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#1 |
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diyAudio Member
Join Date: Jul 2005
Location: CT
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Is there any reason to not use a low duty-cycle design? Would 9% be too little? What ramifications, if any, does this have?
regards gene |
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#2 |
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diyAudio Member
Join Date: Jun 2004
Location: Warsaw
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For the same voltage and power, this will cause 5 times more peak current stress compared to 45%.
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#3 |
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diyAudio Member
Join Date: Jul 2005
Location: CT
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Yes, I see what you mean. In simulation, on SEPIC topology, Vin = 50V, Vo=3.3V, Iout = 2.0A, duty cycle is around 6%. The ripple current current in the inductors is quite high. So I dropped the Vin to 10V and the ripple current dropped as well. Although the average in both cases is the same - as I expected it should be.
I think I will have to change topology to flyback so that the duty cycle can get higher - maybe 50%, seems reasonable. |
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#4 | |
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diyAudio Member
Join Date: Oct 2005
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Quote:
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#5 | |
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diyAudio Member
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Quote:
__________________
I use to feel like the small child in The Emperor's New Clothes tale
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#6 |
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diyAudio Member
Join Date: Jul 2005
Location: CT
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Eva,
Can you tell me if using toroid in flyback supply is ok? I read somewhere (that I can't recall) that it is ok since there are distributed gaps in the core material. But, as I read more, most of the literature points to using a precise gap in the core, by design. How would that play out when using the toroid, where the exact dimensions of the gap are unknown? thanks |
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#7 |
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diyAudio Member
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A single gap in the inner leg of the core is the worst situation because it results in higher copper losses due to proximity effect. The "finging flux" leaking from the gap induces eddy currents in nearby magnet wires. The only advantage is that the windings effectively shield the gap resulting in reduced leakage flux.
Gaps in the outer legs result in lower copper losses at the expense of high leakage flux. Iron powder cores don't suffer from increased copper losses due to fringing flux but they tend to produce more leakage flux, particularly when the windings don't cover the entire core (as in iron powder E cores). Toroids suffer from poor coupling between windings in comparison with E cores with interleaved windings. This is a big problem in flyback topologies because more energy has to be clamped in the primary side (a two-switch flyback may solve this, though). Good line isolation is also quite hard to achieve with toroids and usually results in even worse coupling. Now choose yourself
__________________
I use to feel like the small child in The Emperor's New Clothes tale
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#8 | |
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diyAudio Member
Join Date: Sep 2006
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Quote:
Old style potcores may well offer the best of both options: unlike the present construction, made of two symetrical cups, they were composed of three parts: -A disk with a center pillar -An outer ring -An end disk If the gap is implemented at the top of the pillar, it will still be enclosed and shielded, but it will largely be offset from the main part of the winding, especially so because of the presence of the coil former's flange. Might be time to revive this design with modern materials. |
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#9 |
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diyAudio Member
Join Date: Jun 2002
Location: Melbourne, Australia
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When you think about it, a potcore is an inside-out version of a toroid. The winding and the core are in opposite places. The dual of a toroid perhaps?
__________________
Best-ever T/S parameter spreadsheet. http://www.diyaudio.com/forums/multi...tml#post353269 |
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#10 |
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diyAudio Member
Join Date: Jan 2003
Location: Solna
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"If the gap is implemented at the top of the pillar, it will still be enclosed and shielded, but it will largely be offset from the main part of the winding, especially so because of the presence of the coil former's flange.
Might be time to revive this design with modern materials." IIRC I did a FEM simulation of something similar and the results were even worse as there will be more layers of winding causing increased proximity effect. Spacing the winding away from the gap works well though. You can curve it too and it will be even better. That is, winding is furthest from center leg at the center of the bobbin curving inwards at the ends of the bobbin. |
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