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#1
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Two frequencies, 50Hz and 60Hz.
Two rectification schemes, half wave and full wave. I need to explain in simple terms how to pick capacitor values for these 4 types of circuits. Any thoughts or rules of thumb? This is where I am at on the AAC power supply article.
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.. "Good enough is enemy of the best." An old engineering saying, Author unknown. General info: If you have a question, please start a thread/topic. I do not provide gratis assistance via PM nor E-mail, as that would violate the intent of this Board, which is sharing knowledge ... and deprives you of other knowledgeable input. Thanks for the verbage Wookie. |
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#2
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Hello Bill,
Perhaps the attached PDF will help a bit. I had the remark once that the calculations where not all correct. unfortunately I can not remember wich one it was. Greetings, Bertus
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You don't have to know everything, if you know where to find it. When you do ask questions, you may look stupid. When you do NOT ask questions, you will STAY stupid. It would be nice to have the Timezone ( GMT +/- x ) in the location field in the profile. (User CP -> Edit Your Details) |
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#3
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Thanks, I still have some info Studiot left me a long while back. I need to condense them down into one or two paragraphs, plus math.
__________________
.. "Good enough is enemy of the best." An old engineering saying, Author unknown. General info: If you have a question, please start a thread/topic. I do not provide gratis assistance via PM nor E-mail, as that would violate the intent of this Board, which is sharing knowledge ... and deprives you of other knowledgeable input. Thanks for the verbage Wookie. |
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#4
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I did this for someone a few days ago as it happens..
Reference: A 1 Farad capacitance with a discharge current of one amp discharges at 1V per second. For a rough rule of thumb, divide 1 Farad by the ripple frequency and you will get a capacitor value that gives about 1V ripple per amp of load; eg. 10,000uF at 100Hz.
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Robert Jenkins. |
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#5
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To my dying day, I will remember "Civil Engineers are Queer" (strange!) i.e. C*ΔV = q (Coulombs)
Now i*t = q, so by substitution: i*t = C*ΔV. Rearrange gives: C = i*t/ΔV. So if you want a capacitor to deliver 0.75A for 0.0083ms (full-wave rectified 60Hz), say at the input of a LM317, and ΔV must be smaller than 5V to keep the filter minimum voltage from sagging below Vout + VdropOut, then C = 0.75*0.0083/5 = 0.001245F = 1245uF
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Mike ML |
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#6
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For full wave rectification, I use the following formula. It is a good rule of thumb:
C = Imax / (2 x Freq x Vripple) Or you can use this one: C = Imax / (2 x Freq x Vpeak * ripple_factor) being ripple factor a value from 0 to 1. Note that the formula is an approximation, and works better for ripple factors inferior to 0.1 (or for small Vripples when relative to Vpeak). For the expected DC voltage, check out this guide: Rectifier guidelines.pdf This guide is more precise for AC currents on transformers, though: power_xfrmr_Design_guide.pdf
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I love the smell of toasted transistors in the morning. Last edited by cumesoftware; 02-07-2010 at 11:46 PM. |
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#7
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There's a strange misconception on page 12-36. Apparently the author thinks that "If the charge time becomes too great, then the capacitor may never reach full charge from the incoming pulses from the rectifier". This is not true, of course.
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#8
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Quote:
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#9
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for a capacitor to instantaneously change voltage you would need infinite power.
In such circuits there is nothing restricting current flow so you can have infinite power to change the voltage to the peak as soon as the diode conducts. Obviously any small resistance, i.e from the wire from the rectifier to the capacitor would prevent this from occuring in the real world... |
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#10
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Look at the picture on page 12-35. It shows what happens as the capacitance increases. Now imagine that the filter cap was 1,000,000 microfarads instead of just 1000 microfarads. The slightly downward angle of the blue line would become a nearly horizontal line for 1,000,000 microfarads. It might take a while to reach steaedy state, but once it did, the pulse from the rectifier would keep the cap voltage very near the peak of the sine wave because with a cap of 1,000,000 microfarads the load would discharge it so little that the next rectifier pulse would easily replenish it.
As long as the transformer winding resistance plus the rectifier bulk resistance is substantially less than the load resistance, the DC voltage across the cap will be approximately equal to the sine peak voltage, no matter how large the capacitance. |
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