just use a magnet to clean up the exhaust. Endless possibilities!! Don
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Ohms Law V = I R |
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#14 | |
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diyAudio Member
Join Date: Jun 2003
Location: Dallas,TX
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Quote:
John |
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#15 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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I use a variac to vary the voltage on a winding on the xfmr. The current waveform is monitored by current probe on an oscilloscope. (DC to 50 Mhz response TEK A6302 probe) As the voltage is increased, M6 develops a square wave current initially which then develops a spike at the END of the square wave as one nears the rated voltage. The spike rapidly grows in magnitude near and above the rated voltage. The square wave is most likely due to the square hysteresis curve of square orthonol material.
With non-oriented iron, the current starts out as a triangular waveform and develops a spike in the center at the triangle peak. Similarly, the spike grows rapidly around the rated voltage and above. Toroids with M6 have an especially clean square wave initially, and would be expected to do so since 100% of the material is currectly oriented to the field. This was all learned by testing known transformer materials, and has been very consistent. Probably, something like round permalloy would give a different waveform. I haven't tested anything like M4 or other rarer materials, so this test may not identify them uniquely from grain oriented M6. But for audio, any grain oriented material is likely to be suitable unless it is cross grain oriented at 90 degrees to the field. (Some HF materials are this way.) Another test one could do would be to measure inductance at just below the point of the spike forming current level and calculate material Mu from physical dimensions and turns (a fair amount of work however). The M6 will have a significantly higher Mu than the non grain oriented material. Don
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Ohms Law V = I R |
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#16 |
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diyAudio Member
Join Date: Dec 2001
Location: Hickory, NC
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A few more observations on xfmr current waveform measurements.
At very low voltage, WELL below rated voltage, the current waveform is usually a sine wave (of course this depends on how good the power line sine wave is in your area, it has deteriorated significantly to a flat top here over the years, computers,electronics....) for either oriented or non-oriented material. The initial current spike for an M6 toroid is very narrow at the end of the square wave current. For M6, E lams its broader. The long E lams are in-between. The narrowness of this spike is a good measure of what percentage of the lam is correctly oriented with the field. (the back side of E lams between the fingers are incorrectly oriented) The voltage at which the spike appears is a good indication of weather the xfmr winding has enough turns or iron for the rated voltage. Cheap (skimped on the iron), and also old transformers (110V, 115V) , tend to have the saturation spike set in early. They operate at higher flux level then and suffer higher losses (get hotter, hum and buzz more too). Thick laminations in a xfmr are most likely to be non-oriented iron. Don
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