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#351 |
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diyAudio Member
Join Date: May 2009
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OK. Thanks for the advice.
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#352 | |
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diyAudio Member
Join Date: Jul 2008
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Quote:
My "mistake" was that I placed it too close to a relay (4mm) and now the relay gets warm unnecessarily. |
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#353 |
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diyAudio Member
Join Date: May 2009
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I've been doing a little testing this evening. Interestingly, it was more of an experiment to support some statements I had made elsewhere on a forum I frequent.
I'd be really grateful if someone could take a look at the thread and reassure me that my argument is sound. If it isn't I need to make my apologies and eat some humble pie! The debate is in my build thread here. Skip to the middle of page 6 where I describe the working of the power supply module. The debate builds from that point and covers theory, first principals and practical experimentation to attempt to arrive at the truth. However, my arguments do not sit well with a electronics man of 30 years experience. If I'm talking crap, tell me. |
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#354 |
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diyAudio Member
Join Date: Jul 2008
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First, your explanation is incorrect (but I sped-read it). You achieve the negative -35 Volt DC rail line, not by using the negative cycles of the
wave, but rather by using a separate winding, another 25 V AC secondary which in conjuction with the first secondary gives you a 50 V AC - or expressed in peak-to peak as it should be, +/- 70 V or 140 Volts peak to peak. By rectifying this voltage you then get +/- 70 V DC (excluding losses) and having a centre tap (the two leads of the windings together) you achieve a 0 point. The AC voltage is a sinusoidal and it reaches a peak, positive and negative. It can also be described as "voltage peak to peak" which is much easier to read off the oscilloscope. Eg your 25 V AC secondary is a +/- 35 V shape and you say "this a 70 V peak to peak". I prefer peak to peak because it saves making conversions all the time when I read things off the scope. My signal tone generator also displays peak to peak, not RMS. RMS is about energy - the area under the curve. Use RMS when you want to do power calculations for components. A square wave's RMS would be its peak as the area under the curve has no gaps, a triangular shape would be half the peak, because the area of a trinagle is half of its enclosing rectangle, and the area under the sinusoidal is 0.7 times the area of the square (it has been decades now, but I bet the integral of the sinusoidal function must be a/sqrt(2)). When you FULLY rectify an AC you convert the negatives to positives, you flip whatever is under 0 to the top. You have posted a picture that shows that process in your other thread. The peak is the same on the positive side, it has not changed, but now you are getting twice as many peaks on the positive as you did before, and nothing at all on the negative. This new shape is not AC: it is a heavily modulated DC. The energy it carries is still the same (the RMS value). You then feed that voltage into the filter capacitors, which charge to the peak and then discharge into the load. If there was no load, then one cycle would be enough to charge the caps to the peak value. You would then measure 35 volts even after disconnecting power. 35 volts is the peak reached. When there is a load however the capacitors discharge into that load, so they reach the 35 volts momentarily and then fall gently as the load is eating up their charge, until the next cycle where they would charge pretty rapidly. That seen on the scope is a sawtooth pattern, I have posted a picture hereabouts of what it looks like. The peak-to-peak extend of that ripple depends on the current being drawn and the size of the capacitors. Unless you have really smoothed down and eliminated that ripple, you cannot really call that "DC" neighter can you give it a value, it is all approximate. The above explanation ommits various effects, eg the voltage drop across the bridge rectifier and the energy spent on it. Another way to think about this is that "25 V AC RMS" does not really exist, it is a shorthand notation to describe "70 volts peak to peak in a 50Hz sinusoidal shape". |
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#355 |
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diyAudio Member
Join Date: Jun 2008
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the dc voltage value after the rectifier is the Peak AC voltage value
so if you're starting with 25V ac rms the peak will be something like 25VACrms x (root2) = 35VDC so peak to peak will be x2 = 70 Last edited by Ted205; 7th September 2009 at 10:48 AM. |
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#356 |
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diyAudio Member
Join Date: Jul 2008
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With a 25V AC secondary I got 77 Watts RMS into 7.5 Ohm before clipping. It does get hot and I have added a fan (one fan to 3 chips).
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#357 | |
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just another
diyAudio Moderator
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Quote:
Wintermute's Gainclone also here is a link to your upgrade island post Tony. |
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#358 |
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diyAudio Member
Join Date: Aug 2008
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I think you are mistaken about doubling the voltage for + and -. That comes from using two secondaries and two rectifiers. DC voltage is approximately AC peak voltage for a bridge rectifier, which is RMS * sqrt(2) = RMS * 1.41. Minus 1.4V for diode drop of course.
__________________
Tyler |
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#359 |
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diyAudio Member
Join Date: May 2009
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Thanks guys. Some interesting replies. I not sure I meantioned doubling of the voltage for + / - but two of you highlight it....so that impression must have come from somewhere.
Anyway, I feel a lot more confident that my statements are indeed correct. |
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#360 |
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diyAudio Member
Join Date: May 2009
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A few pictures from my other thread showing some preliminary testing...
![]() The basic rig. ![]() Checking voltage from the power inlet ![]() Checking voltage from the transformer ![]() Checking voltage from the power supply board I did the use the light bulb tester. But nothing happened i.e. I didn't see it light up. I am assuming that this is good. |
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